physics 2111 unit 24 - college of dupagesound is longitudinal wave - media oscillates back and forth...
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![Page 1: Physics 2111 Unit 24 - College of DuPageSound is longitudinal wave - media oscillates back and forth in the direction of travel of the wave Sound Waves Mechanics Lecture 24, Slide](https://reader030.vdocuments.us/reader030/viewer/2022040522/5e7e6a74ddfbe4714239fa5e/html5/thumbnails/1.jpg)
Physics 2111
Unit 24
Today’s Concepts:A) Sound waves
B) Interference
C) Intensity and Intensity Level
D) Doppler Effect
E) Beats
Mechanics Lecture 24, Slide 1
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Sound is longitudinal wave - media oscillates back and forth in the
direction of travel of the wave
Sound Waves
Mechanics Lecture 24, Slide 2
direction of travel
direction of oscillations
So what the heck am I plotting when I show a sound wave like this?
Value of longitudinal displacement! (back and forth, not up and down.)
x
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Recall that if I have two waves that a half of wave length out of phase, I get
destructive interference
Interference
Mechanics Lecture 24, Slide 3
l/2
No sound - silence
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Mechanics Lecture 24, Slide 4
How do I get them out of phase like that?
Start in phase….
Both waves
maximum at
your ear
but travel different distance to receiver
One maximum,
one minimum at
your ear
DL
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Mechanics Lecture 24, Slide 5
L1
L2
L1
L2
L1-L2 = DLDL = l *1, 2, 3, 4... constructive
DL = l *1/2, 3/2, 5/2... destructive
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Example 24.1 (Two Speakers)
Mechanics Lecture 24, Slide 6
A 214 Hz tone is emitted from
two stereo speakers, 3.2
meters apart. Alex stands 2.4
meters in front the right
speaker. The speed of sound
in the surrounding air is
343m/sec. Does he hear a
loud or a soft tone?
3.2m
2.4m
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Question
Mechanics Lecture 24, Slide 7
A 214 Hz tone is emitted from
two stereo speakers, 3.2
meters apart. Alex stands 2.4
meters in front the right
speaker. Does he hear a loud
or a soft tone?
3.2m
2.4m
A) Loud
B) Soft
C) We can’t tell yet
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Example 24.2 (Two Different Speakers)
Mechanics Lecture 24, Slide 8
A varying tone is emitted from two
stereo speakers, 2m meters
apart. Augie stands 3.45 meters
in front the right speaker. The
speed of sound in the sounding
air is 343m/sec. What are the first
two frequencies above 800Hz for
which he hears completely
constructive interference?
Completely destructive
interference?
2m
3.45m
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Question: Interference
Mechanics Lecture 24, Slide 9
A tone of varying frequency is emitted
from two stereo speakers, 2.4 meters
apart. Our hero stands 15 meters in
front the right speaker.
If the tone starts at 2000Hz and
increases what is the first frequency for
which he will hear the loudest sound?
2.4m
15m
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Question: Interference
Mechanics Lecture 24, Slide 10
What is the difference in the distance
the two sound waves traveled?
A) 2.4m
B) 15m
C) 0.25m
D) 0.21m
E) 0.19m
2.4m
15m
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Question: Interference
Mechanics Lecture 24, Slide 11
To here a loud sound, what should the
difference in the distance the two sound
waves traveled be in terms of wave
lengths?
A) n*l
B) l*(n+1/2)
C) l/n
D) l/(n+1/2)
E) n/l
2.4m
15m
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Question: Interference
Mechanics Lecture 24, Slide 12
What is our relationship between
wavelength(l), frequency(f) and velocity
of the wave (v)?
A) f = v*l
B) f = l/v
C) v = l/f
D) v =f*l
E) v = f/l
2.4m
15m
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Question: Interference
Mechanics Lecture 24, Slide 13
Set the difference in the distance
traveled to the requirement for
constructive interference. Use the
relationship between v, f and l just
found. You get what formula?
A) f = n*v/DL
B) f= n*v*DL
C) f = (n+1/2)*v/DL
D) f = (n+1/2)*v*DL
2.4m
15m
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Question: Interference
Mechanics Lecture 24, Slide 14
Take the value for DX we calculated and
the formula we just derived. Plug in
different values of m. What is the
lowest frequency you get above
2000Hz that will have constructive
interference? (vsound = 343m/sec)
A) 2520Hz
B) 3610Hz
C) 3810Hz
D) 4000Hz
2.4m
15m
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Question: Interference
Mechanics Lecture 24, Slide 15
Take the value for DX we calculated and
the formula we just derived. Plug in
different values of m. What is the
lowest frequency you get above
2000Hz that will have destructive
interference? (vsound = 343m/sec)
A) 2110Hz
B) 2350Hz
C) 2420Hz
D) 2710Hz
2.4m
15m
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Phase Angle
Shift written in terms of
“phase angle”
y1(x,t) = sin(kx - wt)
f = 2p*(DL/l)
y2(x,t) = sin(kx - wt + f)
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Phase Angle
Constructive
Shifted by n*2p
just some integer (0, 1, 2, 3, 4……)
Destructive
Difference in phase (n+1/2)*2p
Sometimes use “m” instead of “n”
Sometimes f is in degrees f = 360o*Dx/l
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Intensity
Mechanics Lecture 24, Slide 18
Recall
Power = Energy/Time
Intensity = Power/Area
= Energy/Time*Area
α Amplitude2*w2
Related to how loud it sounds
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Example 24.3 (Intensity)
Mechanics Lecture 24, Slide 19
A ringing bells put out 5 Joules of
sound energy every second. The
sound goes uniformly in all
directions.
What is the intensity of this sound
2m away from the bell?
What is the intensity 4m away?
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Intensity Level
Mechanics Lecture 24, Slide 20
Doubling intensity does not double the “loudness”
of the sound to you.
Human “loudness scale” approximated by
Intensity Level, b
b = 10db log (I/Io)
Recall:
• 10n = y n = log(y)
• log(1) = 0
• log(10) = 1
• log(100) = 2
Io = 10-12 Watt/m2
lowest threshold of hearing
Small changes in value of Intensity Level
BIG changes in power output
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Example 24.4 (Intensity Level)
Mechanics Lecture 24, Slide 21
A ringing bells put out 5 Joules of
sound energy every second. The
sound goes uniformly in all
directions.
What is the intensity level of this
sound 2m away from the bell?
What is the intensity level 4m
away?
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Intensity Level
Mechanics Lecture 24, Slide 22
Two physics students shout at a poor physics
instructor each with an intensity level of 60dB.
What is the intensity level of their combined
voices?
A. Greater than 120dB
B. 120dB
C. Less than 120dB, but greater than 60dB
D. 60dB
E. Less than 60dB
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Intensity Level
Mechanics Lecture 24, Slide 23
A quiet radio has an intensity level of about 40 dB.
Busy street traffic has a level of about 70 dB.
How much greater is the intensity of the street
traffic compared to the radio?
A. about 7/4 greater
B. about 7/3 greater
C. about 70/4 greater
D. about 100 times greater
E. about 1000 times greater
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Intensity Level
Mechanics Lecture 24, Slide 24
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where and
Resonance Patterns/Harmonics
Mechanics Lecture 24, Slide 25
Recall resonance for string instrument
Note the
frequency
pattern:
f = n*v/2L
n=1,2,3,4,5…
These happen
because the
wave reflects from
a node. (We can’t
change the
position.)
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Sound is longitudinal wave - media oscillates back and forth in the
direction of travel of the wave
Sound Waves
Mechanics Lecture 24, Slide 26
direction of travel
direction of oscillations
longitudinal displacement (seen another way –> pressure)
x
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Open Ended Wind Instruments
Mechanics Lecture 24, Slide 28
Sound wave will reflect off either
end of a enclosed pipe…
even if
it’s open.
Air is completely free to move at
open end. motion anti-node
l/4
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Open Ended Wind Instruments
Mechanics Lecture 24, Slide 29
l/4 These happen because
the wave reflects from a
anti-node. (We can’t
change the pressure.)
DEMO
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Mechanics Lecture 24, Slide 30
diagram
from week’s
lab.
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where and
Mechanics Lecture 24, Slide 31
Note the
frequency
pattern:
f = n*v/4L
n=1,3,5,7,9…
Even
harmonics
are missing
f = (n-1/2)*v/8L
l = 8L/(n-1/2)
n=1,2,3,4,5…
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Example 24.4 Resonance in Tube
Mechanics Lecture 24, Slide 32
You have a tube that is 15cm long
with one end up and one end closed
(like in lab). What is the fundamental
frequency?
That is, what tuning fork you could
hold over the open end so that it
would resonant at it fundamental
frequency?
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Question
Mechanics Lecture 24, Slide 33
You have a tube that is 15cm long with one
end up and one end closed (like in lab). We
just found fundamental frequency was
572Hz.
What is the frequency for the first overtone?
A) 858Hz
B) 1144Hz
C) 1716Hz
D) 2288Hz
E) 2860Hz
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Question - Resonance in Tube
Mechanics Lecture 24, Slide 34
You have a tube that is 15cm long with one
end up and one end closed (like in lab). We
just found fundamental frequency was
572Hz.
What if both ends were open? What would
be the fundamental frequency now?
A) 143Hz
B) 286HZ
C) 572Hz
D) 1144Hz
E) 2288HZ
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Mechanics Lecture 24, Slide 35
Doppler Effect
Image a speaker put out a uniform tone in all
directions.
Distance between waves
peaks is v*T = l
Distance between
waves peaks is
v*T – vE*T = l’
Now image
the speaker
moves
forward as it
puts out
sound
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Mechanics Lecture 24, Slide 36
Doppler Effect (moving observer)
What if the observer moves?
= fE (1+vR/fsl)
Observer now “runs into” more
waves per second than before.
Hear higher frequency.
fR = fE +vR/l
= fE (1+vR/vS)
fR = fE(1 +/- vR/vsound)
(1 -/+ vE/vsound)
Combine the two
equations
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Mechanics Lecture 24, Slide 37
Example 24.3 (police car)
A police car is moving to the left at 34m/sec while its
siren is emitting a 600Hz tone.
What tone would you hear if you were parked along
side the road?
What tone would you hear if the police car were parked
and you were moving towards the police car at
34m/sec?
What if you are both moving at 34m/sec?
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Question
Mechanics Lecture 24, Slide 38
For reasons that are not clear, Jane and Frank are
standing in the middle of the road as a Naperville
police car approaches with its siren on. The siren
emits a 9000Hz tone. Jane is 20 meters in front of
the car and Frank is 40 in front of the car. Who hears
a higher tone from the siren?
A) Frank
B) Jane
C) The both hear the same frequency.
JaneFrank
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Question
Mechanics Lecture 24, Slide 39
For reasons that are still not clear, Jane and Frank
are still standing in the middle of the road as a
Naperville police car comes along with its siren on.
But now the car has pasted Jane so she is 10 meters
behind the car and Frank is 10 meters in front of the
car. Who hears a higher tone from the siren?
A) Frank
B) Jane
C) The both hear the same frequency.
JaneFrank
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But something odd happens when added two sound waves with slightly different frequencies. Let’s do the math….
where
Beats
Mechanics Lecture 24, Slide 40
Y(x,t)total = A*sin(k1x-w1t) + A*sin(k2x-w2t)
Second, recall:
sin(a) + sin(b) = 2sin((a+b)/2)*cos((a-b)/2)
We know to find the resultant of two different waves at the same spot, you just add the two wave functions……
First, since we’re only going to look at one point in space, so the kx terms are constant…. We can ignore them.
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So we’d wind up with something that looked like…….
where and
cos(wLt) sin(wHt)
Beats
( )212
1www -L
( )21 fffBeat -
( ) ( )ttAtAtA LH wwww cossin2)sin()sin( 21 +
Mechanics Lecture 24, Slide 41
( )212
1www +H