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    AQA AS Specification

    Lessons Topics

    1 & 2 Progressive Waves

    Oscillation of the particles of the medium; amplitude, frequency, wavelength,

    speed, phase, (path differencecovered in optics section).

    c = f

    3 & 4 Longitudinal and transverse wavesCharacteristics and examples, including sound and electromagnetic waves.

    Polarisation as evidence for the nature of transverse waves; applications e.g.

    Polaroid sunglasses, aerial alignment for transmitter and receiver.

    5 to 8 Superposition of waves, stationary waves

    The formation of stationary waves by two waves of the same frequency

    travelling in opposite directions; no mathematical treatment required.Simple graphical representation of stationary waves, nodes and antinodes on

    strings.

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    Waves

    A wave is a means of transferring energy

    and momentum from one point to

    another without there being any transfer

    of matter between the two points.

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    Describing Waves

    1. Mechanical or Electromagnetic

    Mechanical waves are made up of particles vibrating.

    e.g. sound air molecules; water water mo lecules

    All these waves require a substance for transmission

    and so none of them can travel through a vacuum.

    Electromagneticwaves are made up of oscillatingelectric and magnetic fields.

    e.g. l ight and radio

    These waves do not require a substance fortransmission and so all of them can travel through avacuum.

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    Describing Waves

    2. Progressive or Stationary

    Progressivewaves are waves where there is a nettransfer of energy and momentum from one point toanother.

    e.g. sound produced by a person speaking; l igh t from alamp

    Stationarywaves are waves where there is a NO nettransfer of energy and momentum from one point to

    another.e.g. the wave on a gu itar str ing

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    Describing Waves

    3. Longitudinal or Transverse

    Longitudinalwaves are waves

    where the direction of vibration of

    the particles is parallel to thedirection in which the wave

    travels.

    e.g. sound

    wave direction

    vibrations

    LONGITUDINAL WAVE

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    Describing Waves

    Transversewaves are waveswhere the direction of vibration of

    the particles or fields is

    perpendicular to the direction in

    which the wave travels.

    e.g. water and all electrom agnetic

    waves

    Test fo r a transverse wave:Only TRANVERSE waves undergo

    polarisation.

    wave direction

    vibrations

    TRANSVERSE WAVE

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    Polarisation

    The oscillations within a transverse wave and the

    direction of travel of the wave define a plane. If the

    wave only occupies one plane the wave is said to

    be plane polarised.

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    Polarisation

    Light from a lamp is unpolarised. However,

    with a polarising filter it can be plane

    polarised.

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    Polarisation

    If two crossed filters are used then no light

    will be transmitted.

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    Aerial alignment

    Radio waves (and microwaves) aretransmitted as plane polarised waves.In the case of satellite television, twoseparate channels can be transmittedon the same frequency but withhorizontal and vertical planes ofpolarisation.

    In order to receive thesetransmissions the aerial has to bealigned with the plane occupied by theelectric field component of theelectromagnetic wave.

    The picture shows an aerial aligned toreceive horizontally polarised waves.

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    Measuring waves

    Displacement,x

    This is the distance of an oscillating particle from its undisturbedor equilibrium position.

    Amplitude, a

    This is the maximum displacement of an oscillating particle from

    its equilibrium position. It is equal to the height of a peak or thedepth of a trough.

    amplitude a

    undisturbed

    or equilibrium

    position

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    Measuring waves

    Phase, This is the point that a particle is at within anoscillation.

    Examples: top of peak, bottom of trough

    Phase is sometimes expressed in terms of anangle up to 360. If the top of a peak is 0then

    the bottom of a trough will be 180.

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    Measuring waves

    Phase difference,This is the fraction of a cycle between two particleswithin one or two waves.

    Examp le: the top of a peak has a phase dif ference ofhal f of one cycle compared w ith the bo ttom of a

    trough.

    Phase difference is often expressed as an angledifference. So in the above case the phase difference is180. Also with phase difference, angles are usually

    measured in radians.Where: 360= 2 radian; 180= rad; 90= /2 rad

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    Measuring waves

    Wavelength,This is the distance between two consecutiveparticles at the same phase.

    Example: top-of-a-peak to the next top -of -a-peak

    unitmetre, m

    wavelength

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    Measuring wavesPeriod, T

    This is equal to the time taken for one complete

    oscillation in of a particle in a wave.

    unitsecond, s

    Frequency, f

    This is equal to the number of complete oscillations in

    one second performed by a particle in a wave.

    unithertz, HzNOTE: f = 1 / T

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    The wave equation

    For all waves:

    speed = frequency x wavelength

    c = f

    where speed is in ms

    -1

    provided frequency is in hertzand wavelength in metres

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    Complete

    Wave speed Frequency Wavelength Period

    600 m s-1 100 Hz 6 m 0.01 s

    10 m s-1 2 kHz 0.5 cm 0.5 ms

    340 ms-1 170 Hz 2 m 5.88 ms

    3 x 108ms-1 200 kHz 1500 m 5 x 10-6s

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    Answers

    Wave speed Frequency Wavelength Period

    600 m s-1 100 Hz 6 m 0.01 s

    10 m s-1 2 kHz 0.5 cm 0.5 ms

    340 ms-1 170 Hz 2 m 5.88 ms

    3 x 108ms-1 200 kHz 1500 m 5 x 10-6s

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    Superposition of waves

    This is the process thatoccurs when two waves ofthe same type meet.

    The principle ofsuperposition

    When two waves meet,the total displacement at apoint is equal to the sum

    of the individualdisplacements at thatpoint

    reinforcement

    cancellation

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    Stationary waves

    A stationary wave can be formed by thesuperposition of two progressive waves

    of the same frequency travelling in

    opposite directions.

    This is usually achieved by superposing

    a reflected wave with its incident wave.

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    Formation of a stationary wave

    Consider two waves, Aand B, each ofamplitude a, frequency fand period Ttravelling

    in opposite directions.

    (1) At time, t = 0

    Wave B Amplitude = 2a

    Wave A

    RESULTANT WAVEFORM

    REINFORCEMENT

    N A N A N A N A N A N A N

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    (2) One quarter of a cycle later, at time, t = T/4both waves have moved by a quarter of a

    wavelength in opposite directions.

    Wave B

    Wave A

    RESULTANT WAVEFORM

    CANCELLATION

    Amplitude = 0

    N A N A N A N A N A N A

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    (3) After another quarter of a cycle, at time,t = T/2both waves have now moved by a

    half of a wavelength in opposite directions.

    Wave B

    Wave A

    Amplitude = 2a

    RESULTANT WAVEFORM

    REINFORCEMENT

    N A N A N A N A N A N A N

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    (4) One quarter of acycle later, at time,t = 3T/4both waves will

    undergo cancellationagain.

    (5) One quarter of acycle later, at time, t = Tthe two waves willundergo superpositionin the same way as attime, t = 0

    N A N A N A N A N A N

    (6) Placing all fourresultant waveforms on topof each other gives:

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    Nodes (N) and Antinodes (A)

    NODES are points within a stationary wave thathave the MINIMUM (usually zero) amplitude.

    These have been marked by an N in the

    prev ious waveforms.

    ANTINODESare points within a stationary

    wave that have the MAXIMUM amplitude.

    These have been marked by an A in the

    previous waveforms and have an ampl i tude

    equal to 2a

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    Comparison of stationary and progressive waves

    Property Stationary Wave Progressive Wave

    Energy &Momentum No net transfer from one pointto another Both move with speed:c = f x

    Amplitude Varies from zero at NODES to a

    maximum at ANTINODES

    Is the same for all particles

    within a wave

    Frequency All particles oscillate at the

    same frequency except those at

    nodes

    All particles oscillate at the

    same frequency

    Wavelength This is equal to TWICE the

    distance between adjacent

    nodes

    This is equal to the distance

    between particles at the

    same phase

    Phase

    differencebetween two

    particles

    Between nodes all particles are

    at the same phase. Any othertwo particles have phase

    difference equal to m where

    m is the number of nodes

    between the particles

    Any two particles have

    phase difference equal to2d / where d is the

    distance between the two

    particles

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    Examination question

    The diagram below shows a microphone being used todetect the nodes of the stationary sound wave formedbetween the loudspeaker and reflecting surface. Thesound wave has a frequency of 2.2 kHz.

    to

    oscilloscope

    microphonereflecting

    surface

    loudspeaker

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    (a) Explain how a stationary is formed between theloudspeaker and reflecting surface. [3]

    (b) When the microphone is moved left to right by 45 cm

    it covers six inter-nodal distances. Calculate thewavelength and speed of the progressive sound wavesbeing used to form the stationary wave. [4]

    (c) The nodes nearest to the reflecting surface havenearer zero amplitude compared with those nearer the

    loudspeaker. Why? [3]

    to

    oscilloscope

    microphonereflecting

    surface

    loudspeaker

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    (a)

    The reflected sound wave undergoes

    superposition with the incident sound waveproduced by the loudspeaker. [1 mark]

    Nodes are formed when the peak of one wave

    superposes with the trough of the other,cancellation occurs. [1 mark]

    Antinodes are formed when the peak of one

    wave superposes with the peak of the other,reinforcement occurs. [1 mark]

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    (b)

    Wavelength equals twice the distance between

    nodes.Internodal distance = 45 cm / 6 = 7.5 cm

    Therefore sound wavelength = 15 cm [2 marks]

    c = f x

    = 2.2 kHz x 15 cm

    = 2 200 Hz x 0.15 m

    speed of sound waves = 330 ms-1 [2 marks]

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    (c)

    The amplitude of a sound wavedecreases with distance due to its energyspreading out. [1 mark]

    The size of a peak just before reflectionand that of a trough just after reflectionwill be similar and so almost perfectcancellation will occur and theconsequent node produced will have anear zero amplitude. [1 mark]

    The size of a peak just after productionby the loudspeaker will, however, bemuch larger than that of a trough afterreflection and travel back to the speaker.Therefore incomplete cancellation willoccur and the consequent node producedwill still have a significant amplitude.

    [1 mark]

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    Stationary waves on strings

    Fundamental mode, foThis is the lowest frequency that can produce astationary wave.

    The length of the loop, L is equal to half of a wavelength.

    and so: = 2L

    also: fo= c / = c / 2L

    L= length of a loop

    node nodeantinode

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    First Overtone, 2foThis is the second lowest frequency that can produce a

    stationary wave.The length of two loops, L is equal to one wavelength.

    and so: = L

    also: 2 fo= c / L

    L= length of two loops =

    N A N A N

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    QuestionA string of length 60 cm has fundamental frequency of20 Hz. Calculate:(a) the wavelength of the fundamental mode

    (b) the speed of the progressive waves making up thestationary wave

    (c) the number of loops formed if with the same stringthe length of the string was increased to 1.2m and thefrequency to 30Hz

    (a) In the fundamental mode there is one loop of length

    equal to .Therefore wavelength = 2 x 60 cm

    = 1.2 m

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    (b) c = f x

    = 20 Hz x 1.2 m

    Speed of the progressive waves = 24 ms-1

    (c) If the frequency is increased to 30Hz the wavelengthwill now be given by:

    = c / f

    = 24 / 30= 0.8 m

    but each loop length =

    = 0.4 m

    there will therefore be: 1.2 / 0.4 loops

    Number of loops = 3

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    Internet Links Wave lab- shows simple transverse & longitudinal

    waves with reflection causing a stationary wave - by

    eChalk Wave Effects- PhET - Make waves with a dripping

    faucet, audio speaker, or laser! Add a second source

    or a pair of slits to create an interference pattern. Also

    shows diffraction.

    Virtual Ripple Tank- falstad

    Fifty-Fifty Game on Wave Types - by KT - Microsoft

    WORD

    Simple transverse wave- netfirms Simple longitudinal wave- netfirms

    Simple wave comparision- amplitude, wavelength -

    7stones

    Fifty-Fifty Game on Wave Types - by KT - Microsoft

    WORD

    Wave on a String- PhET - Watch a string vibrate in

    slow motion. Wiggle the end of the string and make

    waves, or adjust the frequency and amplitude of anoscillator. Adjust the damping and tension. The end

    can be fixed, loose, or open.

    Vend diagram quiz comparing light and sound waves-

    eChalk

    Superposition of two pulses- NTNU

    Superpositon of two oppositely movingprogressive waves- NTNU

    Superposition of two pulses or waves-

    7stones

    Fourier - Making Waves-PhET - Learn how to

    make waves of all different shapes by adding up

    sines or cosines. Make waves in space and time

    and measure their wavelengths and periods. See

    how changing the amplitudes of different harmonicschanges the waves. Compare different

    mathematical expressions for your waves.

    Beats - Sound Pulses- Explore Science

    Beats- netfirms

    Beats- Fendt

    Resonance in a string- netfirms

    Stationary wave modes of vibration- netfirms

    Standing Longitudinal Wave- Fendt

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    Core Notes from Breithaupt pages 174 to 1851. Draw diagrams and explain what is

    meant by (a) transverse and (b)

    longitudinal waves. Give twoexamples of each type.

    2. (a) What is meant by polarisation? (b)What is the difference between planepolarised and unpolarised light? (c)How can unpolarised light be changedinto plane polarised light? (d) Whattype of waves can display polarisationeffects?

    3. What is a stationary wave? How is itdifferent from a progressive wave?(see page 180)

    4. Define in the context of wave motion:(a) amplitude; (b) frequency; (c)wavelength; & (d) phase. You may

    wish to illustrate your answers withdiagrams.

    5. Give the equation for wave speed interms of other wave quantities.

    6. What is the principle of superposition? Explain,using diagrams, how the processes ofreinforcement and cancellation can occur (p180).

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    Notes on Describing Waves & Polarisation

    from Breithaupt pages 174, 175 & 180

    1. Draw diagrams and explain what is meant by (a)transverse and (b) longitudinal waves. Give twoexamples of each type.

    2. (a) What is meant by polarisation? (b) What is thedifference between plane polarised and unpolarised

    light? (c) How can unpolarised light be changed intoplane polarised light? (d) What type of waves candisplay polarisation effects?

    3. What is a stationary wave? How is it different from aprogressive wave? (see page 180)

    4. What are (a) mechanical & (b) electromagnetic waves.In what ways are they different?

    5. Try the Summary Questions on page 175.

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    Notes on Measuring Waves

    from Breithaupt pages 176 & 177

    1. Define in the context of wave motion: (a) amplitude; (b)frequency; (c) wavelength; & (d) phase. You may wishto illustrate your answers with diagrams.

    2. Give the equation for wave speed in terms of otherwave quantities.

    3. Calculate (a) the speed of a wave of frequency 60 Hzand wavelength 200 m. (b) the wavelength of a waveof speed 3 x 108ms-1and frequency 150 kHz; (c) thefrequency of a wave of wavelength 68 cm and speed340 ms-1

    4. What is meant by phase difference? Show howangular measurement in radians is used.

    5. Try the Summary Questions on page 177.

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    Notes on Superposition & Stationary Waves

    from Breithaupt pages 180 to 185

    1. What is the principle of superposition?

    Explain, using diagrams, how the

    processes of reinforcement and

    cancellation can occur (p180).


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