for source moving away from observer, wavelength increases following the same procedures gives ...

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For source moving away from observer, wavelength increases Following the same procedures gives For source moving away, f o <f s . Observer hears lower pitch. d T s v v / v 1 1 s s o f f Moving Observer If the observer moves toward the source (which is at rest) with speed v o , the emitted wavelength remains constant

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Page 1: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

For source moving away from observer, wavelength increases

Following the same procedures gives

For source moving away, fo<fs. Observer hears lower pitch.

’d

Tsv

v/v1

1

sso ff

Moving Observer

If the observer moves toward the source (which is at rest) with speed vo, the emitted wavelength remains constant

Page 2: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

But the observer can “run’’ into more cycles (wave crests) than if she remained at rest. The number of additional cycles encountered is

Or the additional number of cycles/second, which is a frequency, is

Therefore, the frequency heard by the observer is

/vot

f /vo

sso

sssso

fff

ffffff

v/ since v

v1

v1

v

o

oo

Page 3: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

Therefore, if the observer is moving towards the source, the frequency heard by the observer is increased, fo>fs

Now, for the observer moving away from the source, he will encounter vot/ fewer wave crests than if she remained stationary. The observed frequency will be:

v

v1

v1

v

o

oo

so

sssso

ff

ffffff

In this case f0<fs

Page 4: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

To summarize: 1) Moving source

v/v1

1

sso ff

2) Moving observer:

v

v1 o

so ff

(-) moving together

(+) moving apart

(+) moving together

(-) moving apart

Note that equations look similar, but mechanism for frequency shifts (f=fo-fs) are different

Finally, both observer and source can be moving

v/v1

v/v1

s

o

so ff

Page 5: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

Example ProblemSuppose you are stopped for a traffic light and an ambulance approaches from behind with a speed of 18 m/s. The siren on the ambulance produces sound with a frequency of 955 Hz. The air sound speed is 343 m/s. What is the wavelength of the sound reaching your ears?

Solution:

Given: vo=0,vs=18 m/s, v=343 m/s, fs=955 Hz

Method: find fo then o, use moving source equation

Page 6: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

m 0.359Hz) 955/()m/s 343(v/

m 0.340Hz) 1000/()m/s 343(v/ v/ Hz 1008

/343)(18-1

1Hz) 955(

v/v1

1

v/v1

1

o

s

s

ss

oo

o

so

so

f

ff

ff

ff

Use (-) since source is approaching observer, fo>fs

Compare to source wavelength

Example Problem

A microphone is attached to a spring that is sus-pended from a ceiling. Directly below on the floor is a stationary 440-Hz source of sound. The micro-

Page 7: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

phone vibrates up and down in SHM with a period of 2.0 s. The difference between the the maximum and minimum sound frequencies detected by the microphone is 2.1 Hz. Ignoring any sound reflections in the room, determine the amplitude of the SHM of the microphone.

Solution:

s

o

Given: vs=0, fs=440 Hz, fo,max –fo, min = 2.1 Hz = f, Tmicrophone=Tm=2.0 s (SHM), assume vsound=343 m/s

Observer is moving:

v

v1 o

so ff

y

Page 8: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

Frequency of observer (microphone) is maximum when microphone has maximum velocity approaching the source, and minimum when microphone has maximum velocity receding from source. Since microphone is moving with SHM, its velocity is

)/2(

|v|

t)sin(v

max o,

o

mTA

A

A

m

so

so T

Afff

v

21

v

v1 max,

max,

A, the SHM amplitude, is what we want to find.

Microphone moving towards source Microphone

moving away from source

vo

t

Page 9: For source moving away from observer, wavelength increases  Following the same procedures gives   For source moving away, f o

m 26.0Hz) 440(4

)Hz 1.2)(s 0.2)(m/s 343(

4

v

v

4

v

21

v

21

v

21

v

21

Hz 1.2

v

21

v

v1

min,max,

max,min,

A

f

fTA

T

Af

T

A

T

Af

T

Af

T

Af

fff

T

Afff

s

m

m

s

mm

s

m

s

m

s

oo

m

so

so

Measured by microphone

Microphone is oscillating with this amplitude