Friday, December 11, 1998 Chapter 14: standing waves superposition interference REVIEW of Chapters...
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Transcript of Friday, December 11, 1998 Chapter 14: standing waves superposition interference REVIEW of Chapters...
Friday, December 11, 1998
Chapter 14: standing waves superposition interference
REVIEW of Chapters 13 & 14
Our final exam period is scheduled for thevery last possible day of finals’ week:
Friday, December 18, 1998!10:30 am - 12:30 pm
Please, do not leave town early
This 2-hour exam period will contain TWO exams.
The first 50 minutes will be used for an examon the material that we cover Chapters 13 & 14.It will be structured very much like Exam #3(three sections, one of which will be multiplechoice---you do two of the three). You will bepermitted to use the usual 3”X5” note card.
Final Exam: 1 hour plus comprehensive
5 sections, you do 4 (one will be multiple choice)
Each section somewhat shorter (25 points)
8.5”X11” crib sheet + 3”X5” note card fromExam #4
I will give you math & constants but notphysics formulae
Exam #4 (during the first 50 minutes of our final exam period) counts the same as the previous 3 exams (the best 3 scores from Exams #1 - 4 count 15% each).
If you are REALLY happy with your performance on the first 3 exams, simply notify me and you will be permitted to SKIP Exam #4. In this case you may show up 50 minutes into the exam period.
(I’m guessing there won’t be too many of YOU!)
Everyone MUST take the Final Exam.
You cannot pass this class without completing the final exam.
The final exam counts for everyone andis worth 20% of your final grade.
This is best demonstrated with an example.
Notice that all points on the slinky oscillateup and down with the same frequency, butdifferent amplitudes. Some points on theslinky do not move at all.
These points are called NODES.
Notice that the fixed end of the slinky issuch a nodal point---always in the sameplace---never moving.
We also observe nodes at various otherpoints along the slinky, spaced by acharacteristic distance equal to one halfof a wavelength.
In between the nodes are places at whichthe spring oscillates with the greatestamplitudes along its length.
Such places are called ANTI-NODES.
Notice that the end of the slinky from whichI force the waves is such an anti-node.
The lowest frequency (longest wavelength)standing wave that I can produce on theslink is 1/4 of a wavelength.
This lowest frequency is known as thefundamental frequency (a.k.a. the firstharmonic) of the slinky.
And I can produce a whole series of otherwaves, known as harmonics, on the slinky.
Notice that there is a discrete set of possiblewaves that the slinky will support. In fact,for this system (fixed at one end, open at theother), only waves with the followingfrequencies are permitted:
f nv
Lnwave4
L = length of slinkyn = 1, 3, 5, 7, ...
If our slinky were fixed at both ends, onlywaves with integral numbers of half-wavelengths could be supported on theslinky, since both ends would have tobe nodes.
f nv
Lnwave2
L = length of slinkyn = 1, 2, 3, 4, 5, ...
And though hard to imagine with our slinky,if it were free to move at both ends, againonly waves with integral numbers of half-wavelengths could be supported on theslinky’s length. The slinky would requireanti-nodes at both ends!
f nv
Lnwave2
L = length of slinkyn = 1, 2, 3, 4, 5, ...
Rules of thumb:
Open (free) ends have anti-nodes.
Closed (fixed) ends have nodes.
Recall that the speed of the wavespropagating along strings (such as onharps, violins, and pianos) is given by
F
And the speed of the wavespropagating in the air inside pipesare given by the speed of sound.
vsound = 340 m/s
Superposition of WavesSuperposition of Waves
How do I add waves together? Point-by-Point
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
0.0 2.5 5.0 7.5
time
Am
plit
ud
e
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
0.0 2.5 5.0 7.5
time
Am
plit
ud
e
+=
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
0 2.5 5 7.5
timeam
pli
tud
e
constructiveinterference
constructiveinterference
When waves interfere constructively, theanti-nodes become greater in magnitudethan either of the waves of which theresulting wave is composed.
Sounds emanating from stereo speakersare louder in places of constructiveinterference.
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
0.0 2.5 5.0 7.5
time
Am
plit
ud
e
+=
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
0 2.5 5 7.5
time
Am
plit
ud
e
-2
-1.5
-1
-0.5
0
0.5
1
1.5
2
0 2.5 5 7.5
time
Am
pli
tud
e
These two waves are 180o out-of-phase. Thatis, if you shifted one by 180o relative to the other,the two waves would appear exactly the same.
destructiveinterference
destructiveinterference
When waves interfere destructively, theanti-nodes precisely cancel one another,resulting in a constant node.
Sounds emanating from stereo speakersare softer in places of destructiveinterference. If the tone is pure, the sounddisappears completely.
Please do your best to fill out these evaluationforms. Your comments are appreciated!
In Part IV of our story, we wave good-byeto our beloved Physics 111 students tothunderous ovations, boos, and hissesas they propagate into the holiday seasonto ring in the New Year.
F = - kx
PE kxspring 1
22 KE PE PEg spring
TA
v
m
k
22
max
fk
m
1
2 2 f
k
m
vk
mA x ( )2 2
Fixedend
x
Tr
v
2
Angular Frequency f
Frequency f = 1/T
FT
Fg
s
F mg sin
TL
g2
Good for SMALLamplitude
oscillations!
Height of Block vs Time
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Time (s)
Hei
gh
t (m
)
Equilibriumposition
Amplitude
period
Amplitude
TRAVELLING WAVES:
Therefore, we note that waves do NOTultimately transport matter. They onlytemporarily displace the matter in whichthey move.
v f
Height of Block vs Time
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Time (s)
Hei
gh
t (m
)
Equilibriumposition
Amplitude
period
Amplitude
Position of Piece of Slinky vs Time
Height of Block vs Time
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Time (s)
Hei
gh
t (m
)
Equilibriumposition
Amplitude
wavelength
Amplitude
Shape of Slinky at Time 1
X-position
Y-p
osi
tio
n
crest
trough
The propagation speed is governed bythe mass per unit length () of the materialand the tension (FT) within the material.
vF
What happens to a wave when it hits afixed boundary?
Bounces back (reflects) inverted.
What happens to a wave when it gets tothe end of the slinky that is not fixed?
Reflects with the same orientation.
mo
lecu
les
rare
fied
mo
lecu
les
com
pre
ssed
t = t3
mo
lecu
les
rare
fied
mo
lecu
les
com
pre
ssed
mo
lecu
les
com
pre
ssed
mo
lecu
les
rare
fied
Crests & Troughs in direction of propagation!
In fact, we find that thespeed of sound is given by:
vB
s
Where B is the bulk modulus and is the equilibrium density of the medium.
In solids, we find that thespeed of sound is given by:
vY
sound
Where Y is the Young’s modulus and is the equilibrium density of the medium.
IP
A
FHGIKJ( ) log10
0
dBI
I
Where I is the intensity of the sound andI0 is the intensity of a reference level, usually
taken to be the threshold of hearing(10-12 W/m2).
Listener Moving f fu
' 0
+ approach
- recede
Source Movingf f
v vsound
'( / )
FHG
IKJ0
1
1
- approach+ recede
v = speedof source
Both moving
Rule of Thumb:
If the objects are getting closer together,the frequency should be higher.
If the objects are separating, the frequencyshould be lower.
f fu v
v vsound
sound
'( / )
( / )
FHG
IKJ0
1
1
u = speed listenerv = speed source
I wish you a happy, peaceful, andrestful holiday season.
It has been my sincere pleasure andprivilege to have the opportunityto explore the world of physics withyou this semester.