Wave Behaviour

サイト: Young Education
コース: Waves
ブック: Wave Behaviour
印刷者: Guest user
日付: 2026年 11月 9日(月曜日) 16:40

1. Superposition

Learning outcomes
  • I can explain the principle of superposition.
  • I can predict the combined displacement of overlapping waves.
  • I can distinguish between constructive and destructive interference.
  • I can sketch simple superposition diagrams.
  • I can explain why waves continue unchanged after passing through one another.

Superposition

When two or more waves meet in the same region, they can temporarily overlap. While they overlap, their individual displacements combine to produce a resultant displacement.

This behaviour is described by the principle of superposition.

Superposition explains many important wave phenomena, including:

  • constructive interference
  • destructive interference
  • interference patterns
  • standing waves
  • sound interference
  • noise-cancelling technology

An important feature of superposition is that the waves do not normally destroy or permanently change one another. After overlapping, each wave continues travelling with its original shape and direction, provided the medium behaves linearly.

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The Principle of Superposition

The principle of superposition states that when two or more waves overlap, the resultant displacement at any point is the sum of the individual displacements of the waves at that point.

In simple form:

resultant displacement = displacement₁ + displacement₂ + ...

For two waves:

y_resultant = y₁ + y₂

Displacement must include direction.

A displacement above the equilibrium position can be treated as positive, while a displacement below equilibrium can be treated as negative.


Displacement

Displacement describes how far and in which direction a point in a medium has moved from its equilibrium position.

For a transverse wave:

  • above equilibrium → positive displacement
  • below equilibrium → negative displacement
  • on equilibrium → zero displacement

For example:

Wave A displacement = +3 cm

Wave B displacement = +2 cm

Then:

resultant = +3 + (+2)

resultant = +5 cm


Adding Positive and Negative Displacements

Suppose:

Wave A = +4 cm

Wave B = −3 cm

Then:

resultant = +4 + (−3)

resultant = +1 cm

The point is therefore 1 cm above its equilibrium position.

Superposition is essentially an algebraic addition of displacements.


Superposition Happens Only During Overlap

Imagine two pulses travelling toward each other along a rope.

Before they meet, each pulse travels independently.

During overlap, their displacements combine.

After they pass through each other, the original pulses continue travelling.

The sequence is:

approach → overlap → separate

The combined shape exists only while the waves overlap.

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Constructive Interference

Constructive interference occurs when overlapping waves have displacements in the same direction.

Their displacements add together.

For example:

Wave A = +3 cm

Wave B = +2 cm

Resultant:

+3 + +2 = +5 cm

The resulting displacement is larger than either individual displacement.


Complete Constructive Interference

Suppose two identical upward pulses each have an amplitude of:

2 cm

When they overlap perfectly:

resultant displacement = 2 + 2

= 4 cm

For that instant, the resultant pulse has twice the amplitude of either original pulse.

After the overlap, each 2 cm pulse continues travelling.

The waves have not permanently combined into a 4 cm wave.


Constructive Interference Below Equilibrium

Constructive interference does not necessarily mean the displacement must be upward.

Suppose:

Wave A = −2 cm

Wave B = −3 cm

Then:

resultant = −2 + (−3)

= −5 cm

Both displacements are downward, so they reinforce one another.

The magnitude of the resultant displacement is:

5 cm

This is also constructive interference.


Destructive Interference

Destructive interference occurs when overlapping waves have displacements in opposite directions.

One displacement is positive while the other is negative.

For example:

Wave A = +5 cm

Wave B = −2 cm

Resultant:

+5 + (−2)

= +3 cm

The waves partially cancel.

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Complete Destructive Interference

Complete destructive interference occurs when two equal but opposite displacements overlap.

Suppose:

Wave A = +4 cm

Wave B = −4 cm

Then:

resultant = +4 + (−4)

= 0 cm

At that instant, the medium may appear completely undisturbed at the overlapping location.

However, the waves have not disappeared permanently.

They continue through one another and reappear as they separate.


Partial Destructive Interference

Destructive interference does not always produce zero displacement.

Suppose:

Wave A = +6 cm

Wave B = −4 cm

Then:

resultant = +6 − 4

= +2 cm

The waves partially cancel.

Because the upward displacement is larger, the resultant displacement remains upward.


Constructive vs Destructive Interference

Constructive Interference Destructive Interference
Displacements reinforce Displacements oppose
Same-direction displacements Opposite-direction displacements
Resultant magnitude can increase Resultant magnitude decreases
+3 + +2 = +5 +3 + −2 = +1
−3 + −2 = −5 +3 + −3 = 0

The key is to add the displacements with their signs.


Interference

Interference is the result of waves overlapping and combining through superposition.

Interference may be:

  • constructive
  • destructive
  • partially constructive
  • partially destructive

The exact result depends on the displacement contributed by each wave at each position.


Superposition Point by Point

When entire wave shapes overlap, you must add their displacements point by point.

Suppose two waves overlap.

At one position:

Wave A = +2 cm
Wave B = +3 cm

Resultant:

+5 cm

At another position:

Wave A = +1 cm
Wave B = −1 cm

Resultant:

0 cm

At another position:

Wave A = −2 cm
Wave B = −1 cm

Resultant:

−3 cm

The final waveform is constructed by repeating this process across the entire overlapping region.


A Superposition Table

A table can help when constructing a resultant wave.

Position Wave A Wave B Resultant
A 0 cm 0 cm 0 cm
B +1 cm +2 cm +3 cm
C +3 cm −1 cm +2 cm
D +2 cm −2 cm 0 cm
E −1 cm −2 cm −3 cm
F 0 cm 0 cm 0 cm

For every position:

resultant = Wave A + Wave B


Sketching a Superposition Diagram

To sketch the resultant of two overlapping waves:

  1. Draw the equilibrium line.
  2. Identify corresponding positions on both waves.
  3. Determine the displacement of Wave A at each position.
  4. Determine the displacement of Wave B at the same position.
  5. Add the two displacements algebraically.
  6. Plot the resultant displacement.
  7. Repeat across the entire overlap.
  8. Connect the points smoothly if the waves are continuous.

Do not simply add the amplitudes unless the corresponding peaks or troughs are actually overlapping.


Example: Two Upward Pulses

Suppose two upward pulses approach each other.

Pulse A has amplitude:

+3 cm

Pulse B has amplitude:

+2 cm

When their peaks overlap perfectly:

resultant = +3 + +2

= +5 cm

At that instant, the resultant pulse reaches 5 cm above equilibrium.

This is:

constructive interference

Afterward, the pulses separate and continue travelling.


Example: Upward and Downward Pulses

Suppose:

Pulse A = +4 cm

Pulse B = −3 cm

When their largest displacements overlap:

resultant = +4 + (−3)

= +1 cm

The resultant is 1 cm upward.

This is:

partial destructive interference


Example: Complete Cancellation

Two pulses have equal amplitudes but opposite directions:

Pulse A = +5 cm

Pulse B = −5 cm

During complete overlap:

resultant = +5 + (−5)

= 0 cm

The rope may temporarily appear flat.

Moments later, the two pulses emerge and continue travelling.

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Why Waves Pass Through One Another

In many ordinary wave systems, each wave causes its own displacement independently.

During overlap, these displacements add.

Once the waves no longer overlap, each continues to propagate according to the properties of the medium.

Therefore, superposition is temporary.

The waves do not normally:

  • bounce off one another
  • permanently merge
  • permanently cancel
  • exchange identities

Instead, they pass through one another.


Waves Are Not Solid Objects

It can be tempting to imagine two pulses as objects colliding.

But waves are disturbances, not solid objects.

When two balls collide, they can exert forces on each other and change their motion.

When two ordinary small-amplitude waves overlap in a linear medium, the medium simply responds to the combined displacement.

Afterward, each disturbance continues.

This is why two sound waves, for example, can travel through the same region simultaneously.


Superposition and Energy

Complete destructive interference does not mean that the wave energy has simply vanished.

During interference, energy can be redistributed within the wave system.

In sustained interference patterns, some regions may have greater wave intensity while others have less.

Therefore:

zero displacement at one point does not necessarily mean zero energy everywhere.

The original waves can continue after the interference occurs.


Superposition of Continuous Waves

Superposition applies not only to individual pulses but also to continuous waves.

When continuous waves overlap, their displacements continually add.

Depending on their relative positions or phase, they may produce:

  • constructive interference
  • destructive interference
  • alternating combinations

This can create stable interference patterns under suitable conditions.


Waves in Phase

Two waves are in phase when corresponding points in their cycles line up.

For example:

  • crest aligns with crest
  • trough aligns with trough

If two waves of the same frequency are in phase, they produce strong constructive interference.

For identical waves:

crest + crest → larger crest

trough + trough → deeper trough


Waves Out of Phase

Two waves can be out of phase.

If a crest from one wave aligns with a trough of another, destructive interference occurs.

For identical waves exactly half a cycle apart:

crest + equal trough → zero displacement

This corresponds to complete destructive interference.


Phase Difference

Phase difference describes how far apart two waves are in their cycles.

For two identical sinusoidal waves:

0° phase difference → maximum constructive interference

180° phase difference → maximum destructive interference

Intermediate phase differences produce partial interference.


Path Difference

Interference can also depend on the difference in the distances travelled by two waves.

This is called the:

path difference

For waves of wavelength λ, constructive interference commonly occurs when the path difference is:

0, λ, 2λ, 3λ, ...

Destructive interference commonly occurs when the path difference is:

λ/2, 3λ/2, 5λ/2, ...

These relationships are particularly useful when studying interference patterns.


Sound-Wave Interference

Sound waves obey the principle of superposition.

Suppose two sound waves reach the same location.

The pressure variations produced by the waves combine.

If they reinforce:

constructive interference

can produce greater sound intensity.

If they oppose:

destructive interference

can reduce the sound intensity.

This principle has important technological applications.


Noise-Cancelling Headphones

Active noise-cancelling headphones use destructive interference.

A simplified process is:

  1. A microphone detects surrounding sound.
  2. Electronics analyze the sound.
  3. The headphones produce another sound wave.
  4. This wave is designed to oppose the unwanted sound.
  5. The two pressure disturbances superpose.
  6. Destructive interference reduces the unwanted sound at the listener's ear.
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This works especially well for relatively steady, low-frequency background noise such as:

  • aircraft engine noise
  • vehicle noise
  • ventilation systems

Real noise cancellation is more complex than simply producing one perfectly inverted wave everywhere.


Interference of Water Waves

Water waves can also superpose.

If two sets of water waves overlap:

  • crest + crest → constructive interference
  • trough + trough → constructive interference
  • crest + trough → destructive interference

A ripple tank can be used to observe these patterns.

Regions of strong and weak wave motion can appear across the water surface.


Interference of Light

Light waves also obey the principle of superposition.

When coherent light waves overlap, they can produce:

  • bright regions from constructive interference
  • dark regions from destructive interference

Interference experiments provide strong evidence for the wave behaviour of light.

Applications include:

  • interferometers
  • precision measurement
  • optical coatings
  • spectroscopy
  • holography

Thin-Film Colours

The colours seen in:

  • soap bubbles
  • thin oil films
  • some coated lenses

can involve interference.

Light reflects from different surfaces of the thin layer.

The reflected waves travel slightly different distances.

When they recombine, some wavelengths interfere constructively while others interfere destructively.

This can produce changing colours.

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Standing Waves

Superposition is also responsible for standing waves.

A standing wave can form when two waves of the same frequency and similar amplitude travel in opposite directions.

Their continuous superposition produces locations called:

  • nodes
  • antinodes

At a node, displacement remains zero.

At an antinode, the oscillation has maximum amplitude.

Standing waves are important in:

  • strings
  • musical instruments
  • air columns
  • resonant systems

Superposition of More Than Two Waves

The principle is not limited to two waves.

Suppose three waves overlap at one point:

Wave A = +2 cm

Wave B = −4 cm

Wave C = +3 cm

Then:

resultant = +2 − 4 + 3

resultant = +1 cm

The same principle works for any number of overlapping waves:

add all individual displacements.


Worked Example: Three Waves

At one instant, three waves produce these displacements at the same point:

Wave A = +5 mm

Wave B = −2 mm

Wave C = −1 mm

Resultant:

+5 + (−2) + (−1)

= 5 − 2 − 1

= +2 mm

The resultant displacement is:

2 mm above equilibrium


Worked Example: Predicting Interference

Two identical sinusoidal waves have amplitudes of:

4 cm

Their crests arrive at the same point at the same time.

At that instant:

resultant = +4 + +4

= +8 cm

This is maximum constructive interference.

Later, suppose a crest from one wave overlaps an equal trough from the other:

resultant = +4 + (−4)

= 0 cm

This is complete destructive interference.


Reading Superposition Diagrams

When interpreting a superposition diagram, do not focus only on the peaks.

Look at each horizontal position.

Ask:

What is Wave A's displacement here?

What is Wave B's displacement here?

Then calculate:

A + B

Repeat across the diagram.

This produces the complete resultant waveform.


Predicting the Sign of the Resultant

A useful shortcut is to compare the displacements.

If both are positive:

resultant is positive and larger in magnitude

If both are negative:

resultant is negative and larger in magnitude

If one is positive and one negative:

subtract their magnitudes

The larger displacement determines the direction of the resultant.

If they are equal and opposite:

resultant = 0


After the Waves Overlap

Consider two pulses:

Pulse A travels right.

Pulse B travels left.

During overlap, a resultant waveform appears.

After overlap:

  • Pulse A continues right
  • Pulse B continues left
  • each returns to its original form in an ideal linear medium

The waves have passed through one another.

This is one of the most important ideas in superposition.


Temporary Cancellation Does Not Destroy the Waves

Suppose two identical opposite pulses overlap perfectly.

For an instant:

resultant displacement = 0

It may look as though both waves have disappeared.

They have not.

A moment later, they separate and become visible again.

The cancellation applied to the resultant displacement during overlap, not to the permanent existence of the two waves.


Limits of the Simple Superposition Model

The simple principle of superposition works extremely well when the system behaves linearly.

This is a good approximation for many:

  • small waves on strings
  • sound waves
  • water-wave experiments
  • electromagnetic waves

For very large disturbances or strongly nonlinear materials, waves can interact in more complicated ways.

At the level of most introductory wave problems, however, we assume:

waves pass through one another unchanged after superposition.


A Complete Pulse Example

Two pulses move toward each other.

Pulse A has a maximum displacement of:

+6 cm

Pulse B has a maximum displacement of:

−4 cm

Before overlap, each pulse has its own shape.

At complete overlap:

resultant maximum displacement = +6 + (−4)

= +2 cm

This is partial destructive interference.

After overlap:

  • the +6 cm pulse continues in its original direction
  • the −4 cm pulse continues in its original direction
  • each has its original shape and amplitude

The +2 cm pulse exists only as the temporary resultant during overlap.


A Reliable Strategy for Superposition Problems

When two or more waves overlap:

  1. Draw or identify the equilibrium line.
  2. Choose a position on the waves.
  3. Determine each wave's displacement at that position.
  4. Assign positive and negative signs correctly.
  5. Add the displacements algebraically.
  6. Plot the resultant displacement.
  7. Repeat at several positions.
  8. Connect the resultant points smoothly when appropriate.
  9. Identify whether the interference is constructive or destructive.
  10. Remember that the resultant exists only while the waves overlap.
  11. After overlap, draw the original waves continuing in their original directions.
  12. Check that no wave has mysteriously disappeared or changed permanently.

Common Mistakes

Adding amplitudes instead of displacements

Superposition requires the displacement at each position to be added, including its direction.

Ignoring negative displacement

A trough or downward pulse should normally be represented with a negative displacement.

Thinking constructive interference always points upward

Two downward displacements can also reinforce each other.

Thinking destructive interference always gives zero

Only equal and opposite displacements cancel completely.

Thinking zero displacement means the waves have disappeared

The waves can still be present and continue after overlap.

Thinking waves bounce off each other

In the simple linear model, waves pass through one another.

Thinking the larger resultant pulse is permanent

It exists only while the appropriate waves overlap.

Adding only the peaks

The entire resultant waveform must be found by adding displacements point by point.

Confusing interference with reflection

Interference occurs when waves overlap.

Reflection occurs when a wave encounters a boundary and returns.

Thinking destructive interference destroys energy

Interference redistributes wave effects; cancellation of displacement at a point does not mean all wave energy has vanished.


Key Terms

Superposition — principle stating that overlapping wave displacements add to produce a resultant displacement.

Displacement — distance and direction of a point from its equilibrium position.

Equilibrium position — undisturbed or central position of a vibrating medium.

Resultant displacement — combined displacement produced by all waves at a particular point.

Interference — effect produced when waves overlap and superpose.

Constructive interference — interference in which wave displacements reinforce one another.

Destructive interference — interference in which wave displacements oppose one another.

Complete constructive interference — maximum reinforcement when appropriate matching wave displacements overlap.

Complete destructive interference — cancellation to zero resultant displacement when equal and opposite displacements overlap.

Partial destructive interference — incomplete cancellation caused by opposite displacements of unequal magnitude.

Phase — position of a wave within its cycle.

In phase — waves whose corresponding points in their cycles align.

Out of phase — waves whose corresponding points do not align.

Phase difference — difference between the positions of two waves within their cycles.

Path difference — difference between the distances travelled by two waves before reaching a location.

Pulse — single disturbance travelling through a medium.

Resultant wave — temporary combined waveform produced by superposition.

Node — location in a standing wave where displacement remains zero.

Antinode — location in a standing wave where oscillation amplitude is greatest.

Standing wave — wave pattern produced by superposition of suitable waves travelling in opposite directions.

Linear medium — medium in which individual wave effects can be added using the principle of superposition.


Key Takeaways

  • Superposition occurs when two or more waves overlap.
  • The resultant displacement is the algebraic sum of the individual displacements.
  • Positive and negative directions must be included when adding displacements.
  • Superposition must be applied point by point across overlapping waves.
  • Constructive interference occurs when displacements reinforce each other.
  • Constructive interference can occur above or below equilibrium.
  • Destructive interference occurs when displacements oppose each other.
  • Complete destructive interference requires equal and opposite displacements.
  • Partial destructive interference occurs when opposite displacements have different magnitudes.
  • A zero resultant displacement does not mean that the original waves have permanently disappeared.
  • In an ideal linear medium, waves continue unchanged after passing through one another.
  • The resultant waveform exists only while the original waves overlap.
  • Waves should not be treated like solid objects colliding with one another.
  • Continuous waves can also undergo constructive and destructive interference.
  • Waves that are in phase tend to reinforce each other.
  • Waves 180° out of phase can produce complete destructive interference when their amplitudes are equal.
  • Path difference can determine whether interference is constructive or destructive.
  • Sound, water waves, and light can all demonstrate interference.
  • Active noise cancellation uses destructive interference.
  • Thin-film colours can result from interference of light.
  • Standing waves are produced through superposition of waves travelling in opposite directions.
  • Superposition can involve more than two waves.
  • The principle of superposition is fundamental to understanding how multiple waves can occupy the same region at the same time.

Check Your Understanding

  1. State the principle of superposition in your own words.
  2. Two waves produce displacements of +3 cm and +5 cm at the same point. Calculate the resultant displacement and identify the type of interference.
  3. Two waves produce displacements of −2 cm and −4 cm. Calculate the resultant displacement. Is this constructive or destructive interference?
  4. At one point, Wave A has a displacement of +7 cm and Wave B has a displacement of −3 cm. Calculate the resultant displacement.
  5. Two waves each have amplitudes of 6 cm. One produces a displacement of +6 cm while the other produces −6 cm at the same point. What is the resultant displacement, and what type of interference occurs?
  6. Explain the difference between constructive and destructive interference.
  7. Explain why destructive interference does not always result in zero displacement.
  8. Describe how you would construct a resultant wave from two overlapping wave diagrams.
  9. Two pulses travelling in opposite directions overlap completely and temporarily produce a flat rope. Explain what happens to the pulses immediately afterward.
  10. Explain why waves can pass through one another rather than behaving like two solid objects in a collision.
  11. Three waves produce displacements of +4 mm, −7 mm, and +5 mm at the same point. Calculate the resultant displacement.
  12. Explain what is meant by waves being in phase and describe the interference expected when two identical waves are perfectly in phase.
  13. Explain how active noise-cancelling headphones use the principle of superposition.
  14. A student says, "When two waves undergo complete destructive interference, both waves are destroyed and their energy disappears." Explain why this statement is incorrect.
  15. Two identical pulses travel toward each other on a rope. One pulse points upward and the other downward. Sketch or describe the wave pattern before overlap, during complete overlap, and after overlap, and explain how the sequence demonstrates the principle of superposition.
 
 
 

2. Reflection and Refraction of Waves

Learning outcomes
  • I can describe reflection of waves at boundaries.
  • I can explain refraction due to changes in wave speed.
  • I can predict changes in wavelength during refraction.
  • I can compare reflection and refraction.
  • I can identify examples of both phenomena.

Reflection and Refraction of Waves

Waves can change their behaviour when they reach a boundary between two regions or materials.

Two important possibilities are:

  • reflection — the wave returns into the original region
  • refraction — the wave enters a new region, changes speed, and may change direction

These behaviours occur with many types of waves, including:

  • water waves
  • sound waves
  • seismic waves
  • light and other electromagnetic waves

Understanding reflection and refraction allows us to predict how waves behave when their surroundings change.

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6

Waves at Boundaries

A boundary is a place where the conditions through which a wave travels change.

Examples include:

  • the end of a rope
  • deep water meeting shallow water
  • air meeting glass
  • air meeting water
  • one rock layer meeting another
  • warm air meeting cooler air

When a wave reaches a boundary, its energy may be:

  • reflected
  • transmitted
  • refracted
  • absorbed

Often, more than one of these occurs at the same time.

For example, when light reaches a glass window, some light is reflected while some enters the glass.


Reflection of Waves

Reflection occurs when a wave encounters a boundary and some or all of the wave travels back into the original region.

The incoming wave is called the:

incident wave

The returning wave is called the:

reflected wave

Reflection does not require the wave to change into a different type of wave.

Instead, its direction of propagation changes.


Reflection of a Wave Pulse

Imagine sending a pulse along a rope toward a boundary.

The pulse travels toward the end of the rope.

When it reaches the boundary, a reflected pulse travels back along the rope.

The exact behaviour of the reflected pulse depends on the type of boundary.

https://images.openai.com/static-rsc-4/Q6Kztj3ZilnxXQKEv47F7gv3N6lhehB-mT_Mo1Uf4oPA9Wor4KohGle29WkOzvF12q5sjCrMH205Hm2jfiUxoKClMww73rfGx1utFaJlRHIQOPkYHDA_e0znnRhBKHwx92zmbnJVbSQecWWHJWKdE3tzj0in7y8m6OD9p-tQjA-ElDrZAfUyxF7xSI__suOP?purpose=fullsize
 

Reflection at a Fixed Boundary

A fixed boundary is a boundary that cannot move freely.

For example, a rope may be firmly attached to a wall.

When an upward pulse reaches the fixed end, it reflects as a downward pulse.

The reflected pulse is therefore:

inverted

So:

upward incident pulse → downward reflected pulse

The reflected pulse then travels back along the rope.


Reflection at a Free Boundary

A free boundary can move.

When a pulse reflects from an ideal free end, it is not inverted.

Therefore:

upward incident pulse → upward reflected pulse

The pulse still reverses its direction of travel, but its displacement orientation remains the same.


Fixed vs Free Boundary

Boundary Reflected Pulse
Fixed end Inverted
Free end Not inverted

This distinction is particularly useful when studying waves on strings and ropes.


Reflection of Continuous Waves

Continuous waves can also reflect.

Examples include:

  • water waves reflecting from a harbour wall
  • sound reflecting from a building
  • light reflecting from a mirror
  • seismic waves reflecting from boundaries inside Earth

The same basic principle applies:

wave energy returns from a boundary.


Reflection and the Normal

For waves approaching a flat boundary, angles are measured relative to an imaginary line called the:

normal

The normal is perpendicular to the boundary.

The angle of incidence is measured between the incident wave direction and the normal.

The angle of reflection is measured between the reflected wave direction and the normal.


The Law of Reflection

For reflection from a suitable flat boundary:

angle of incidence = angle of reflection

or:

θᵢ = θᵣ

For example, if a wave reaches a boundary at:

θᵢ = 35°

then:

θᵣ = 35°

The angles must be measured from the normal.

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4

Reflection of Water Waves

Water waves can reflect from barriers such as:

  • walls
  • rocks
  • harbour structures
  • shorelines

A ripple tank can be used to observe this behaviour.

Straight wavefronts approaching a straight barrier reflect according to the law of reflection.

This makes water waves useful for modelling many general wave behaviours.


Reflection of Sound

Sound waves can reflect from surfaces.

A reflected sound may be heard as an:

echo

Large, hard surfaces are often effective reflectors of sound.

Examples include:

  • cliffs
  • walls
  • buildings
  • tunnel surfaces

Reflection of sound is used in technologies such as:

  • sonar
  • ultrasound imaging
  • echo sounding

Echoes

Suppose a sound travels toward a wall, reflects, and returns to the observer.

The sound travels:

to the wall + back from the wall

Therefore:

distance to wall = speed × total time / 2

For example, if:

speed of sound = 340 m/s

echo time = 0.60 s

then:

distance = (340 × 0.60)/2

distance = 204/2

distance = 102 m


Reflection of Light

Light can reflect from surfaces such as:

  • mirrors
  • glass
  • water
  • polished metal

Mirrors are designed to produce strong, organized reflection.

The law of reflection applies:

θᵢ = θᵣ

Reflection allows mirrors and many other optical instruments to control the direction of light.


Refraction of Waves

Refraction occurs when a wave enters a region where its speed changes and, if it enters at an angle, its direction changes.

Refraction therefore involves:

change in wave speed

and often:

change in wave direction

Examples include:

  • water waves moving from deep to shallow water
  • light moving from air into glass
  • sound moving through air at different temperatures
  • seismic waves moving between layers inside Earth
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8

Why Waves Refract

Consider a straight wavefront approaching a boundary at an angle.

Suppose one side of the wavefront enters the new region first.

If the wave travels more slowly there, that side slows down while the rest of the wavefront continues at its original speed.

The wavefront rotates.

As a result, the direction of wave travel changes.

This is the basic mechanism of refraction.


Refraction Requires a Change in Wave Speed

A wave changes direction during refraction because its speed changes across the boundary.

If the speed does not change, there is no refraction due to the boundary.

Therefore, the key idea is:

change in wave speed → possible change in direction

The amount of bending depends on the difference in wave speeds and the angle at which the wave reaches the boundary.


Entering a Slower Region

When a wave enters a region where it travels more slowly at an angle, it bends:

toward the normal

Therefore:

faster → slower = toward the normal

For example, water waves moving from deeper water into sufficiently shallow water slow down.

If they enter the shallow region at an angle, their direction bends toward the normal.


Entering a Faster Region

When a wave enters a region where it travels faster at an angle, it bends:

away from the normal

Therefore:

slower → faster = away from the normal

For example, shallow-water waves moving into deeper water generally speed up and bend away from the normal.


A Useful Refraction Rule

Remember:

slower → toward the normal

faster → away from the normal

This applies when the wave crosses the boundary at an angle.


What Happens at 0°?

Suppose a wave travels directly along the normal.

It reaches the boundary at:

0° to the normal

Its speed may change.

Its wavelength may also change.

However, it does not bend sideways because the entire wavefront reaches the boundary simultaneously.

Therefore:

refraction can occur without a change in direction.

The wave can still experience a change in speed and wavelength.


Frequency During Refraction

When a wave crosses into a different region, its frequency remains constant.

The source determines the frequency.

Crossing the boundary does not suddenly change how frequently the source produces waves.

Therefore:

f₁ = f₂

The wave's speed and wavelength may change, but its frequency does not.


Wave Speed and Wavelength

The wave equation is:

v = fλ

where:

v = wave speed

f = frequency

λ = wavelength

During refraction:

frequency stays constant

Therefore, if speed changes:

wavelength must change


Entering a Slower Region

Suppose a wave enters a slower region.

Since:

v = fλ

and f remains constant:

v decreases → λ decreases

Therefore:

slower wave → shorter wavelength

The wavefronts become closer together.


Entering a Faster Region

If a wave enters a faster region:

v increases

while:

f remains constant

Therefore:

λ increases

So:

faster wave → longer wavelength

The wavefronts become farther apart.


Predicting Wavelength Changes

A useful summary is:

Change Speed Frequency Wavelength
Enters slower region Decreases Same Decreases
Enters faster region Increases Same Increases

This relationship is one of the most important ideas in wave refraction.


Worked Example: Slower Region

A water wave has:

f = 4 Hz

v = 2.0 m/s

Calculate its wavelength.

Use:

v = fλ

Rearrange:

λ = v/f

λ = 2.0/4

λ = 0.50 m

The wave enters shallower water where its speed decreases to:

1.2 m/s

The frequency remains:

4 Hz

New wavelength:

λ = 1.2/4

λ = 0.30 m

Therefore:

  • speed decreased
  • frequency stayed constant
  • wavelength decreased

Worked Example: Faster Region

A wave has:

f = 5 Hz

and travels at:

v = 3 m/s

Its wavelength is:

λ = v/f

λ = 3/5

λ = 0.60 m

The wave enters a region where its speed becomes:

5 m/s

Frequency remains:

5 Hz

New wavelength:

λ = 5/5

λ = 1.0 m

The wavelength increased because the wave speed increased.


Reading Wavefront Diagrams

A wavefront joins points on a wave that are at the same stage of their cycle.

For water waves, each line in a wavefront diagram may represent a crest.

The spacing between adjacent wavefronts represents:

wavelength

Therefore:

closer wavefronts → shorter wavelength

farther-apart wavefronts → longer wavelength

This makes wavefront diagrams particularly useful for studying refraction.


Direction of Travel and Wavefronts

The direction in which a wave travels is perpendicular to its wavefronts.

Therefore, if wavefronts rotate at a boundary, the direction of travel also changes.

When interpreting a diagram:

  1. identify the wavefronts
  2. identify their spacing
  3. draw or imagine a line perpendicular to them
  4. use that line to determine the direction of wave travel

Water Waves in Deep and Shallow Water

Water-wave speed depends on water depth.

In sufficiently shallow water, waves travel more slowly than they do in deeper water.

Therefore, when water waves travel:

deep → shallow

they generally:

  • slow down
  • keep the same frequency
  • decrease in wavelength
  • bend toward the normal if entering at an angle

When they travel:

shallow → deep

they generally:

  • speed up
  • keep the same frequency
  • increase in wavelength
  • bend away from the normal if entering at an angle
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7

Why Ocean Waves Turn Toward the Shore

Ocean waves often approach a coastline at an angle.

The part of the wavefront that reaches shallow water first slows down first.

The deeper-water part continues moving faster.

This rotates the wavefront.

As a result, waves tend to become more nearly parallel to the shoreline as they approach.

This is an important real-world example of:

wave refraction


Refraction of Light

Light also refracts when its speed changes.

For example, light travels more slowly in glass than in air.

When light enters glass from air at an angle:

  • speed decreases
  • wavelength decreases
  • frequency remains constant
  • ray bends toward the normal

When it returns from glass to air:

  • speed increases
  • wavelength increases
  • frequency remains constant
  • ray bends away from the normal

Refractive Index

For light, the speed change can be described using refractive index:

n = c/v

where:

n = refractive index

c = speed of light in vacuum

v = speed of light in the material

A higher refractive index corresponds to a lower speed of light in that material.

Therefore, refractive index helps predict how light will refract at a boundary.


Refraction of Sound

Sound can also refract.

The speed of sound depends on properties of the medium, including temperature.

If different layers of air have different temperatures, sound may travel at different speeds through them.

This can cause sound waves to bend.

This helps explain why sound can sometimes be heard unusually well over long distances under certain atmospheric conditions.


Refraction of Seismic Waves

Seismic waves travel through Earth's interior.

Their speeds change as they encounter regions with different physical properties.

As a result, seismic waves:

  • refract
  • reflect
  • change direction

Scientists analyze these changes to investigate Earth's internal structure.

This provides evidence about:

  • the mantle
  • outer core
  • inner core
  • boundaries between Earth's layers

Reflection and Refraction Can Occur Together

A wave reaching a boundary does not always either reflect or refract.

Both can occur simultaneously.

For example, when light strikes a glass window:

  • some light reflects from the surface
  • some enters the glass and refracts

Similarly, seismic waves reaching an internal Earth boundary may be partly reflected and partly transmitted and refracted.

Wave energy can therefore be divided at a boundary.


Comparing Reflection and Refraction

Reflection Refraction
Wave returns from boundary Wave enters another region
Direction changes Direction may change
Wave remains in original region Wave is transmitted into new region
Caused by interaction with boundary Associated with change in wave speed
θᵢ = θᵣ for regular reflection Bending depends on relative wave speeds
Frequency remains unchanged Frequency remains unchanged
Examples: mirrors, echoes Examples: lenses, shallow-water bending

The main distinction is:

reflection → wave returns

refraction → wave enters a new region and changes speed


Reflection vs Refraction in a Window

Imagine looking through a glass window at night.

You may see:

  • objects outside through the glass
  • a faint reflection of yourself

The light reaching the window has been divided.

Some light:

reflects

Some light:

enters the glass and refracts

This everyday example shows that reflection and refraction can occur at the same boundary.


Reflection vs Refraction of Water Waves

Suppose water waves reach a region of shallow water next to a barrier.

At the barrier:

reflection may send waves back.

At the deep-to-shallow boundary:

refraction may change their speed, wavelength, and direction.

The two phenomena involve different physical processes even though both can change the direction of a wave.


Reflection vs Refraction of Sound

Sound reflection can produce:

echoes

Sound refraction can produce:

bending through regions where sound speed differs

For example:

  • a cliff can reflect sound
  • atmospheric temperature differences can refract sound

This demonstrates that reflection and refraction are general wave behaviours rather than properties unique to light.


Reflection vs Refraction of Seismic Waves

When seismic waves encounter a boundary inside Earth:

some energy may:

reflect back

while some may:

enter the next layer and refract

By detecting these waves at different locations, scientists can infer properties of Earth's interior.


Sketching Reflection

To sketch reflection:

  1. Draw the boundary.
  2. Draw the normal perpendicular to the boundary.
  3. Draw the incident direction.
  4. Measure or estimate the angle of incidence from the normal.
  5. Draw the reflected direction on the other side of the normal.
  6. Make the angle of reflection equal to the angle of incidence.
  7. Add arrows showing direction of travel.

Remember:

θᵢ = θᵣ


Sketching Refraction

To sketch refraction:

  1. Draw the boundary.
  2. Draw the normal.
  3. Draw the incident wave direction.
  4. Determine whether the new region is faster or slower.
  5. If slower, bend the wave toward the normal.
  6. If faster, bend the wave away from the normal.
  7. Keep frequency unchanged.
  8. Change the wavelength appropriately.
  9. Add arrows showing direction of travel.

For wavefront diagrams, also change the spacing between wavefronts.


A Complete Refraction Example

Water waves travel from deep water into shallow water.

Before the boundary:

v = 2.4 m/s

f = 3 Hz

Calculate wavelength:

λ = v/f

λ = 2.4/3

λ = 0.80 m

In shallow water:

v = 1.5 m/s

Frequency remains:

3 Hz

New wavelength:

λ = 1.5/3

λ = 0.50 m

Therefore:

  • speed decreases from 2.4 m/s to 1.5 m/s
  • frequency remains 3 Hz
  • wavelength decreases from 0.80 m to 0.50 m
  • if the wave enters at an angle, it bends toward the normal

A Complete Boundary Example

A wave approaches a boundary.

Part of the wave returns to the original region.

Another part enters the new region and slows down.

The returning part demonstrates:

reflection

The transmitted part demonstrates:

refraction

Because the transmitted wave slows down:

its wavelength decreases

because frequency remains constant.

If it crosses at an angle:

it bends toward the normal

Several wave behaviours can therefore be observed at the same boundary.


Applications of Wave Reflection

Reflection is useful in many technologies.

Examples include:

Sonar

Reflected sound determines distance to underwater objects.

Medical ultrasound

Reflected ultrasound provides information about structures inside the body.

Mirrors

Reflected light forms images.

Radar

Reflected electromagnetic waves can locate objects and determine motion.

Seismology

Reflected seismic waves reveal underground structures.

Echo sounding

Reflected sound measures water depth.


Applications of Wave Refraction

Refraction also has many applications.

Examples include:

Lenses

Refraction focuses or spreads light.

Eyeglasses

Lenses redirect light to improve image formation in the eye.

Cameras

Lens systems refract light onto sensors.

Microscopes

Lenses use refraction to form magnified images.

Telescopes

Refracting telescopes use lenses to collect and focus light.

Seismology

Refraction helps scientists investigate Earth's internal structure.

Coastal engineering

Water-wave refraction helps predict how wave energy reaches shorelines.


Wave Behaviour Around Coastlines

Refraction can redistribute wave energy along a coastline.

As waves approach irregular shores:

  • wavefronts bend
  • energy may become concentrated around headlands
  • energy may become more spread out in bays

This can influence:

  • erosion
  • sediment transport
  • beach formation
  • harbour design

Wave refraction is therefore important in coastal science and engineering.


A Reliable Strategy for Boundary Problems

When a wave reaches a boundary:

  1. Identify the incident wave.
  2. Identify the boundary.
  3. Determine whether the wave reflects, enters the new region, or both.
  4. If it reflects, apply the reflection rule.
  5. If it enters another region, compare wave speeds.
  6. Determine whether the wave speeds up or slows down.
  7. Remember that frequency stays constant.
  8. Use v = fλ to predict the wavelength change.
  9. If the wave slows, wavelength decreases.
  10. If the wave speeds up, wavelength increases.
  11. If it enters at an angle, predict the direction of bending.
  12. Slower means toward the normal.
  13. Faster means away from the normal.
  14. Check that the final diagram is consistent with all of these predictions.

Common Mistakes

Thinking reflection and refraction are the same

Reflection sends a wave back. Refraction involves transmission into a region where wave speed changes.

Thinking a reflected wave always becomes inverted

Inversion depends on the type of boundary. A rope pulse at a fixed end inverts; at a free end it does not.

Measuring angles from the boundary

Angles are measured from the normal.

Thinking frequency changes during refraction

Frequency remains constant when the wave crosses the boundary.

Thinking wavelength remains constant

If speed changes while frequency remains constant, wavelength must change.

Thinking slower waves have longer wavelengths during refraction

With constant frequency:

slower → shorter wavelength

Thinking faster waves bend toward the normal

For ordinary refraction:

faster → away from normal

slower → toward normal

Thinking a wave must change direction to undergo refraction

A wave entering along the normal can change speed and wavelength without changing direction.

Thinking reflection and refraction cannot happen together

A boundary can reflect some wave energy while transmitting and refracting the rest.

Thinking wavefront spacing represents frequency

Wavefront spacing represents wavelength.


Key Terms

Boundary — location where the conditions through which a wave travels change.

Incident wave — wave approaching a boundary.

Reflected wave — wave travelling back from a boundary.

Transmitted wave — portion of a wave that passes into another region.

Reflection — return of a wave from a boundary.

Refraction — change in wave behaviour caused by a change in wave speed when entering another region, often producing a change in direction.

Normal — imaginary line perpendicular to a boundary.

Angle of incidence — angle between the incident direction and the normal.

Angle of reflection — angle between the reflected direction and the normal.

Fixed boundary — boundary that cannot move freely and can invert a reflected rope pulse.

Free boundary — boundary able to move, producing a non-inverted reflected pulse in the ideal rope model.

Wave speed (v) — speed at which a wave disturbance propagates.

Frequency (f) — number of complete wave cycles passing a point each second.

Wavelength (λ) — distance between corresponding points on consecutive wave cycles.

Wavefront — line joining points on a wave that are at the same stage of oscillation.

Refractive index — quantity describing the reduction of light speed in a material relative to vacuum.

Echo — reflected sound that reaches an observer after the original sound.

Transmission — passage of wave energy through a boundary into another region.


Key Takeaways

  • Waves can reflect and refract when they encounter boundaries.
  • Reflection occurs when wave energy returns into the original region.
  • Refraction occurs when a wave enters a region where its speed changes.
  • A reflected rope pulse inverts at an ideal fixed end.
  • A reflected rope pulse does not invert at an ideal free end.
  • For regular reflection, the angle of incidence equals the angle of reflection.
  • Angles are measured from the normal.
  • Refraction occurs because wave speed changes.
  • A wave entering a slower region at an angle bends toward the normal.
  • A wave entering a faster region at an angle bends away from the normal.
  • A wave entering along the normal can change speed without changing direction.
  • Frequency remains constant when a wave crosses a boundary.
  • The wave equation is v = fλ.
  • If speed decreases while frequency remains constant, wavelength decreases.
  • If speed increases while frequency remains constant, wavelength increases.
  • Wavefront spacing represents wavelength.
  • Water waves slow and shorten in wavelength when moving into sufficiently shallow water.
  • Light refracts when its speed changes between optical media.
  • Sound can refract when sound speed varies through the atmosphere or another medium.
  • Seismic waves reflect and refract at boundaries inside Earth.
  • Reflection and refraction can occur simultaneously at the same boundary.
  • Echoes, mirrors, sonar, and ultrasound demonstrate reflection.
  • Lenses, water-wave bending, atmospheric sound bending, and seismic-wave paths demonstrate refraction.
  • Comparing speed, wavelength, and direction provides a reliable way to analyze wave behaviour at boundaries.

Check Your Understanding

  1. Define reflection of a wave.
  2. Explain what happens when a wave pulse reflects from an ideal fixed boundary and compare this with reflection from a free boundary.
  3. State the law of reflection and explain how the angles are measured.
  4. Define refraction and explain why a wave can change direction when it enters a new region.
  5. Water waves travel from deep water into shallower water at an angle. Predict what happens to their speed, frequency, wavelength, and direction.
  6. Why does the frequency of a wave remain constant when it crosses a boundary?
  7. A wave has a frequency of 5 Hz and travels at 4 m/s. Calculate its wavelength.
  8. The wave in Question 7 enters another region where its speed decreases to 2.5 m/s. Calculate its new wavelength.
  9. Explain why wavefronts become closer together when a wave enters a slower region.
  10. A wave enters a faster region at an angle. Predict how its direction and wavelength change.
  11. Explain why a wave travelling directly along the normal can undergo refraction without changing direction.
  12. Compare reflection and refraction, identifying at least two similarities and two differences.
  13. Explain how both reflection and refraction can occur when light reaches a glass window.
  14. Describe one example of reflection involving sound, light, water waves, or seismic waves, and explain the physical process involved.
  15. Ocean waves approach a beach at an angle. One end of each wavefront reaches shallow water before the other. Explain how this causes the wavefront to rotate, predict the changes in speed and wavelength, and explain why the waves tend to become more nearly parallel to the shoreline.
 
 
 

3. Diffraction

Learning Outcomes
  • I can explain diffraction.
  • I can predict when diffraction is greatest.
  • I can describe diffraction around obstacles.
  • I can relate wavelength to diffraction.
  • I can identify real-world examples of diffraction.

Diffraction

Diffraction is the spreading or bending of waves when they pass through an opening or travel around the edge of an obstacle.

Diffraction is a fundamental property of waves and can occur with:

  • water waves
  • sound waves
  • light waves
  • radio waves
  • microwaves
  • seismic waves

The amount of diffraction depends strongly on the relationship between the wavelength and the size of the opening or obstacle.

https://images.openai.com/static-rsc-4/iYauiC_wWh5bCwrONF88BZBGbN5UdhL8WJRt1iBIKhCUg57Ln_c6ANTTaAS9Bl0WzvOcdLFmpKXr0fFpkVPHSJkewHvcbzuWwwgN-KFnmhOQY5vgRI_LyUNMAVvSakk0wyfPnHrgdsdEV1sRFbYz0T-q8soyMEVftoO7mhxbUSzn_5hacVa7F3qgMwO0ClXQ?purpose=fullsize
 
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7

What Is Diffraction?

When a wave encounters an opening or obstacle, it does not always continue only in a straight line.

Instead, the wave can spread into regions that would otherwise appear to be behind the barrier.

This spreading is called:

diffraction

For example, water waves passing through a narrow gap can spread outward in curved wavefronts.

Similarly, sound can travel around a doorway or corner even when the sound source cannot be seen directly.


Diffraction Through an Opening

Imagine straight water-wave fronts approaching a gap in a barrier.

After passing through the gap, the waves spread outward.

The amount of spreading depends on:

  • wavelength, λ
  • width of the opening

If the opening is very wide compared with the wavelength, there is relatively little spreading.

If the opening is similar in size to the wavelength, there is strong spreading.

https://images.openai.com/static-rsc-4/Ngzt93MUpLafwA7yvoHqcaaDNYQf6FGWgQzb_fwv7EdBVz9Dx51VYMI_6P9eLpFYFr7dWtFEzYh_Kq0zT2CO7Asx05pvPb92qG2uDDuOfpXSBXcC1PrU5fAWiOJ_di2ufNJA2pktHyMGJ2OMSqHPaN0NuOQ-z1H9qthUmLPJsyQCsQn8x_MangbiPFpwfw8A?purpose=fullsize
 
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5

When Is Diffraction Greatest?

Diffraction is especially noticeable when the size of the opening is approximately comparable to the wavelength.

A useful rule is:

opening size ≈ wavelength → strong diffraction

If the opening becomes smaller relative to the wavelength, spreading can become even more pronounced, although less wave energy may pass through a very small opening.

If:

opening size ≫ wavelength

the waves mainly continue forward with only limited spreading near the edges.


Comparing Gap Sizes

Suppose waves have wavelength:

λ = 2 m

Consider three openings.

Opening A = 20 m

The opening is much larger than the wavelength.

Result:

little diffraction

Opening B = 2 m

The opening is approximately equal to the wavelength.

Result:

strong diffraction

Opening C = 1 m

The opening is smaller than the wavelength.

Result:

very strong spreading of the transmitted wave, although the amount of transmitted energy may be reduced.


Wide Opening

When the opening is much wider than the wavelength:

gap ≫ λ

most of the wavefront continues approximately straight.

Diffraction occurs mainly near the edges.

The central part of the wavefront remains relatively straight.

This is sometimes described as:

weak diffraction


Opening Similar to the Wavelength

When:

gap ≈ λ

the wave spreads strongly after passing through the opening.

The outgoing wavefront can become approximately semicircular in a two-dimensional ripple-tank model.

This is one of the clearest demonstrations of diffraction.


Very Narrow Opening

When an opening is narrow compared with the wavelength, the portion of the wave that passes through can spread through a very large range of directions.

The opening behaves approximately like a new source of waves.

This idea helps explain why narrow gaps can produce strongly curved outgoing wavefronts.


Wavelength and Diffraction

For a fixed opening:

longer wavelength → more noticeable diffraction

shorter wavelength → less noticeable diffraction

The wavelength must always be considered relative to the dimensions of the obstacle or opening.

It is therefore better to ask:

How large is the wavelength compared with the gap or obstacle?

rather than simply asking whether the wavelength is "long" or "short."


Comparing Two Wavelengths

Suppose an opening is:

1 m wide

Wave A has:

λ = 0.10 m

Wave B has:

λ = 1.0 m

For Wave A:

gap = 10λ

The opening is much wider than the wavelength.

Diffraction is relatively small.

For Wave B:

gap = λ

The opening is comparable to the wavelength.

Diffraction is strong.

Therefore:

Wave B diffracts more strongly.


Diffraction Around an Obstacle

Waves can also diffract around the edges of obstacles.

Instead of creating a perfectly sharp wave-free region behind the obstacle, waves can bend into the region behind it.

The amount of diffraction depends on the obstacle's size relative to the wavelength.

https://images.openai.com/static-rsc-4/Y4NH1ORwGLe1qOJIgNP8g5_crbzZ9VHB3XZfzt2ro8K7Bug1ZUYNSjvgAG0NsWdWp7POvxGuel7sAKy-OBs5-xPGkpVE0hkAC23MCZfRdvI-dIiedqn8Z1BfR0oI4NDs5DknQSkLzRqsQD2j53DSPvz4q7pxrVqQ6wfD_7wI-RLGnoZAwlqS-Ff0Fxw_Rcye?purpose=fullsize
 
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12

Large Obstacles

Suppose the obstacle is much larger than the wavelength.

Then:

obstacle size ≫ wavelength

diffraction around the edges is relatively limited.

A substantial wave shadow can form behind the obstacle.

This is one reason short-wavelength waves tend to produce sharper shadow regions.


Obstacles Comparable to the Wavelength

If the obstacle is similar in size to the wavelength, diffraction becomes much more noticeable.

The waves bend around the edges and can enter the region behind the obstacle.

Therefore:

obstacle size ≈ wavelength → significant diffraction


Diffraction Does Not Mean the Wave Changes Speed

Diffraction is different from refraction.

During diffraction in the same medium:

  • wave speed remains the same
  • frequency remains the same
  • wavelength remains the same

What changes is mainly:

the direction in which the wave energy spreads

This is an important distinction.


Diffraction vs Refraction

Diffraction

occurs when waves spread around obstacles or through openings.

Refraction

occurs when wave speed changes as a wave enters a different region or medium.

During diffraction in the same medium:

v, f, and λ remain unchanged

During refraction:

v and λ can change while f remains constant


Diffraction vs Reflection

Reflection

causes a wave to return from a boundary.

Diffraction

causes a wave to spread around an edge or through an opening.

For example, when water waves encounter a harbour wall:

  • some waves may reflect from the wall
  • waves passing the end of the wall may diffract around it

Several wave behaviours can therefore occur in the same situation.


Comparing Reflection, Refraction, and Diffraction

Phenomenon Main Behaviour Typical Cause
Reflection Wave returns Boundary
Refraction Speed and often direction change Change in wave speed
Diffraction Wave spreads Gap or obstacle

All three are general wave behaviours.


Water-Wave Diffraction

Water waves provide an easy way to observe diffraction.

In a ripple tank, straight wavefronts can be directed toward a barrier containing a gap.

When the gap is wide compared with the wavelength:

  • most wavefronts continue straight
  • some spreading occurs near the edges

When the gap is comparable to the wavelength:

  • the wave spreads strongly
  • curved wavefronts emerge
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6

Changing the Gap Width

Suppose wavelength stays constant.

If the gap becomes progressively narrower:

diffraction generally becomes more noticeable

when the gap becomes comparable to the wavelength.

This is why ripple-tank experiments often use an adjustable gap.

Students can change the opening while keeping the wave source approximately constant.


Changing the Wavelength

Suppose gap width stays constant.

Increasing the wavelength makes the gap smaller relative to the wavelength.

Therefore:

longer wavelength → stronger diffraction

Decreasing wavelength makes the gap larger relative to the wavelength.

Therefore:

shorter wavelength → weaker diffraction


Sound Diffraction

Sound waves have wavelengths large enough that diffraction is common in everyday life.

This is why you can often hear someone:

  • around a corner
  • through an open doorway
  • behind an obstacle
  • on the other side of a partially open barrier

The sound waves diffract around edges and through openings.


Hearing Around a Corner

Suppose someone is speaking in a hallway around a corner.

There is no straight line between the speaker and listener.

However, sound waves can diffract around the corner.

Some sound energy reaches the listener.

Therefore:

you can hear someone you cannot see.

This is a simple everyday example of diffraction.


Low- and High-Frequency Sound

For sound travelling at approximately the same speed:

v = fλ

Therefore:

λ = v/f

Lower-frequency sound has a:

longer wavelength

Higher-frequency sound has a:

shorter wavelength

Since longer wavelengths generally diffract more strongly around a given obstacle:

low-frequency sounds tend to bend around large obstacles more effectively than high-frequency sounds.


Worked Example: Sound Wavelength

Assume the speed of sound is:

340 m/s

A low-frequency sound has:

f = 170 Hz

Calculate wavelength:

λ = v/f

λ = 340/170

λ = 2.0 m

Now consider a sound with:

f = 3400 Hz

λ = 340/3400

λ = 0.10 m

The 170 Hz sound has a much longer wavelength.

It will generally show more noticeable diffraction around metre-scale obstacles.


Why Bass Can Be Heard Around Obstacles

Bass sounds have relatively low frequencies and long wavelengths.

Their wavelengths may be comparable to the sizes of:

  • doorways
  • walls
  • vehicles
  • buildings

As a result, low-frequency sound can diffract significantly.

This is one reason bass from music may remain noticeable even when the source is behind an obstacle.


Light Diffraction

Light is also a wave and therefore undergoes diffraction.

However, visible-light wavelengths are extremely small:

approximately:

380–750 nm

or:

3.8 × 10⁻⁷ m to 7.5 × 10⁻⁷ m

Everyday objects and openings are usually enormously larger than these wavelengths.

Therefore, diffraction of visible light is often difficult to notice in ordinary situations.


Why Light Appears to Travel in Straight Lines

A doorway might be approximately:

1 m wide

Visible-light wavelength is approximately:

10⁻⁷ m

The doorway is therefore millions of wavelengths wide.

Consequently, diffraction is extremely small on the everyday scale.

Light therefore appears to travel in nearly straight lines and can produce sharp shadows.

Sound, with much longer wavelengths, can spread around the same doorway much more noticeably.


Diffraction of Light Through a Narrow Slit

If light passes through an extremely narrow slit whose dimensions become sufficiently small relative to its wavelength, diffraction becomes observable.

Instead of producing a perfectly sharp narrow line on a screen, the light spreads into a pattern.

A typical single-slit diffraction pattern includes:

  • a broad central bright region
  • darker regions
  • weaker bright regions on either side

This provides strong evidence that light behaves as a wave.

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6

Diffraction and Wave Evidence

Diffraction is characteristic of wave behaviour.

Experiments showing light diffraction helped establish that light has wave properties.

Today, light is understood through quantum physics, but diffraction remains one of the clearest demonstrations of its wave behaviour.


Radio-Wave Diffraction

Radio waves can have wavelengths much longer than visible light.

Depending on their frequency, some radio waves can diffract around:

  • buildings
  • hills
  • other large obstacles

This can allow signals to reach regions without a perfectly clear line of sight.

The amount of diffraction depends on the wavelength and the dimensions of the obstacle.


Radio Frequency and Wavelength

Since:

v = fλ

and electromagnetic waves in air travel at approximately the same speed:

lower-frequency radio waves generally have:

longer wavelengths

Higher-frequency electromagnetic waves generally have:

shorter wavelengths

Longer-wavelength signals can therefore show stronger diffraction around a given obstacle.


Communication Systems

Diffraction is important when engineers design communication systems.

They must consider:

  • transmitter frequency
  • wavelength
  • buildings
  • terrain
  • antenna positions
  • line of sight

Different frequencies behave differently around obstacles.

This affects technologies such as:

  • radio broadcasting
  • wireless communication
  • navigation systems
  • telecommunications

Microwaves and Diffraction

Microwaves also undergo diffraction.

Their wavelengths can range from approximately millimetres to tens of centimetres, depending on frequency.

Engineers must consider diffraction when designing:

  • microwave communication links
  • radar systems
  • satellite communication
  • antennas

At many microwave frequencies, obstacles such as buildings are much larger than the wavelength, so line-of-sight effects can become particularly important.


Diffraction Around Harbour Openings

Harbours provide a useful large-scale example of diffraction.

Ocean waves enter through an opening between harbour walls.

After passing through the entrance, the waves can spread into the sheltered region.

If the entrance width is comparable to the wavelength, significant diffraction can occur.

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9

Breakwaters

A breakwater is a structure designed to reduce wave energy reaching a protected area.

However, waves can diffract around the ends of a breakwater.

Engineers must therefore consider:

  • wavelength
  • breakwater length
  • harbour entrance width
  • direction of incoming waves

A region behind a barrier may not be completely protected because waves can spread into it through diffraction.


Seismic-Wave Diffraction

Seismic waves can also diffract around structures and boundaries inside Earth.

Their wavelengths can be very large.

This means they can bend and spread around geological features.

Seismologists consider diffraction along with:

  • reflection
  • refraction
  • wave-speed changes

when interpreting seismic data.


Diffraction and Shadows

Diffraction explains why wave shadows are not always perfectly sharp.

For short wavelengths relative to an obstacle:

sharper shadow

For wavelengths comparable to the obstacle:

greater spreading into the shadow region

This explains why:

  • visible light often produces relatively sharp shadows
  • sound can reach behind obstacles

The Huygens Idea

A useful model for understanding diffraction is Huygens' principle.

It treats each point on a wavefront as a source of small secondary wavelets.

The next wavefront is formed from the combined effect of these wavelets.

At an opening or edge, some of these wavelets spread into regions that would otherwise be behind the barrier.

This helps explain why waves diffract.


Diffraction Through a Narrow Gap Using Huygens' Principle

Imagine a plane wave reaching a very narrow gap.

Only a small portion of the original wavefront passes through.

The opening then behaves approximately like a point source.

The outgoing waves spread in many directions.

In two dimensions, the resulting wavefronts can appear approximately semicircular.

This explains the strong diffraction seen in ripple-tank experiments.


Diffraction Around an Edge

Huygens' principle also helps explain diffraction around an obstacle.

Points on the wavefront near the edge act as sources of secondary wavelets.

These wavelets spread into the region behind the obstacle.

Therefore, the boundary of the wave shadow is not perfectly sharp.


Predicting Diffraction from a Diagram

When given a wave diagram, compare:

λ = wavelength

with:

a = opening or obstacle size

If:

a ≫ λ

predict:

little diffraction

If:

a ≈ λ

predict:

strong diffraction

If:

a < λ

predict:

very strong angular spreading of the transmitted wave, although transmission through a very small opening may be reduced.


Example: Comparing Three Waves

A gap is:

2 m wide

Wave A:

λ = 0.1 m

Wave B:

λ = 1.5 m

Wave C:

λ = 2.0 m

Compare the ratios.

Wave A:

2/0.1 = 20 wavelengths across

Diffraction is relatively weak.

Wave B:

2/1.5 ≈ 1.3 wavelengths across

Diffraction is strong.

Wave C:

2/2 = 1 wavelength across

Diffraction is very strong.

Therefore, Wave C produces the greatest spreading of the three.


Example: Changing Frequency

Two sound waves travel through the same air.

Wave A:

f = 200 Hz

Wave B:

f = 2000 Hz

Because they travel at approximately the same speed:

Wave A has the longer wavelength.

Therefore, around the same obstacle:

Wave A generally diffracts more strongly.

This shows the connection:

lower frequency → longer wavelength → greater diffraction

when wave speed and obstacle size remain approximately constant.


Diffraction Does Not Create New Waves

When a wave diffracts, it may look as though new waves are being produced at an opening.

However, the outgoing wave is the continuation of the original disturbance.

Its energy has been redistributed across a wider range of directions.

Diffraction changes the spatial distribution of wave energy.

It does not create energy.


Energy and Diffraction

As a wave spreads over a larger region, its energy is distributed over that region.

Therefore, strong spreading does not mean that every point receives the same intensity as the original wave.

The shape and intensity of a real diffraction pattern depend on factors such as:

  • wavelength
  • opening geometry
  • distance from the opening
  • original wave amplitude

Applications of Diffraction

Diffraction has many practical consequences.

Sound

Allows sound to spread around obstacles and through openings.

Radio communication

Helps some radio signals reach behind hills and buildings.

Harbours

Causes water waves to spread through harbour entrances and around breakwaters.

Optical instruments

Diffraction places a fundamental limit on resolution.

Spectroscopy

Diffraction gratings can separate light according to wavelength.

Astronomy

Diffraction affects the smallest details telescopes can resolve.

Microscopy

Diffraction limits how closely spaced structures can be distinguished using ordinary light.


Diffraction Gratings

A diffraction grating contains many closely spaced parallel lines or openings.

Light passing through or reflecting from the grating diffracts.

The diffracted waves interfere with one another.

Different wavelengths emerge strongly at different angles.

This allows a diffraction grating to separate light into a spectrum.

Diffraction gratings are widely used in:

  • spectrometers
  • laboratory instruments
  • astronomy
  • chemical analysis

Diffraction and Optical Resolution

Even a perfect optical instrument cannot resolve infinitely small details.

Light passing through a finite aperture diffracts.

This produces a small diffraction pattern rather than an infinitely sharp point.

Therefore, diffraction places a fundamental limit on the resolution of:

  • telescopes
  • microscopes
  • cameras

Larger apertures generally reduce diffraction spreading and improve potential resolution for a given wavelength.


A Complete Water-Wave Example

Water waves have:

λ = 4 cm

They approach a barrier with a:

20 cm opening.

The opening is:

20/4 = 5 wavelengths wide.

Some diffraction occurs, especially near the edges, but the wavefront remains substantially forward-directed.

The opening is then reduced to:

4 cm.

Now:

gap = wavelength.

Strong diffraction occurs.

The waves spread broadly beyond the opening.

The wavelength has not changed because the waves remain in the same water conditions.

Only their pattern of propagation has changed.


A Complete Sound Example

A sound wave travels through air at:

340 m/s

with frequency:

170 Hz

Its wavelength is:

λ = v/f

λ = 340/170

λ = 2.0 m

The sound reaches a doorway approximately:

2 m wide.

Therefore:

doorway width ≈ wavelength

Significant diffraction can occur.

The sound can spread through the doorway into a wide range of directions.

This helps explain why a person inside the room can hear the sound even without standing directly in front of the doorway.


A Reliable Strategy for Diffraction Problems

When analyzing diffraction:

  1. Identify the type of wave.
  2. Determine the wavelength if it is given.
  3. If necessary, calculate wavelength using λ = v/f.
  4. Identify the width of the opening or size of the obstacle.
  5. Compare this size with the wavelength.
  6. If the opening is much larger than λ, predict limited diffraction.
  7. If the opening is comparable to λ, predict strong diffraction.
  8. If the opening is smaller than λ, predict very strong angular spreading of the transmitted wave.
  9. For obstacles, consider how much the wave can spread into the shadow region.
  10. Remember that frequency does not change simply because diffraction occurs.
  11. Remember that speed and wavelength also remain unchanged if the wave remains in the same medium.
  12. Sketch the outgoing wavefronts with appropriate curvature.

Common Mistakes

Thinking diffraction is refraction

Diffraction involves spreading around edges or through openings.

Refraction involves a change in wave speed.

Thinking diffraction requires a new medium

A wave can diffract while remaining entirely in the same medium.

Thinking wavelength changes during diffraction

If the medium remains unchanged, speed and frequency remain unchanged, so wavelength remains unchanged.

Thinking only water waves diffract

All waves can diffract.

Thinking light does not diffract

Light does diffract, but its very short wavelength makes everyday diffraction difficult to notice.

Thinking sound travels around corners because it reflects from everything

Reflection may contribute in real environments, but diffraction itself allows sound to spread around edges.

Thinking diffraction occurs only through gaps

Waves also diffract around obstacles and edges.

Thinking a narrow opening always produces more transmitted energy

A narrower opening can produce greater angular spreading while allowing less total wave energy through.

Thinking longer wavelengths always diffract more in every situation

The important factor is the wavelength relative to the size of the opening or obstacle.

Thinking a diffracted wave has gained energy

Diffraction redistributes existing wave energy; it does not create energy.


Key Terms

Diffraction — spreading of waves as they pass through openings or around obstacles.

Wavelength (λ) — distance between corresponding points on consecutive wave cycles.

Opening — gap through which a wave can pass.

Obstacle — object that blocks part of an incoming wave.

Wavefront — line joining points on a wave that are at the same stage of oscillation.

Wave shadow — region behind an obstacle receiving reduced wave energy.

Ripple tank — apparatus used to observe water-wave behaviour.

Huygens' principle — model in which points on a wavefront act as sources of secondary wavelets.

Secondary wavelet — small wave used in Huygens' model to construct the next wavefront.

Single-slit diffraction — spreading of a wave after passing through one narrow opening.

Diffraction grating — structure containing many closely spaced lines or openings that produces diffraction and interference.

Resolution — ability of an instrument to distinguish closely spaced details.

Aperture — opening through which a wave enters an optical or other wave system.

Shadow region — region behind an obstacle where direct wave propagation is blocked.

Frequency (f) — number of complete wave cycles passing a point each second.

Wave speed (v) — rate at which a wave disturbance propagates.


Key Takeaways

  • Diffraction is the spreading of waves through openings and around obstacles.
  • All types of waves can undergo diffraction.
  • The amount of diffraction depends strongly on wavelength relative to opening or obstacle size.
  • Diffraction is especially noticeable when the opening is comparable to the wavelength.
  • A wave can spread very strongly when an opening is smaller than its wavelength, although less energy may be transmitted.
  • A wide opening compared with wavelength produces relatively little diffraction.
  • Longer wavelengths generally diffract more strongly around a fixed-size opening or obstacle.
  • Shorter wavelengths generally produce less diffraction for the same geometry.
  • During diffraction in the same medium, speed remains unchanged.
  • Frequency remains unchanged.
  • Wavelength remains unchanged.
  • Diffraction changes the directions over which wave energy propagates.
  • Waves can diffract around obstacles into regions that would otherwise be wave shadows.
  • Sound diffraction explains why sounds can often be heard around corners.
  • Low-frequency sound generally has longer wavelengths and diffracts more noticeably around everyday obstacles.
  • Visible light diffracts, but its wavelength is extremely short compared with most everyday objects.
  • Narrow slits can produce observable diffraction patterns with light.
  • Water-wave diffraction can be clearly observed in a ripple tank.
  • Radio waves can diffract around large obstacles depending on their wavelengths.
  • Ocean waves can diffract through harbour openings and around breakwaters.
  • Diffraction gratings use diffraction and interference to separate wavelengths.
  • Diffraction places a fundamental limit on the resolution of optical instruments.
  • Huygens' principle provides a useful model for explaining how waves spread around edges and through openings.
  • Reflection, refraction, and diffraction are distinct but fundamental wave behaviours.

Check Your Understanding

  1. Define diffraction.
  2. Describe what happens when straight water waves pass through a narrow opening.
  3. Under what condition is diffraction especially noticeable?
  4. Waves with a wavelength of 3 cm approach two openings. Opening A is 30 cm wide and Opening B is 3 cm wide. Predict which opening will produce greater diffraction and explain why.
  5. Explain how the amount of diffraction changes when wavelength increases while gap width remains constant.
  6. Explain how the amount of diffraction changes when gap width decreases while wavelength remains constant.
  7. Describe how waves can diffract around an obstacle and explain what happens in the wave-shadow region.
  8. A sound wave travels at 340 m/s and has a frequency of 170 Hz. Calculate its wavelength. Would you expect significant diffraction through a doorway approximately 2 m wide? Explain.
  9. Two sounds have frequencies of 200 Hz and 2000 Hz and travel through the same air. Which one is likely to diffract more strongly around a large obstacle? Explain using wavelength.
  10. Explain why sound can often be heard around a corner even when the sound source cannot be seen.
  11. Visible light and sound both pass through a doorway. Explain why sound generally shows much more obvious diffraction than visible light.
  12. During diffraction, what happens to the wave's speed, frequency, and wavelength if the medium does not change?
  13. Compare diffraction, reflection, and refraction. Describe the main cause and behaviour associated with each.
  14. Explain why diffraction is important when engineers design harbour entrances, breakwaters, communication systems, microscopes, or telescopes.
  15. A student says, "If I make a gap narrower, the wavelength of the wave becomes shorter and that causes more diffraction." Explain what is wrong with this statement and give the correct relationship between gap size, wavelength, and diffraction.

4. Interference

Learning Outcomes
  • I can explain how interference patterns form.
  • I can distinguish between constructive and destructive interference.
  • I can identify conditions for interference.
  • I can interpret simple interference diagrams.
  • I can explain applications of interference.

Interference

Interference occurs when two or more waves overlap and combine. The displacement produced at any point is determined by the principle of superposition:

resultant displacement = displacement₁ + displacement₂ + ...

When waves repeatedly overlap in a predictable way, they can produce an interference pattern containing regions of strong and weak wave effects.

Interference occurs with many types of waves, including:

  • water waves
  • sound waves
  • light waves
  • microwaves
  • radio waves
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6

How Interference Patterns Form

Consider two sources producing waves in the same region.

Each source sends waves outward. Where the waves overlap, their displacements combine.

At some locations, the waves reinforce each other.

This produces:

constructive interference

At other locations, the waves oppose each other.

This produces:

destructive interference

If the sources continuously produce waves with a stable relationship, fixed regions of constructive and destructive interference can develop.

Together, these regions form an:

interference pattern


Superposition and Interference

Interference is a consequence of the principle of superposition.

At every point where waves overlap:

resultant displacement = sum of individual displacements

For example:

Wave A = +3 cm
Wave B = +2 cm

Resultant:

+3 + 2 = +5 cm

The waves reinforce each other.

Now suppose:

Wave A = +3 cm
Wave B = −2 cm

Resultant:

+3 − 2 = +1 cm

The waves partially cancel.


Constructive Interference

Constructive interference occurs when waves overlap with displacements that reinforce one another.

For example:

crest + crest → larger crest

trough + trough → deeper trough

If two identical waves each have an amplitude of 4 cm and their crests overlap:

resultant displacement = +4 + +4

= +8 cm

This is maximum constructive interference.

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8

Destructive Interference

Destructive interference occurs when overlapping waves have displacements in opposite directions.

For example:

crest + trough → reduced displacement

If:

Wave A = +5 cm

Wave B = −3 cm

then:

resultant = +5 − 3

= +2 cm

This is partial destructive interference.


Complete Destructive Interference

If two equal and opposite displacements overlap:

Wave A = +5 cm

Wave B = −5 cm

then:

resultant = +5 − 5

= 0 cm

This is complete destructive interference.

The waves have not been permanently destroyed. Their displacements simply cancel at that location and instant.

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7

Constructive vs Destructive Interference

Constructive Interference Destructive Interference
Waves reinforce Waves oppose
Crest aligns with crest Crest aligns with trough
Trough aligns with trough Opposite displacements overlap
Resultant amplitude increases Resultant amplitude decreases
Can produce maximum intensity Can produce minimum intensity

The exact result depends on the amplitudes and relative phases of the waves.


Phase

Phase describes where a wave is within its cycle.

Two waves are in phase when corresponding parts of their cycles occur together.

For example:

  • crest aligns with crest
  • trough aligns with trough
  • equilibrium crossing aligns in the same direction

Identical waves that are perfectly in phase produce maximum constructive interference.


Waves in Phase

Consider two identical waves.

If their crests and troughs line up exactly:

phase difference = 0°

They undergo maximum constructive interference.

For equal-amplitude waves:

A + A = 2A

Therefore, two waves each with amplitude A can produce a resultant amplitude of 2A when perfectly in phase.


Waves 180° Out of Phase

Suppose the crest of one identical wave aligns with the trough of another.

The waves are:

180° out of phase

or:

half a cycle out of phase

If their amplitudes are equal, they undergo complete destructive interference.

The resultant displacement is:

0


Intermediate Phase Differences

Waves do not have to be perfectly in phase or exactly 180° out of phase.

An intermediate phase difference produces partial interference.

The result may be:

  • partially constructive
  • partially destructive

Therefore, interference exists across a range of possibilities rather than only complete reinforcement or complete cancellation.


Conditions for a Stable Interference Pattern

To produce a clear, stable interference pattern, the waves should have a predictable phase relationship.

Sources that maintain a constant phase relationship are called:

coherent sources

For a stable pattern, waves generally need:

  • the same frequency
  • a constant phase difference
  • to overlap in the same region

Comparable amplitudes make destructive interference especially noticeable.


Coherent Sources

Coherent sources produce waves with:

  • the same frequency
  • a constant phase difference

The sources do not necessarily have to be exactly in phase.

What matters is that their phase difference remains constant.

If the phase relationship changes randomly, the positions of constructive and destructive interference continually shift, and a stable pattern is difficult to observe.


Why Frequency Matters

Suppose two sources have different frequencies.

Their relative phase continually changes.

A location that experiences constructive interference at one moment may soon experience destructive interference.

Therefore, a stable interference pattern normally requires waves of the same frequency.


Path Difference

Even if two sources are in phase, their waves may travel different distances before reaching a particular point.

The difference between these distances is called the:

path difference

Suppose:

distance from Source 1 = d₁

distance from Source 2 = d₂

Then:

path difference = |d₁ − d₂|

Path difference helps determine whether the waves arrive in phase or out of phase.


Constructive Interference and Path Difference

For two coherent sources initially in phase, maximum constructive interference occurs when the path difference is a whole number of wavelengths:

path difference = 0, λ, 2λ, 3λ, ...

This can be written:

path difference = nλ

where:

n = 0, 1, 2, 3, ...

At these locations, crest tends to meet crest and trough tends to meet trough.


Destructive Interference and Path Difference

For two coherent sources initially in phase, maximum destructive interference occurs when the path difference is an odd number of half-wavelengths:

path difference = λ/2, 3λ/2, 5λ/2, ...

This can be written:

path difference = (n + 1/2)λ

where:

n = 0, 1, 2, 3, ...

At these locations, a crest from one wave tends to meet a trough from the other.


Path Difference Summary

For coherent sources that begin in phase:

Path Difference Interference
0 Constructive
λ/2 Destructive
λ Constructive
3λ/2 Destructive
2λ Constructive
5λ/2 Destructive
3λ Constructive

A useful pattern is:

whole wavelengths → constructive

odd half-wavelengths → destructive


Worked Example: Path Difference

Two coherent waves have:

λ = 0.40 m

At a particular point, one wave travels:

3.2 m

while the other travels:

2.8 m

Path difference:

3.2 − 2.8 = 0.40 m

Since:

λ = 0.40 m

the path difference is:

1λ

Therefore, the waves arrive in phase and produce:

constructive interference

assuming the sources started in phase.


Worked Example: Destructive Interference

Two coherent waves have:

λ = 0.60 m

At a particular location, the path difference is:

0.30 m

Since:

0.30 m = λ/2

the waves arrive 180° out of phase.

Therefore:

destructive interference

occurs.

If their amplitudes are equal, the cancellation can be complete.


Two-Source Interference

Imagine two identical sources:

S₁ and S₂

producing circular water waves at the same frequency and in phase.

As the circular waves expand, they overlap.

At some locations:

crest + crest

produces constructive interference.

At others:

crest + trough

produces destructive interference.

A repeating pattern develops across the water surface.

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7

Antinodal Lines

A line along which constructive interference repeatedly occurs is called an:

antinodal line

Along these regions, the waves reinforce each other.

For equal-amplitude coherent sources, the oscillation amplitude can be relatively large.

Antinodal lines therefore correspond to regions of strong wave motion.


Nodal Lines

A line along which destructive interference repeatedly occurs is called a:

nodal line

For equal-amplitude coherent sources, complete destructive interference can produce very small or zero resultant amplitude along these lines.

In a water-wave interference pattern, nodal lines can appear as regions with little vertical movement.


The Central Antinodal Line

Suppose two sources are:

  • coherent
  • in phase

Points exactly midway between the two sources are the same distance from each source.

Therefore:

d₁ = d₂

Path difference:

d₁ − d₂ = 0

A zero path difference corresponds to constructive interference.

Therefore, the centre of a symmetrical two-source pattern contains a:

central antinodal line


Moving Across an Interference Pattern

As you move across a two-source interference pattern, the path difference changes.

You may encounter:

constructive → destructive → constructive → destructive

This creates alternating regions of:

  • maximum wave effect
  • minimum wave effect

The pattern is not caused by waves stopping at those positions.

It is caused by continuous superposition.


Interpreting an Interference Diagram

When examining a diagram with two wave sources:

  1. Identify the two sources.
  2. Determine whether they are coherent.
  3. Identify the wavelength if possible.
  4. Choose a point of interest.
  5. Determine the distance from each source to that point.
  6. Calculate or compare the path difference.
  7. Compare the path difference with λ.
  8. Predict constructive or destructive interference.

For in-phase sources:

nλ → constructive

(n + 1/2)λ → destructive


Reading Crest-Line Diagrams

Some interference diagrams show only wave crests.

If two crest lines intersect:

crest + crest

This indicates constructive interference.

If a crest from one source meets a trough from another, destructive interference occurs.

If trough lines are not drawn, you may need to infer their positions halfway between neighbouring crest lines.


Interference of Water Waves

A ripple tank can demonstrate interference clearly.

Two vibrating sources create circular waves.

Where the waves overlap:

  • constructive interference produces larger oscillations
  • destructive interference produces smaller oscillations

A stable pattern of nodal and antinodal regions can form.

This is one of the easiest ways to visualize wave interference.


Interference of Sound Waves

Sound waves can also interfere.

Sound consists of pressure variations travelling through a medium.

When two sound waves overlap:

  • pressure variations can reinforce
  • pressure variations can oppose

Constructive interference can produce greater sound intensity.

Destructive interference can produce reduced sound intensity.


Two Loudspeakers

Suppose two loudspeakers produce the same pure tone and are driven coherently.

As a listener moves through the room, the distances from the two speakers change.

At some locations, the sound waves arrive nearly in phase.

The sound is stronger.

At other locations, the waves arrive nearly out of phase.

The sound is weaker.

This can produce alternating:

loud and quiet regions

due to interference.


Noise-Cancelling Headphones

Active noise-cancelling headphones use destructive interference.

A simplified process is:

  1. A microphone detects unwanted sound.
  2. Electronics analyze the incoming waveform.
  3. The headphones generate another sound.
  4. The generated sound is arranged to oppose the unwanted pressure variation.
  5. The waves overlap near the ear.
  6. Destructive interference reduces the unwanted sound.

This is particularly effective for steady, low-frequency noise.

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7

Interference of Light

Light waves also interfere.

When coherent light waves overlap, they can produce alternating regions of:

  • constructive interference
  • destructive interference

On a screen, these may appear as:

  • bright regions
  • dark regions

Bright regions correspond to greater light intensity.

Dark regions correspond to reduced intensity.


Young's Double-Slit Experiment

A famous demonstration of light interference is Young's double-slit experiment.

Light passes through two closely spaced slits.

The slits act as coherent sources.

The light waves spread by diffraction and overlap.

On a screen:

  • constructive interference produces bright fringes
  • destructive interference produces dark fringes

The result is an:

interference pattern

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9

Why the Double Slits Must Be Close

For a clear interference pattern, the waves emerging from the two slits must overlap significantly.

Diffraction from the slits helps the light spread.

If the geometry is suitable, waves from both slits reach the same parts of the screen.

Their path differences then determine whether each location is bright or dark.

Thus, diffraction and interference often work together in experiments.


Bright Fringes

For coherent, in-phase light sources, bright fringes occur where:

path difference = nλ

The waves arrive in phase.

Their electric-field amplitudes reinforce.

The observed light intensity is high.

This corresponds to:

constructive interference


Dark Fringes

Dark fringes occur where:

path difference = (n + 1/2)λ

The waves arrive out of phase.

Their electric-field amplitudes oppose.

For equal amplitudes, strong or nearly complete cancellation can occur.

This corresponds to:

destructive interference


Thin-Film Interference

Interference also explains colours seen in:

  • soap bubbles
  • oil films
  • thin transparent coatings

Light reflects from different surfaces of the thin layer.

The reflected waves travel different optical paths.

When they recombine:

  • some wavelengths interfere constructively
  • other wavelengths interfere destructively

Different wavelengths are therefore enhanced or reduced.

The result can be colourful patterns.

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8

Anti-Reflection Coatings

Interference can be deliberately used to reduce unwanted reflections.

An anti-reflection coating is a carefully designed thin layer placed on an optical surface.

Reflections from different boundaries of the coating can be arranged to interfere destructively for selected wavelengths.

This reduces reflected light and allows more light to pass through.

Applications include:

  • eyeglasses
  • camera lenses
  • microscopes
  • telescopes
  • optical sensors

Interferometers

An interferometer divides a wave into separate paths and then recombines the waves.

Small changes in path length alter the interference pattern.

Because wavelengths can be extremely small, interferometers can detect very small changes in:

  • distance
  • position
  • refractive index
  • surface shape

This makes interference useful for extremely precise measurement.


Interference and Standing Waves

Standing waves are another important result of interference.

A standing wave forms when two waves of:

  • the same frequency
  • similar or equal amplitude

travel in opposite directions and overlap.

Their interference produces fixed:

  • nodes
  • antinodes

Standing waves occur in:

  • guitar strings
  • violin strings
  • organ pipes
  • air columns
  • resonant cavities

Nodes and Antinodes in Standing Waves

A node is a position where destructive interference continuously produces zero displacement in the ideal case.

An antinode is a position where constructive interference produces maximum oscillation amplitude.

Standing waves demonstrate that interference can create stable spatial patterns.


Interference Does Not Permanently Change the Waves

When waves interfere, they do not normally destroy or permanently alter one another.

During overlap:

their displacements combine

Afterward:

each wave continues

This is a consequence of superposition in a linear system.

Even complete destructive interference does not mean that the waves have ceased to exist.


Interference and Energy

Destructive interference at one location does not mean energy has been destroyed.

Interference redistributes wave energy.

In an interference pattern:

  • some regions receive greater intensity
  • other regions receive lower intensity

The total energy remains consistent with conservation of energy.

This is especially clear in optical interference patterns, where bright regions are accompanied by dark regions.


Amplitude and Intensity

Amplitude and intensity are related, but they are not the same quantity.

For many waves:

intensity ∝ amplitude²

Therefore, if two equal coherent waves interfere constructively so that the amplitude doubles:

A → 2A

the maximum intensity can become:

(2A)² = 4A²

So the intensity can be four times that of one individual wave under ideal conditions.

This is an important distinction:

double amplitude does not simply mean double intensity.


Worked Example: Constructive Interference

Two identical coherent waves each have amplitude:

3 mm

They arrive perfectly in phase.

Resultant amplitude:

3 + 3 = 6 mm

The amplitude doubles.

If intensity is proportional to amplitude squared:

individual intensity ∝ 3² = 9

resultant maximum intensity ∝ 6² = 36

Therefore:

36/9 = 4

The maximum intensity is four times that produced by either wave individually.


Worked Example: Identifying a Node

Two coherent in-phase sources produce waves with:

λ = 0.80 m

At point P:

d₁ = 5.2 m

d₂ = 4.8 m

Path difference:

|5.2 − 4.8| = 0.40 m

Since:

λ/2 = 0.40 m

the path difference is:

λ/2

Therefore, point P lies on a region of:

destructive interference

For equal amplitudes, it can be a node.


Worked Example: Identifying an Antinode

Two coherent in-phase sources produce waves with:

λ = 0.50 m

At point Q:

d₁ = 4.0 m

d₂ = 3.0 m

Path difference:

|4.0 − 3.0| = 1.0 m

Since:

1.0 m = 2λ

the path difference is a whole number of wavelengths.

Therefore:

constructive interference

Point Q lies on an antinodal region.


Applications of Interference

Interference is important in many areas of science and technology.

Noise cancellation

Destructive interference reduces unwanted sound.

Optical coatings

Destructive interference reduces reflections.

Interferometry

Interference allows extremely precise measurements.

Spectroscopy

Interference helps separate and analyze wavelengths.

Radio communication

Interference affects signal strength and reception.

Musical instruments

Interference contributes to standing waves and resonance.

Thin films

Interference produces colours in soap bubbles and oil films.

Astronomy

Interferometry can combine information from multiple telescopes.


Radio-Wave Interference

Radio waves from different paths can interfere.

For example, a signal may travel:

  • directly from transmitter to receiver
  • indirectly after reflecting from a building

The two versions of the signal can arrive with different phases.

They may interfere:

  • constructively
  • destructively

This can cause signal strength to vary with position.


Why Moving Can Change Reception

If you move a receiver slightly, the path lengths from different wave sources or reflected paths change.

This changes the path difference.

A position that previously produced destructive interference may become constructive.

This is one reason wireless or radio signal strength can change significantly over relatively short distances.


Requirements for Clear Interference

For a clear and stable interference pattern, several conditions are helpful:

  • waves must overlap
  • sources should be coherent
  • frequencies should be the same
  • phase difference should remain constant
  • amplitudes should be sufficiently similar for strong contrast
  • the waves must be capable of interacting in the same region

For light, polarization can also matter. Waves with compatible polarization produce clearer interference.


Interference vs Superposition

These terms are closely related but not identical.

Superposition is the principle that overlapping wave displacements add.

Interference is the observable pattern or effect resulting from that superposition.

Therefore:

superposition is the rule

while:

interference is the resulting wave behaviour


Interference vs Diffraction

Interference and diffraction are also related.

Interference

usually emphasizes the combination of waves from two or more coherent contributions.

Diffraction

describes the spreading of waves through openings or around obstacles.

However, diffraction patterns themselves arise from interference between different parts of a wavefront.

Therefore, the two ideas are deeply connected.


A Complete Interference Example

Two coherent water-wave sources oscillate in phase.

The wavelength is:

0.40 m

At Point A:

d₁ = 3.0 m
d₂ = 3.0 m

Path difference:

0 m = 0λ

Therefore:

constructive interference

At Point B:

d₁ = 3.4 m
d₂ = 3.0 m

Path difference:

0.40 m = 1λ

Therefore:

constructive interference

At Point C:

d₁ = 3.2 m
d₂ = 3.0 m

Path difference:

0.20 m = λ/2

Therefore:

destructive interference

A pattern of constructive and destructive regions forms across the water surface.


Interpreting an Interference Pattern

When examining an interference diagram, ask:

Where are the sources?

Are the sources coherent?

What is the wavelength?

Are the sources initially in phase?

What is the path difference to the point?

Then compare that difference with the wavelength.

For in-phase sources:

0, λ, 2λ, 3λ... → constructive

λ/2, 3λ/2, 5λ/2... → destructive

This provides a reliable method for interpreting simple interference diagrams.


A Reliable Strategy for Interference Problems

  1. Identify the waves or sources.
  2. Check whether the waves overlap.
  3. Determine whether the sources are coherent.
  4. Identify the wavelength.
  5. Determine whether the sources begin in phase.
  6. Find the path length from each source to the point.
  7. Calculate the path difference.
  8. Express the path difference in terms of λ.
  9. For in-phase sources, use whole wavelengths for constructive interference.
  10. Use odd half-wavelengths for destructive interference.
  11. Determine whether the point is near a node or antinode.
  12. If amplitudes are given, add the displacements using superposition.
  13. Interpret the physical result.
  14. Check whether the answer matches the diagram.

Common Mistakes

Thinking interference occurs only when two waves collide head-on

Waves can interfere whenever they overlap.

Confusing interference with superposition

Superposition is the rule for adding displacements. Interference is the resulting effect or pattern.

Thinking constructive interference always means two crests

Two troughs can also reinforce each other.

Thinking destructive interference always gives zero

Complete cancellation requires equal and opposite displacements.

Thinking destructive interference destroys the waves

The waves continue after overlapping.

Thinking destructive interference destroys energy

Energy is redistributed through the interference pattern.

Thinking coherent means identical amplitude

Coherence requires a stable phase relationship, not necessarily equal amplitudes.

Thinking coherent sources must always be exactly in phase

They may have a constant non-zero phase difference.

Using the whole-wavelength rule without checking source phase

The simple nλ and (n + 1/2)λ rules given here assume sources that begin in phase.

Confusing path difference with distance from one source

Path difference is the difference between the two path lengths.

Thinking every dark fringe contains absolutely no light

Perfect cancellation requires ideal equal-amplitude coherent waves. Real experiments may not produce perfectly zero intensity.

Confusing nodes and antinodes

Nodes correspond to minimum displacement; antinodes correspond to maximum oscillation in standing-wave patterns.


Key Terms

Interference — effect produced when overlapping waves combine through superposition.

Interference pattern — arrangement of regions of constructive and destructive interference.

Superposition — principle stating that overlapping wave displacements add.

Constructive interference — reinforcement of overlapping wave displacements.

Destructive interference — reduction of resultant displacement when opposing wave displacements overlap.

Complete destructive interference — zero resultant displacement produced by equal and opposite contributions.

Phase — position of a wave within its oscillation cycle.

Phase difference — difference between the phases of two waves.

In phase — waves whose corresponding parts of their cycles align.

Coherent sources — sources that maintain the same frequency and a constant phase difference.

Path length — distance travelled by a wave from its source to a particular point.

Path difference — difference between the path lengths travelled by two waves.

Node — position of minimum or zero displacement in an ideal interference or standing-wave pattern.

Antinode — position of maximum oscillation in a standing-wave pattern.

Nodal line — line of destructive interference in a two-source wave pattern.

Antinodal line — line of constructive interference in a two-source wave pattern.

Fringe — bright or dark band in an optical interference pattern.

Intensity — rate of wave energy transfer per unit area.

Interferometer — instrument that uses interference for precise measurement.

Thin-film interference — interference involving waves reflected from different surfaces of a thin layer.


Key Takeaways

  • Interference occurs when waves overlap.
  • Interference is explained using the principle of superposition.
  • Constructive interference occurs when wave displacements reinforce.
  • Destructive interference occurs when wave displacements oppose.
  • Equal in-phase waves can produce a resultant amplitude twice that of either wave alone.
  • Equal waves 180° out of phase can undergo complete destructive interference.
  • A stable interference pattern requires a stable phase relationship between waves.
  • Coherent sources have the same frequency and a constant phase difference.
  • Path difference determines the relative phase of waves arriving at a point.
  • For coherent sources initially in phase, path differences of nλ produce constructive interference.
  • For coherent sources initially in phase, path differences of (n + 1/2)λ produce destructive interference.
  • Nodal regions correspond to destructive interference.
  • Antinodal regions correspond to constructive interference.
  • Two coherent water-wave sources can produce a visible pattern of nodal and antinodal lines.
  • Sound interference can create loud and quiet regions.
  • Active noise cancellation uses destructive interference.
  • Light interference produces bright and dark fringes.
  • Young's double-slit experiment demonstrates the interference of light.
  • Thin-film interference produces colours in soap bubbles and oil films.
  • Anti-reflection coatings use destructive interference to reduce reflected light.
  • Interferometers use interference for extremely precise measurements.
  • Interference does not permanently destroy the original waves.
  • Destructive interference does not violate conservation of energy.
  • Diffraction and interference are closely connected wave phenomena.
  • Interference provides important evidence for the wave behaviour of light and other forms of radiation.

Check Your Understanding

  1. Explain how an interference pattern forms when two waves overlap.
  2. Distinguish between constructive and destructive interference.
  3. Two waves produce displacements of +4 cm and +3 cm at the same point. Calculate the resultant displacement and identify the type of interference.
  4. Two waves produce displacements of +5 cm and −5 cm. Calculate the resultant displacement and explain what has happened.
  5. What does it mean for two wave sources to be coherent?
  6. Why is a constant phase relationship important for producing a stable interference pattern?
  7. Define path difference.
  8. Two coherent, in-phase sources produce waves with λ = 0.50 m. At a point, the path difference is 1.0 m. Determine whether constructive or destructive interference occurs.
  9. The same sources produce waves with λ = 0.50 m. At another point, the path difference is 0.25 m. Determine the type of interference.
  10. Explain the difference between a nodal line and an antinodal line in a two-source water-wave pattern.
  11. Describe how two coherent loudspeakers can produce alternating loud and quiet regions in a room.
  12. Explain how active noise-cancelling headphones use destructive interference.
  13. Describe how Young's double-slit experiment produces alternating bright and dark fringes.
  14. Explain why complete destructive interference does not mean that wave energy has been destroyed.
  15. Two coherent water-wave sources are in phase and produce waves with λ = 0.60 m. Point P is 4.8 m from Source 1 and 3.6 m from Source 2, while Point Q is 4.5 m from Source 1 and 3.6 m from Source 2. Calculate the path difference at each point, determine whether each point experiences constructive or destructive interference, and explain how these different regions contribute to the overall interference pattern.
 
 
 

5. Applications of Wave Behavior

Learning outcomes
  • I can identify examples of reflection, refraction, diffraction, and interference.
  • I can explain how wave behavior is used in communication technologies.
  • I can describe wave behavior in musical instruments.
  • I can explain applications in medicine and engineering.
  • I can evaluate how understanding wave behavior improves modern technology.

Applications of Wave Behavior

Wave behaviour is not limited to laboratory demonstrations. The ways waves reflect, refract, diffract, and interfere are used in communication, medicine, engineering, music, transportation, astronomy, and many everyday technologies.

Engineers can control waves because their behaviour is predictable. By choosing appropriate:

  • wavelengths
  • frequencies
  • materials
  • shapes
  • boundaries
  • openings

they can design systems that transmit information, create images, reduce unwanted noise, detect hidden objects, and make precise measurements.

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The Four Major Wave Behaviours

Four important behaviours appear repeatedly in technological applications.

Reflection

A wave encounters a boundary and some or all of it returns.

Refraction

A wave enters a region where its speed changes and may change direction.

Diffraction

A wave spreads through an opening or around an obstacle.

Interference

Two or more waves overlap and combine through superposition.

Many technologies use more than one of these behaviours at the same time.


Comparing Wave Behaviours

Behaviour What Happens Common Example
Reflection Wave returns from boundary Echo
Refraction Speed changes and wave may bend Lens
Diffraction Wave spreads around edges/openings Sound around doorway
Interference Overlapping waves combine Noise cancellation

Recognizing these behaviours is an important first step in explaining wave technology.


Reflection in Everyday Life

Reflection occurs with many types of waves.

Examples include:

  • light reflecting from mirrors
  • sound reflecting from walls
  • water waves reflecting from harbour barriers
  • radio waves reflecting from objects
  • ultrasound reflecting from tissue boundaries
  • seismic waves reflecting from underground layers

In each case, information can sometimes be obtained by analyzing the reflected wave.


Echo Ranging

Reflection can be used to determine distance.

A wave is:

  1. transmitted
  2. reflected by an object
  3. detected when it returns

If the wave speed and travel time are known:

total distance travelled = speed × time

Because the wave travels to the object and back:

distance to object = speed × time / 2

This principle is used in:

  • sonar
  • medical ultrasound
  • echo sounding
  • some radar systems

Sonar

Sonar uses sound waves, usually in water, to detect objects or measure distances.

A sonar system sends out a sound pulse.

The pulse travels through water, reflects from an object, and returns as an echo.

The travel time allows the object's distance to be calculated.

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6

Worked Example: Sonar

A sonar pulse travels through seawater at:

v = 1500 m/s

The echo returns after:

t = 0.80 s

Total distance travelled:

d = vt

d = 1500 × 0.80

d = 1200 m

This is the distance down and back.

Depth:

1200/2 = 600 m

The water is approximately:

600 m deep


Sonar Applications

Sonar is used for:

  • measuring ocean depth
  • mapping the seafloor
  • locating underwater objects
  • navigation
  • fish finding
  • marine research
  • studying underwater geology

The technology works because sound travels effectively through water and can reflect from boundaries.


Radar

Radar uses electromagnetic waves rather than sound.

A transmitter sends electromagnetic waves toward a target.

Some of the radiation reflects back.

The returning signal can provide information about:

  • distance
  • position
  • motion
  • sometimes size or shape

Radar is used in:

  • aviation
  • weather monitoring
  • navigation
  • vehicle safety systems
  • speed measurement
  • satellite observations

Reflection is therefore important far beyond visible light and sound.


Refraction in Technology

Refraction allows waves to be redirected when their speed changes.

For light, refraction is fundamental to lenses.

Applications include:

  • eyeglasses
  • contact lenses
  • cameras
  • microscopes
  • telescopes
  • projectors
  • binoculars

By controlling the shape and material of a lens, engineers control how light is refracted.


Corrective Lenses

The eye must focus light accurately onto the retina.

If the optical system does not focus appropriately, corrective lenses can alter the path of incoming light.

Depending on the vision condition, optical correction may use:

  • converging lenses
  • diverging lenses
  • more complex lens shapes

The corrective lens refracts incoming light before it enters the eye, helping the eye form a clearer retinal image.


Cameras

A camera uses refraction through a lens system to focus light onto an image sensor.

Modern camera lenses may contain many individual lens elements.

These are designed to control:

  • focus
  • magnification
  • field of view
  • optical distortion
  • colour aberrations

Understanding refraction allows engineers to create increasingly compact and precise cameras.


Optical Fibres

Optical fibres transmit light through long, thin transparent fibres.

They rely strongly on total internal reflection, a phenomenon related to refraction and refractive index.

The fibre contains:

  • a core
  • surrounding cladding

The core has a higher refractive index than the cladding.

Under suitable conditions, light reaching the core-cladding boundary undergoes total internal reflection and remains guided along the fibre.

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6

Fibre-Optic Communication

Information can be encoded into pulses of light and transmitted through optical fibres.

Fibre-optic networks can carry:

  • internet data
  • telephone signals
  • television data
  • business communications

Advantages include:

  • very high data capacity
  • relatively low signal loss
  • immunity to many forms of electromagnetic interference
  • ability to carry signals over long distances

Wave physics therefore plays a major role in modern global communication.


Diffraction in Communication

Communication waves do not always travel only in straight lines.

Diffraction can allow waves to spread around obstacles.

The amount of diffraction depends strongly on wavelength relative to the obstacle.

In general:

longer wavelength relative to obstacle → greater diffraction

This can influence whether a signal reaches locations behind:

  • buildings
  • hills
  • walls
  • other structures

Radio Waves Around Obstacles

Some radio waves have wavelengths large enough to show significant diffraction around large obstacles.

This can allow signals to reach locations that are not directly visible from the transmitter.

However, the amount depends on:

  • wavelength
  • obstacle dimensions
  • terrain
  • transmitter and receiver positions

Communication engineers consider these effects when planning networks.


Why Frequency Matters in Communication

For electromagnetic waves:

v = fλ

In air, the speed is approximately constant.

Therefore:

higher frequency → shorter wavelength

lower frequency → longer wavelength

Because diffraction depends on wavelength, different communication frequencies can behave differently around the same obstacle.

This creates engineering trade-offs when selecting frequencies.


Reflection in Communication

Communication signals can also reflect.

Radio and microwave signals may reflect from:

  • buildings
  • the ground
  • terrain
  • other structures

These reflected waves may help a signal reach some locations.

However, they can also interfere with direct signals.

Therefore, reflection can be:

useful in one situation and problematic in another.


Multipath Interference

Suppose a wireless signal reaches a receiver by two paths.

One signal travels directly.

Another reflects from a building before reaching the receiver.

The two signals have travelled different distances.

They may therefore arrive with different phases.

When they overlap, they can undergo:

  • constructive interference
  • destructive interference

This is called multipath propagation and can cause signal strength to vary from one location to another.


Why Moving a Phone Can Change Signal Strength

Moving a receiver changes the distances travelled by different signal paths.

This changes their:

path difference

A location experiencing destructive interference may become a location of constructive interference after a relatively small movement.

This helps explain why wireless signal strength can sometimes change even when the transmitter remains in the same place.

Modern communication systems use sophisticated techniques to reduce or even exploit multipath effects.


Diffraction Gratings in Communication and Science

A diffraction grating contains many closely spaced lines or openings.

Incoming light diffracts from these structures.

The resulting waves interfere, causing different wavelengths to emerge strongly in different directions.

Diffraction gratings are used in:

  • spectrometers
  • telecommunications
  • astronomy
  • chemical analysis
  • optical laboratories

They allow wavelengths to be measured and separated precisely.


Wave Behaviour in Musical Instruments

Musical instruments depend heavily on:

  • reflection
  • interference
  • resonance
  • standing waves

Different instruments control waves in different ways.

Examples include:

  • strings in guitars and violins
  • air columns in flutes and organs
  • membranes in drums
  • air columns and vibrating reeds in clarinets and saxophones
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8

Waves on Strings

When a guitar string is plucked, transverse waves travel along the string.

When the waves reach the fixed ends, they reflect.

The incident and reflected waves overlap.

Their interference can create a:

standing wave

Standing waves contain:

  • nodes
  • antinodes

The allowed standing-wave patterns determine the frequencies produced by the string.


Fundamental Frequency

The lowest natural frequency of a vibrating system is called the:

fundamental frequency

For a string fixed at both ends, the simplest standing-wave pattern contains:

  • a node at each end
  • one antinode in the middle

The string length corresponds to half a wavelength:

L = λ/2

Therefore:

λ = 2L

The fundamental frequency can then be determined using:

v = fλ


Worked Example: Vibrating String

A string is:

L = 0.75 m

For its fundamental mode:

λ = 2L

λ = 2 × 0.75

λ = 1.50 m

Suppose waves travel along the string at:

v = 300 m/s

Then:

f = v/λ

f = 300/1.50

f = 200 Hz

The fundamental frequency is:

200 Hz


Changing the Pitch of a String

The frequency produced by a string depends on factors including:

  • string length
  • tension
  • mass per unit length

For example, shortening the vibrating portion of a guitar string generally increases its fundamental frequency.

The pitch rises.

This is why pressing a guitar string against different frets changes the note.


Air Columns

Wind instruments use standing waves in columns of air.

Sound waves travel through the air column and reflect from boundaries.

The incident and reflected waves interfere.

At particular frequencies, stable standing-wave patterns form.

This produces:

resonance

Examples include:

  • flutes
  • clarinets
  • trumpets
  • organ pipes

Resonance

Resonance occurs when a system is driven near one of its natural frequencies and responds with a relatively large amplitude.

Musical instruments are designed to encourage useful resonances.

Resonance helps:

  • strengthen certain frequencies
  • produce characteristic tones
  • increase sound output

The shape and dimensions of the instrument determine which resonant frequencies are supported.


Harmonics

Musical instruments usually produce more than one frequency.

Higher natural frequencies related to the fundamental are called:

harmonics

The combination of fundamental and higher-frequency components contributes to an instrument's:

timbre

or characteristic sound quality.

This helps explain why a violin and flute can play the same musical note but still sound different.


Sound Reflection in Concert Halls

Concert halls are designed using wave physics.

Sound reflects from:

  • walls
  • ceilings
  • floors
  • acoustic panels

Some reflection is useful because it distributes sound throughout the hall.

Too much reflection can cause excessive:

reverberation

Too much absorption can make a space sound acoustically "dead."

Engineers therefore balance:

  • reflection
  • absorption
  • diffusion of sound
  • room geometry

Diffraction in Musical Environments

Sound can diffract around:

  • seats
  • people
  • pillars
  • stage structures
  • doorways

Longer-wavelength sounds tend to diffract more strongly around these obstacles.

This helps distribute low-frequency sound throughout a performance space.

Acoustic engineers must consider both reflection and diffraction when designing venues.


Interference and Music

Sound waves from multiple sources can interfere.

For example, two loudspeakers producing the same frequency may create regions where sound is:

  • stronger
  • weaker

Poor speaker placement can therefore produce uneven sound coverage.

Audio engineers carefully position and control speaker systems to reduce unwanted interference.


Beats

When two sound waves with slightly different frequencies overlap, their interference changes over time.

The sound alternates between stronger and weaker intensity.

This effect is called:

beats

The beat frequency is:

f_beat = |f₁ − f₂|

Musicians can use beats when tuning instruments.


Worked Example: Beats

Two notes have frequencies:

f₁ = 440 Hz

f₂ = 444 Hz

Then:

f_beat = |440 − 444|

f_beat = 4 Hz

The listener hears approximately four changes in loudness each second.

As the instrument approaches correct tuning, the beat frequency becomes smaller.


Wave Behaviour in Medicine

Medicine uses waves for:

  • imaging
  • diagnosis
  • monitoring
  • treatment

Important technologies include:

  • ultrasound imaging
  • Doppler ultrasound
  • endoscopy
  • medical lasers
  • optical imaging

Different technologies use different wave behaviours.


Medical Ultrasound

Medical ultrasound sends high-frequency sound waves into the body.

When ultrasound reaches boundaries between tissues with different acoustic properties, some of the wave is reflected.

The returning echoes are detected by a transducer.

A computer uses information about:

  • echo time
  • echo strength
  • direction

to construct an image.

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8

Why Ultrasound Gel Is Used

Air between an ultrasound transducer and the skin would strongly interfere with efficient transmission of ultrasound into the body.

Ultrasound gel helps remove air gaps and improves the transfer of sound between:

transducer → body

This allows stronger useful echoes to be detected.


Doppler Ultrasound

Doppler ultrasound uses changes in the frequency of reflected sound to investigate motion.

It can be used to study:

  • blood flow
  • movement of heart structures
  • direction of flowing blood
  • relative flow speed

This is an application of the Doppler effect, another important wave phenomenon.


Medical Endoscopes

Endoscopes allow doctors to view inside the body.

Modern systems may use:

  • optical fibres
  • lenses
  • light sources
  • miniature cameras

Optical fibres can guide light through flexible pathways using total internal reflection.

This allows imaging of locations that would otherwise be difficult to observe directly.


Wave Behaviour in Engineering

Engineers use waves to:

  • inspect structures
  • measure distances
  • detect faults
  • communicate
  • reduce noise
  • study materials
  • monitor machines
  • design safer buildings

Wave behaviour often allows measurements to be made without damaging the object being tested.


Ultrasonic Testing

Ultrasonic testing is a form of non-destructive testing.

High-frequency sound waves are sent into a material.

If the wave encounters:

  • a crack
  • void
  • boundary
  • defect

some ultrasound reflects.

The returning echo can reveal the location of the defect.

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7

Worked Example: Finding a Crack

An ultrasonic pulse travels through steel at:

v = 5900 m/s

An echo from a crack returns after:

t = 0.000020 s

Total travel distance:

d = vt

d = 5900 × 0.000020

d = 0.118 m

The wave travelled to the crack and back.

Depth:

0.118/2 = 0.059 m

or:

5.9 cm

The crack is approximately 5.9 cm below the surface.


Why Non-Destructive Testing Matters

Engineers may need to inspect:

  • aircraft components
  • bridges
  • pipelines
  • railway tracks
  • pressure vessels
  • machinery

Taking these objects apart may be expensive or impossible.

Wave-based testing can detect hidden problems without destroying the component.

This can improve:

  • safety
  • reliability
  • maintenance
  • cost efficiency

Seismic Waves and Engineering

Buildings experience waves during earthquakes.

Engineers study:

  • seismic-wave frequencies
  • resonance
  • ground motion
  • structural vibration
  • damping

A building can respond strongly if earthquake motion contains frequencies near the building's natural frequencies.

Engineering designs can therefore include features that reduce dangerous oscillations.


Damping

Damping removes energy from an oscillating system.

Engineering structures may include damping systems to reduce unwanted vibrations.

Examples include:

  • shock absorbers
  • vibration isolators
  • tuned mass dampers
  • energy-dissipating structural components

Understanding waves and oscillations allows engineers to control the response of structures.


Noise-Cancelling Technology

Active noise cancellation uses:

destructive interference

A microphone detects unwanted sound.

A second sound wave is generated so that its pressure variation opposes the unwanted sound near the listener.

When the waves overlap:

destructive interference reduces the unwanted sound

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6

Anti-Reflection Coatings

Reflection can be useful, but sometimes engineers want to reduce it.

Thin coatings can be placed on optical surfaces so that reflected light waves interfere destructively.

These anti-reflection coatings are used on:

  • eyeglasses
  • camera lenses
  • microscopes
  • telescopes
  • optical sensors
  • solar cells

Reducing reflection allows more light to pass through the surface.

This technology combines:

reflection + interference


Interferometry

Interferometry uses interference to make extremely precise measurements.

A wave can be divided into different paths and then recombined.

A tiny change in one path changes the interference pattern.

Interferometers can measure extremely small changes in:

  • distance
  • position
  • surface shape
  • refractive index

Interference therefore turns tiny physical changes into measurable patterns.


Diffraction and Optical Instruments

Diffraction is not always helpful.

It places a fundamental limit on the resolution of optical instruments.

Light passing through a finite aperture spreads slightly because of diffraction.

As a result, a point object does not produce an infinitely small image point.

This affects:

  • microscopes
  • telescopes
  • cameras

Engineers must account for diffraction when designing high-resolution instruments.


Telescope Resolution

A larger telescope aperture generally allows finer detail to be resolved at a given wavelength.

A simplified diffraction relationship is:

smaller wavelength + larger aperture → better potential resolution

This is one reason astronomical telescopes often have very large mirrors.

Large apertures also collect more light.


Microscopes and Resolution

Ordinary optical microscopes are also limited by diffraction.

If two structures are too close together compared with the wavelength of light and the capabilities of the optical system, they cannot be clearly distinguished.

Simply increasing magnification will not necessarily reveal additional detail.

This is why:

magnification and resolution are different.


Wave Behaviour in Transportation

Modern transportation uses wave technologies extensively.

Examples include:

  • radar in aircraft
  • sonar in ships
  • ultrasonic parking sensors
  • automotive radar
  • optical cameras
  • wireless navigation and communication

These systems may use reflection, refraction, diffraction, and interference to detect objects and transmit information.


Wave Behaviour in Astronomy

Astronomers use wave behaviour to study the universe.

Telescopes use:

  • reflection
  • refraction
  • diffraction
  • interference

Reflecting telescopes use mirrors.

Refracting telescopes use lenses.

Diffraction affects telescope resolution.

Interferometers combine signals from multiple telescopes to obtain information equivalent to observations made across a much larger effective separation.


Radio Telescope Interferometry

Several radio telescopes can observe the same astronomical source.

Their signals can be combined using interference principles.

Precise differences in arrival times and phases provide information about the source.

This technique can produce extremely detailed astronomical observations.

It demonstrates how interference can be used as a measurement tool rather than merely being treated as an unwanted effect.


Wave Behaviour in Coastal Engineering

Engineers designing harbours and coastlines must consider:

reflection

Waves can reflect from seawalls and harbour structures.

refraction

Waves change speed and direction as water depth changes.

diffraction

Waves spread through harbour entrances and around breakwaters.

interference

Overlapping waves can create regions of increased or reduced wave amplitude.

Understanding all four behaviours helps engineers design safer coastal structures.

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6

When Wave Behaviour Is Helpful

Wave behaviour can be deliberately used.

Examples include:

  • reflection for sonar
  • refraction for lenses
  • diffraction for spectroscopy
  • interference for noise cancellation
  • total internal reflection for fibre optics
  • standing waves for musical instruments

In these situations, engineers design systems to encourage a particular behaviour.


When Wave Behaviour Causes Problems

The same behaviours can also create problems.

Examples include:

  • reflections producing echoes
  • radio reflections producing multipath interference
  • diffraction limiting optical resolution
  • interference producing weak communication signals
  • resonance causing excessive vibration
  • unwanted sound reflections creating poor room acoustics

Engineering often involves controlling wave behaviour rather than simply producing it.


Designing Better Technology

Understanding waves allows designers to ask questions such as:

  • Which frequency should be used?
  • What wavelength will result?
  • How will the wave interact with obstacles?
  • Will reflections improve or weaken the signal?
  • Will diffraction help the wave reach the receiver?
  • Could destructive interference occur?
  • Which material will refract the wave appropriately?
  • How can unwanted vibration be reduced?
  • What aperture will provide the required resolution?

Wave physics therefore allows technology to be designed systematically rather than through trial and error alone.


Evaluating Communication Technology

Consider a wireless communication system.

Using a shorter wavelength may allow:

  • smaller antennas
  • high data capacity
  • highly directional beams

But shorter wavelengths may also show less diffraction around large obstacles.

Longer wavelengths may:

  • diffract more strongly
  • reach some obstructed regions more effectively

but may require different antenna designs and have different available bandwidths.

There is rarely one "best" wavelength for every application.

Engineers select frequencies based on the requirements of the system.


Evaluating Medical Technology

Ultrasound demonstrates similar trade-offs.

Higher-frequency ultrasound generally provides:

  • shorter wavelengths
  • potentially finer spatial detail

but it is generally attenuated more strongly in tissue, reducing useful penetration depth.

Lower-frequency ultrasound can penetrate more deeply but may provide lower spatial resolution.

Therefore, medical imaging requires a balance between:

resolution and penetration

Understanding wave behaviour makes this choice possible.


Evaluating Optical Technology

Optical systems also involve trade-offs.

A telescope designer may want:

  • high resolution
  • strong light gathering
  • low optical distortion
  • low mass
  • reasonable cost

A larger aperture can improve light collection and diffraction-limited resolution, but it can also make the instrument larger, heavier, and more expensive.

Engineering therefore involves using wave physics while balancing practical constraints.


How Wave Science Improves Technology

Understanding wave behaviour has allowed scientists and engineers to:

  • transmit enormous amounts of digital information
  • image structures inside the human body
  • locate underwater objects
  • detect internal cracks in metals
  • reduce unwanted noise
  • build high-resolution microscopes
  • observe extremely distant astronomical objects
  • design safer buildings
  • improve concert halls
  • measure extremely small distances
  • develop advanced sensors
  • improve navigation systems

These technologies depend on the predictable behaviour of waves.


One Technology Can Use Several Wave Behaviours

Real technologies rarely fit into only one category.

Consider a telescope.

It may involve:

  • reflection from mirrors
  • refraction through lenses
  • diffraction at the aperture
  • interference in optical coatings

Similarly, a communication system may involve:

  • reflection from buildings
  • refraction through the atmosphere
  • diffraction around obstacles
  • interference between multiple signal paths

Understanding the complete system requires considering several wave behaviours together.


A Complete Communication Example

Suppose a radio transmitter sends a signal through a city.

The signal travels toward a receiver.

Along the way:

Reflection

Some waves reflect from buildings.

Diffraction

Some waves spread around building edges.

Refraction

Atmospheric conditions may slightly alter propagation.

Interference

Direct and reflected signals overlap at the receiver.

Engineers design communication systems to operate reliably despite these effects.

Modern technology can sometimes use the effects rather than simply trying to eliminate them.


A Complete Medical Example

Consider an ultrasound scan.

A transducer sends sound waves into the body.

The waves travel through tissue.

At boundaries between different tissues:

some ultrasound reflects

The echoes return to the transducer.

The time taken provides information about:

depth

The strength of the reflection provides information about:

tissue boundaries

A computer processes thousands of returning signals to construct an image.

This turns the reflection of waves into a non-invasive medical imaging technique.


A Complete Engineering Example

An engineer inspects a metal component using ultrasound.

A pulse enters the metal.

Most of the wave travels through the material.

When it reaches an internal crack:

some wave energy reflects

The echo returns to the detector.

The travel time determines the crack's depth.

The echo characteristics provide additional information about the defect.

The component can therefore be inspected without cutting it open.


A Complete Musical Example

A guitar string is plucked.

A disturbance travels along the string.

At the fixed ends:

waves reflect

Incident and reflected waves:

interfere

At suitable frequencies:

standing waves form

The string:

resonates

The resulting vibration causes surrounding air to vibrate and produces sound.

Several wave behaviours therefore work together to create a musical note.


Evaluating Wave Technology

When evaluating a technology based on waves, consider:

Purpose

What problem is the technology solving?

Wave type

What type of wave is being used?

Wave behaviour

Is reflection, refraction, diffraction, interference, or a combination involved?

Benefit

How does this behaviour improve the technology?

Limitation

What problems does the wave behaviour create?

Design response

How do engineers reduce the limitation or exploit the behaviour?

This produces a stronger evaluation than simply naming the wave phenomenon.


A Reliable Strategy for Application Questions

When given an unfamiliar wave application:

  1. Identify the wave involved.
  2. Identify its source.
  3. Determine how the wave travels.
  4. Identify any boundaries.
  5. Look for waves returning from boundaries — reflection.
  6. Look for speed and direction changes — refraction.
  7. Look for spreading around edges or through openings — diffraction.
  8. Look for overlapping waves — interference.
  9. Identify what information or energy the wave carries.
  10. Explain how the behaviour helps the technology operate.
  11. Identify any limitations caused by the wave behaviour.
  12. Explain how the design controls those limitations.
  13. Evaluate whether the chosen wave is appropriate for the application.

Common Mistakes

Thinking each technology uses only one wave behaviour

Many technologies involve several wave phenomena simultaneously.

Confusing reflection and refraction

Reflection sends a wave back. Refraction involves a speed change as a wave enters a different region.

Confusing diffraction and refraction

Diffraction involves spreading around edges or through openings. Refraction results from changing wave speed.

Thinking interference is always undesirable

Interference can be deliberately used in noise cancellation, optical coatings, and measurement.

Thinking reflection is always useful

Unwanted reflections can produce echoes, glare, or communication problems.

Thinking longer wavelengths are always better for communication

Longer wavelengths may diffract more strongly, but communication design involves many other factors.

Thinking higher magnification always means a better microscope or telescope

Resolution is also essential.

Forgetting to divide echo distance by two

Echo-ranging waves travel to the object and back.

Thinking optical fibres simply reflect light from ordinary mirrors

They guide light using total internal reflection at the core-cladding boundary under suitable conditions.

Thinking ultrasound is electromagnetic radiation

Ultrasound is a mechanical sound wave.

Thinking standing waves are separate from interference

Standing waves result from interference between waves travelling in opposite directions.

Thinking technology eliminates all unwanted wave behaviour

Engineering usually involves controlling, reducing, or exploiting wave effects rather than eliminating them completely.


Key Terms

Reflection — return of a wave from a boundary.

Refraction — change in wave speed and often direction when entering a different region.

Diffraction — spreading of waves through openings or around obstacles.

Interference — combination of overlapping waves through superposition.

Echo — reflected sound wave detected after the original sound.

Sonar — technology using sound waves to detect or locate underwater objects.

Radar — technology using electromagnetic waves to detect and locate objects.

Total internal reflection — complete reflection of a wave such as light at a boundary under appropriate conditions.

Optical fibre — thin transparent structure designed to guide light.

Multipath propagation — arrival of a signal by several different paths.

Standing wave — stationary wave pattern produced by interference between suitable waves travelling in opposite directions.

Node — location of minimum or zero displacement in an ideal standing wave.

Antinode — location of maximum oscillation in a standing wave.

Fundamental frequency — lowest natural frequency of an oscillating system.

Harmonic — natural frequency related to the fundamental.

Resonance — large response produced when a system is driven near a natural frequency.

Timbre — characteristic sound quality influenced by the combination of frequencies present.

Beat — periodic variation in amplitude produced by waves with slightly different frequencies.

Ultrasound — sound with frequency above the normal human hearing range.

Non-destructive testing — examination of a material or structure without significantly damaging it.

Damping — reduction of oscillation through energy dissipation.

Interferometry — precise measurement technique based on wave interference.

Resolution — ability to distinguish nearby details as separate.

Diffraction grating — structure containing many closely spaced lines or openings used to diffract and separate wavelengths.

Anti-reflection coating — thin optical coating designed to reduce reflected light using interference.


Key Takeaways

  • Reflection, refraction, diffraction, and interference occur throughout modern technology.
  • Reflection allows waves to return information about distant or hidden objects.
  • Sonar and ultrasound use reflected sound waves.
  • Radar uses reflected electromagnetic waves.
  • Refraction allows lenses to control and focus light.
  • Cameras, microscopes, telescopes, and corrective lenses depend on refraction.
  • Optical fibres guide light and are fundamental to modern communication networks.
  • Diffraction allows waves to spread through openings and around obstacles.
  • Longer wavelengths generally diffract more strongly around a given obstacle.
  • Diffraction influences communication coverage and optical resolution.
  • Interference occurs when waves overlap.
  • Interference may strengthen or weaken communication signals.
  • Active noise cancellation deliberately uses destructive interference.
  • Anti-reflection coatings use interference to reduce unwanted reflections.
  • Musical instruments use reflection, interference, standing waves, resonance, and harmonics.
  • Beats can help musicians tune instruments.
  • Medical ultrasound uses reflection to image structures inside the body.
  • Doppler ultrasound uses wave-frequency changes to investigate motion such as blood flow.
  • Ultrasonic testing can locate internal defects without damaging a structure.
  • Engineers study seismic waves, resonance, and damping when designing structures.
  • Diffraction places a fundamental limit on the resolution of microscopes, telescopes, and cameras.
  • Interferometry allows extremely precise measurements.
  • Real technologies commonly involve several wave behaviours simultaneously.
  • Wave behaviour can be useful or problematic depending on the application.
  • Understanding waves allows engineers to predict these effects and design technology around them.
  • Modern communication, medicine, engineering, music, astronomy, and transportation all depend heavily on wave physics.

Check Your Understanding

  1. Give one real-world example each of reflection, refraction, diffraction, and interference.
  2. Explain how sonar uses wave reflection to determine the distance to an underwater object.
  3. A sonar echo returns after 1.2 s. If sound travels through the water at 1500 m/s, calculate the distance to the reflecting object.
  4. Explain how refraction is used in a camera or corrective lens.
  5. Describe how optical fibres allow information to be transmitted over long distances.
  6. Explain why wavelength is important when considering whether a communication signal will diffract around an obstacle.
  7. A wireless signal reaches a receiver directly and after reflecting from a building. Explain how interference between the two signals could cause the received signal strength to change.
  8. Explain how reflection and interference combine to produce standing waves on a guitar string.
  9. A 0.60 m string supports a fundamental standing wave. Calculate the wavelength of the fundamental mode. If the wave speed is 240 m/s, calculate its fundamental frequency.
  10. Two musical notes have frequencies of 440 Hz and 443 Hz. Calculate their beat frequency and explain how beats can be useful when tuning instruments.
  11. Explain how medical ultrasound uses reflection to form images of structures inside the body.
  12. An ultrasonic pulse travels through a material at 5000 m/s and returns from a defect after 0.000040 s. Calculate the depth of the defect.
  13. Explain how destructive interference is used in either noise-cancelling headphones or anti-reflection coatings.
  14. Choose one technology and identify at least two different wave behaviours involved in its operation. Explain the role of each.
  15. Evaluate the statement: "Understanding wave behaviour is important because engineers can use useful wave effects while reducing unwanted ones." Support your answer with examples from communication, medicine, music, or engineering.