waves topic 11.1 standing waves. v the formation

56
Waves Topic 11.1 Standing Waves

Upload: lorena-hodges

Post on 14-Jan-2016

230 views

Category:

Documents


1 download

TRANSCRIPT

Page 1: Waves Topic 11.1 Standing Waves. v The Formation

WavesTopic 11.1

Standing Waves

Page 2: Waves Topic 11.1 Standing Waves. v The Formation

Standing Waves

The Formation

Page 3: Waves Topic 11.1 Standing Waves. v The Formation

• When 2 waves of

–the same speed

–and wavelength

–and equal or almost equal amplitudes

–travelling in opposite directions

• meet, a standing wave is formed

Page 4: Waves Topic 11.1 Standing Waves. v The Formation

• The standing wave is the result of the superposition of the two waves travelling in opposite directions

• The main difference between a standing and a travelling wave is that in the case of the standing wave no energy or momentum is transferred down the string

Page 5: Waves Topic 11.1 Standing Waves. v The Formation

• A standing wave is characterised by the fact that there exists a number of points at which the disturbance is always zero

• These points are called Nodes

• And the amplitudes along the waveform is different

• In a travelling wave there are no points where the disturbance is always zero, all the points have the same amplitude.

Page 6: Waves Topic 11.1 Standing Waves. v The Formation

At the correct frequencya standing wave is formed

The frequency is increaseduntil a different standing wave is formed

Page 7: Waves Topic 11.1 Standing Waves. v The Formation

Resonance

• If the frequency of the source of a vibration is exactly equal to the natural frequency of the oscillatory system then the system will resonate

• When this occurs the amplitude will get larger and larger

• Pushing a swing is an example of resonance

• Resonance can be useful and harmful

Page 8: Waves Topic 11.1 Standing Waves. v The Formation

• Airplane wings, engines, bridges, tall buildings are objects that need to be protected against resonance from external vibrations due to wind and other vibrating objects

• Soldiers break step when marching over a bridge in case the force which they exert on the bridge starts uncontrollable oscillations of the bridge

Page 9: Waves Topic 11.1 Standing Waves. v The Formation

Resonance and Standing Waves

1. Standing Waves on Strings

Page 10: Waves Topic 11.1 Standing Waves. v The Formation
Page 11: Waves Topic 11.1 Standing Waves. v The Formation

• If you take a wire and stretch it between two points then you can set up a standing wave

• The travelling waves are reflected to and fro between the two ends of the wire and interfere to produce the standing wave

•This has a node at both ends• and an antinode in the middle •– it is called the fundamental

Page 12: Waves Topic 11.1 Standing Waves. v The Formation

• With this wave the length of the string is equal to half the wave length

• L = ½ = 2L

• As v = f • Then f = v / f = v / 2L

• This is the fundamental frequency of the string (the 1st harmonic)

Page 13: Waves Topic 11.1 Standing Waves. v The Formation

• This is not the only standing wave that can exist on the string

• The next standing wave is

This is called the 2nd Harmonic

L =

Page 14: Waves Topic 11.1 Standing Waves. v The Formation

• With this wave the length of the string is equal to the wave length

• L = = L

• As v = f • Then f = v / f = v / L

• This is the 2nd Harmonic frequency of the string

• Notice it is twice the fundamental frequency

Page 15: Waves Topic 11.1 Standing Waves. v The Formation

• The next standing wave is

L = 3/2

This is called the 3rd Harmonic

Page 16: Waves Topic 11.1 Standing Waves. v The Formation

• With this wave the length of the string is equal to 3/2 of the wave length

• L =3/2 = 2/3L• As v = f

• Then f = v / f = v / 2/3L f = 3v / 2L

• This is the 3rd Harmonic frequency of the string• Notice it is three times the fundamental frequency

Page 17: Waves Topic 11.1 Standing Waves. v The Formation

• Notice that the only constraint is that the ends of the string are nodes.

• In general we find that the wavelengths satisfy

= 2L

n

Where n = 1,2,3,4……

Page 18: Waves Topic 11.1 Standing Waves. v The Formation

• This is the harmonic series

• The fundamental is the dominant vibration and will be the one that the ear will hear above all the others

• The harmonics effect the quality of the note

• It is for this reason that different musical instruments sounding a note of the same frequency sound different

• (it is not the only way though)

Page 19: Waves Topic 11.1 Standing Waves. v The Formation

Resonance and Standing Waves

2. Standing Waves in Pipes

Page 20: Waves Topic 11.1 Standing Waves. v The Formation

• Sound standing waves are also formed in pipes

• Exactly the same results apply

• There are two types of pipes

–1. Open ended

–2. Closed at one end

• Nodes exist at closed ends

• Antinodes exists at open ends

Page 21: Waves Topic 11.1 Standing Waves. v The Formation

a) Open Ended

• Fundamental Frequency (1st Harmonic)

L = /2

= 2L

•As v = f •Then f = v / f = v / 2L

Page 22: Waves Topic 11.1 Standing Waves. v The Formation

• 2nd Harmonic

= L

•As v = f •Then f = v / f = v / L

L =

Page 23: Waves Topic 11.1 Standing Waves. v The Formation

• 3rd Harmonic

= 2/3L

•As v = f •Then f = v /

f = v / 2/3L f = 3v / 2L

L = 3/2

Page 24: Waves Topic 11.1 Standing Waves. v The Formation

• The harmonics are in the same series as the string series

• If the fundamental frequency = f

• Then the 2nd harmonic is 2f, 3rd is 3f and the 4th is 4f… etc

Page 25: Waves Topic 11.1 Standing Waves. v The Formation

b) Closed at one End

• Fundamental Frequency (1st Harmonic)

L = /4

= 4L

•As v = f •Then f = v / f = v / 4L

Page 26: Waves Topic 11.1 Standing Waves. v The Formation

• Next Harmonic

= 4/3L

•As v = f •Then f = v /

f = v / 4/3L f = 3v / 4L

L = 3/4

Page 27: Waves Topic 11.1 Standing Waves. v The Formation

• And the next harmonic

= 4/5L

•As v = f •Then f = v /

f = v / 4/5L f = 5v / 4L

L = 5/4

Page 28: Waves Topic 11.1 Standing Waves. v The Formation

• The harmonics are DIFFERENT to the string and open pipe series

• If the fundamental frequency = f

• Then there is no 2nd harmonic

• The 3rd is 3f

• There is no 4th harmonic

• The 5th is 5f

Page 29: Waves Topic 11.1 Standing Waves. v The Formation

WavesTopic 4.3

Standing Waves

Page 30: Waves Topic 11.1 Standing Waves. v The Formation

Standing Waves

The Formation

Page 31: Waves Topic 11.1 Standing Waves. v The Formation

• When 2 waves of

–the same speed

–and wavelength

–and equal or almost equal amplitudes

–travelling in opposite directions

• meet, a standing wave is formed

Page 32: Waves Topic 11.1 Standing Waves. v The Formation

• The standing wave is the result of the superposition of the two waves travelling in opposite directions

• The main difference between a standing and a travelling wave is that in the case of the standing wave no energy or momentum is transferred down the string

Page 33: Waves Topic 11.1 Standing Waves. v The Formation

• A standing wave is characterised by the fact that there exists a number of points at which the disturbance is always zero

• These points are called Nodes

• And the amplitudes along the waveform is different

• In a travelling wave there are no points where the disturbance is always zero, all the points have the same amplitude.

Page 34: Waves Topic 11.1 Standing Waves. v The Formation

At the correct frequencya standing wave is formed

The frequency is increaseduntil a different standing wave is formed

Page 35: Waves Topic 11.1 Standing Waves. v The Formation

Resonance

• If the frequency of the source of a vibration is exactly equal to the natural frequency of the oscillatory system then the system will resonate

• When this occurs the amplitude will get larger and larger

• Pushing a swing is an example of resonance

• Resonance can be useful and harmful

Page 36: Waves Topic 11.1 Standing Waves. v The Formation

• Airplane wings, engines, bridges, tall buildings are objects that need to be protected against resonance from external vibrations due to wind and other vibrating objects

• Soldiers break step when marching over a bridge in case the force which they exert on the bridge starts uncontrollable oscillations of the bridge

Page 37: Waves Topic 11.1 Standing Waves. v The Formation

Resonance and Standing Waves

1. Standing Waves on Strings

Page 38: Waves Topic 11.1 Standing Waves. v The Formation
Page 39: Waves Topic 11.1 Standing Waves. v The Formation

• If you take a wire and stretch it between two points then you can set up a standing wave

• The travelling waves are reflected to and fro between the two ends of the wire and interfere to produce the standing wave

•This has a node at both ends• and an antinode in the middle •– it is called the fundamental

Page 40: Waves Topic 11.1 Standing Waves. v The Formation

• With this wave the length of the string is equal to half the wave length

• L = ½ = 2L

• As v = f • Then f = v / f = v / 2L

• This is the fundamental frequency of the string (the 1st harmonic)

Page 41: Waves Topic 11.1 Standing Waves. v The Formation

• This is not the only standing wave that can exist on the string

• The next standing wave is

This is called the 2nd Harmonic

L =

Page 42: Waves Topic 11.1 Standing Waves. v The Formation

• With this wave the length of the string is equal to the wave length

• L = = L

• As v = f • Then f = v / f = v / L

• This is the 2nd Harmonic frequency of the string

• Notice it is twice the fundamental frequency

Page 43: Waves Topic 11.1 Standing Waves. v The Formation

• The next standing wave is

L = 3/2

This is called the 3rd Harmonic

Page 44: Waves Topic 11.1 Standing Waves. v The Formation

• With this wave the length of the string is equal to 3/2 of the wave length

• L =3/2 = 2/3L• As v = f

• Then f = v / f = v / 2/3L f = 3v / 2L

• This is the 3rd Harmonic frequency of the string• Notice it is three times the fundamental frequency

Page 45: Waves Topic 11.1 Standing Waves. v The Formation

• Notice that the only constraint is that the ends of the string are nodes.

• In general we find that the wavelengths satisfy

= 2L

n

Where n = 1,2,3,4……

Page 46: Waves Topic 11.1 Standing Waves. v The Formation

• This is the harmonic series

• The fundamental is the dominant vibration and will be the one that the ear will hear above all the others

• The harmonics effect the quality of the note

• It is for this reason that different musical instruments sounding a note of the same frequency sound different

• (it is not the only way though)

Page 47: Waves Topic 11.1 Standing Waves. v The Formation

Resonance and Standing Waves

2. Standing Waves in Pipes

Page 48: Waves Topic 11.1 Standing Waves. v The Formation

• Sound standing waves are also formed in pipes

• Exactly the same results apply

• There are two types of pipes

–1. Open ended

–2. Closed at one end

• Nodes exist at closed ends

• Antinodes exists at open ends

Page 49: Waves Topic 11.1 Standing Waves. v The Formation

a) Open Ended

• Fundamental Frequency (1st Harmonic)

L = /2

= 2L

•As v = f •Then f = v / f = v / 2L

Page 50: Waves Topic 11.1 Standing Waves. v The Formation

• 2nd Harmonic

= L

•As v = f •Then f = v / f = v / L

L =

Page 51: Waves Topic 11.1 Standing Waves. v The Formation

• 3rd Harmonic

= 2/3L

•As v = f •Then f = v /

f = v / 2/3L f = 3v / 2L

L = 3/2

Page 52: Waves Topic 11.1 Standing Waves. v The Formation

• The harmonics are in the same series as the string series

• If the fundamental frequency = f

• Then the 2nd harmonic is 2f, 3rd is 3f and the 4th is 4f… etc

Page 53: Waves Topic 11.1 Standing Waves. v The Formation

b) Closed at one End

• Fundamental Frequency (1st Harmonic)

L = /4

= 4L

•As v = f •Then f = v / f = v / 4L

Page 54: Waves Topic 11.1 Standing Waves. v The Formation

• Next Harmonic

= 4/3L

•As v = f •Then f = v /

f = v / 4/3L f = 3v / 4L

L = 3/4

Page 55: Waves Topic 11.1 Standing Waves. v The Formation

• And the next harmonic

= 4/5L

•As v = f •Then f = v /

f = v / 4/5L f = 5v / 4L

L = 5/4

Page 56: Waves Topic 11.1 Standing Waves. v The Formation

• The harmonics are DIFFERENT to the string and open pipe series

• If the fundamental frequency = f

• Then there is no 2nd harmonic

• The 3rd is 3f

• There is no 4th harmonic

• The 5th is 5f