sound, wavefronts wavefronts join points in phase linear wavefronts

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Sound, Wavefronts

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Page 1: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Sound, Wavefronts

Page 2: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Wavefronts join points in phase

Linear wavefronts

Page 3: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Wavefronts for compressional wave.

Page 4: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Rays – a ray is an arrow sketched through the wave fronts (perpendicular) to show direction of wave propagation.

Page 5: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Waves transfer energyEnergy is proportionalto the amplitude.

Less energy

More energy

Page 6: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

For light increased amplitude increases brightness.

Page 7: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

For sound: increased amplitude increases volume.

Page 8: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

What does wave frequency (f) determine?

Wave type for EM waves.

Color for light.

Page 9: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Sound velocity solid

liquid

gas

In gas

hot faster.

cold slower.

Increasing velocity

Page 10: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

The Doppler Effect

Stationary Source Emitting Waves all Directions. Circular wavefronts have = & f.

Page 11: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Doppler Effect from Moving Source

In front of source is less, behind is longer.

Page 12: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Another View

Page 13: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

In front of source -short higher f:

hear higher pitch sound-see shorter light (blue).

behind source - longer lower f:

hear lower pitch soundsee longer light (red).

Page 14: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

When objects are in relative motion:

a) Toward each other, f received increases.

b) Away from each other, f received decreases.

Doppler Effect

Page 15: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Resonance & Sympathetic Vibration

Page 16: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

All objects have a naturalAll objects have a natural

frequency of vibration.frequency of vibration.

ResonanceResonance - the inducing- the inducingof vibrations of a naturalof vibrations of a naturalrate by a vibrating sourcerate by a vibrating source

having the same frequencyhaving the same frequency

““sympathetic vibrations”sympathetic vibrations”

Page 17: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Push at natural frequency, amplitude increases

Page 18: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Resonance:

An oscillatory system that is driven by a force with a frequency = to its natural frequency.

System will resonate – amplitude will increase.

Page 19: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Resonance & Sympathetic Vibration

Resonance occurs when a wave is in vicinity of an object & is vibrating at the natural frequency of the object. Object vibrates sympathetically at same frequency.

Continued vibration causes amplitude to increase.

Page 21: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

A broad variety of tone colors exist because most sounds we perceive as pitch contain many frequencies.

• The predominant pitch The predominant pitch is called the is called the fundamental fundamental frequency. It is the frequency. It is the longest longest that forms a that forms a standing wave.standing wave.

Page 22: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Standing Wave patterns form notes.

Each string or pipe vibrates with particular frequencies of standing waves.

Other frequencies tend to die out.

Page 23: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Although we would perceive a string vibrating as a whole,

it vibrates in a pattern that appears erratic producing many different overtone pitches. What results are particular tone colors or timbres of instruments and voices.

Page 24: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Waveform with overtones.

Page 25: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Frequencies which occur along with the primary note are called the harmonic or overtone series.

When C is the fundamental the pitches below represent its first 15 overtones.

Page 26: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

There are several standing waves which can be produced by vibrations on a string, or rope. Each pattern corresponds to vibrations which occur at a particular frequency and is known as a harmonic.

Harmonics

Page 27: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

The lowest possible frequency at which a string could vibrate to form a standing wave pattern is known as the fundamental frequency or the first harmonic.

Page 28: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

2nd Harmonic

Page 29: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Which One??

Page 30: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

String Length L, & Harmonics

Standing waves can form on a string of length L, when the can = ½ L, or 2/2 L, or 3/2L etc.

Standing waves are the overtones or harmonics.

L = nn. n = 1, 2, 3, 4 harmonics. 2

Page 31: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Harmonic Frequencies

form where ½ can fit the string exactly.To calculate f:

L

nvf

2

f

vfv

2

nL

Substitute v/f for .

f

nvL

2

Page 32: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

1st standing wave forms when = 2LFirst harmonic frequency is when n = 1 as below.

L

nvf

21

When n = 1 f is fundamental frequency or 1st harmonic.

Page 33: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

L

nvf

22 For second harmonic n = 2.

f2 = v/L

Other standing waves with smaller wavelengths form other frequencies that ring out along with the fundamental.

Page 34: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

In general,

The harmonic frequencies can be found where n = 1,2,3… and n corresponds to the harmonic. v is the velocity of the wave on the string. L is the string length.

L

nvfn 2

Page 35: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

It is helpful to note that the distance between nodes on a standing wave is ½ .

½

Page 36: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Pipes and Air Columns

Page 37: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

A resonant air column isA resonant air column issimply a standing simply a standing

longitudinallongitudinalwave system, much likewave system, much like

standing waves on a standing waves on a string.string. closed-pipe resonatorclosed-pipe resonator tube in which one end is tube in which one end is

openopenand the other end is closedand the other end is closed

open-pipe resonatoropen-pipe resonatortube in which both endstube in which both ends

are openare open

Page 38: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Open Pipe – open end has antinode.

Page 39: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Standing Waves in Open PipeBoth ends must be antinodes.

How much of the wavelength is the fundamental?

Page 40: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

The 1st harmonic or fundamental can fit ½ into the tube.

Just like the string L = n 2

fn = nv2L

Where n, the harmonic is an integer.

Page 41: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Closed pipes must have a node at closed end and an antinode at the open end.

How many wavelengths??

Page 42: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Here is the next harmonic.How many ’s?

Page 43: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

There are only odd harmonics possible.

L = 1/4.L = 3/4.L = 5/4

fn = nv where n = 1,3,5 … 4L

Page 44: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Beats – caused by constructive & destructive interference from 2

frequency sounds interacting.

• Beat Frequency heard is the difference between 2 frequencies.

• If a 50 Hz wave and a 60 Hz wave overlap, you hear beat of 10 Hz.

Page 45: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

• hear beat frequencies

Page 46: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts
Page 47: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Traveling Waves Beats

Page 48: Sound, Wavefronts Wavefronts join points in phase Linear wavefronts

Holt read 13 - 3

pg 509 38 - 39, 41, 44 46, 47 pg 499 #1 – 4

Start in class finish for hwk.