Physics 207 – Lecture 29 Lecture 29, Dec. 10 Room 5208 ... · Page 10 Physics 207 – Lecture 29 Physics 207: Lecture 29, Pg 19 An example A monatomic gas is compressed isothermally

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Physics 207 – Lecture 29

Physics 207: Lecture 29, Pg 1

Lecture 29, Dec. 10To do :To do :

•• Chapter 21Chapter 21� Understand beats as the superposition of two waves of

unequal frequency.Prep for exam. Room 2103 Chamberlain Hall Sections: 602, 604, 605, 606, 610, 611, 612, 614 Room 5208 Sewell Social Science (1180 Observatory Dr.)Sections: 601, 603, 607, 608, 609, 613Room 5310: McBurney and by prior arrangement

9:25 Evaluations

•• AssignmentAssignment� HW12, Due Friday, Dec. 12th , 10:59 PM


Superposition & Interference

� Consider two harmonic waves A and B meet at t=0.� They have same amplitudes and phase, but

ω2 = 1.15 x ω1.� The displacement versus time for each is shown below:

A(ω1t)

B(ω2t)

CONSTRUCTIVEINTERFERENCE

DESTRUCTIVEINTERFERENCE

C(t) = A(t) + B(t)

Beat Superposition

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Superposition & Interference

� Consider A + B,

DA(x,t)=A cos(k1x–ω1t) DB(x,t)=A cos(k2x–ω2t)And let x=0, D=DA+DB=2A cos[2π (f1 – f2)t/2] cos[2π (f1 + f2)t/2] and |f1 – f2|

≡fbeat = = 1 / Tbeat

A(ω1t)

B(ω2t)

C(t) = A(t) + B(t)Tbeat

t


Exercise Superposition

� The traces below show beats that occur when two different pairs of waves are added (the time axes are the same).

� For which of the two is the difference in frequency of the original waves greater?

A. Pair 1

B. Pair 2

C. The frequency difference was the same for both pairs of waves.

D. Need more information.

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Organ Pipe Example

A 0.9 m organ pipe (open at both ends) is measured to have it’s first harmonic (i.e., its fundamental) at a frequency of 382 Hz.What is the speed of sound (refers to energy transfer) in this pipe?

L=0.9 m

f = 382 Hz and f λ = v with λ = 2 L / m (m = 1)

v = 382 x 2(0.9) m � v = 687 m/s


Standing Wave Question

� What happens to the fundamental frequency of a pipe, if the air (v =300 m/s) is replaced by helium (v = 900 m/s)?

Recall: f λ = v

(A) Increases (B) Same (C) Decreases

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Sample Problem

� The figure shows a snapshot graph D(x, t = 2 s) taken at t = 2 s of a pulse traveling to the left along a string at a speed of 2.0 m/s. Draw the history graph D(x = −2 m, t) of the wave at the position x = −2 m.


Sample Problem

� History Graph:

2 3 64 7time (sec)

2

-25

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Example problem

� Two loudspeakers are placed 1.8 m apart. They play tones of equal frequency. If you stand 3.0 m in front of the speakers, and exactly between them, you hear a maximum of intensity.

� As you walk parallel to the plane of the speakers, staying 3.0 maway, the sound intensity decreases until reaching a minimum when you are directly in front of one of the speakers. The speedof sound in the room is 340 m/s.

a. What is the frequency of the sound?b. Draw, as accurately as you can, a wave-front diagram. On your

diagram, label the positions of the two speakers, the point at which the intensity is maximum, and the point at which the intensity is minimum.

c. Use your wave-front diagram to explain why the intensity is a minimum at a point 3.0 m directly in front of one of the speakers.


Example problem


� As you walk parallel to the plane of the speakers, staying 3.0 maway, the sound intensity decreases until reaching a minimum when you are directly in front of one of the speakers. The speed of sound in the room is 340 m/s.

� What is the frequency of the sound?

v = f λ but we don’t know f or λ DRAW A PICTURE

Constructive Interference in-phase

Destructive Interference out-of-phase

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Example problem


� v = 340 m/s.PUT IN GEOMETRY

v = f λ but we don’t know f or λ AC - BC = 0 (0 phase differenc)AD - BD = λ/2 (π phase shift)AD = (3.02+1.82)1/2

BD = 3.0

λ = 2(AD-BD) =1.0 m

Constructive Interference in-phase

Destructive Interference out-of-phase

3.0 m

1.8

m

A

B

C

D


Example problem


b. Draw, as accurately as you can, a wave-front diagram. On your diagram, label the positions of the two speakers, the point at which the intensity is maximum, and the point at which the intensity is minimum.

c. Use your wave-front diagram to explain why the intensity is a minimum at a point 3.0 m directly in front of one of the speakers.

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Sample problem

� A tube, open at both ends, is filled with an unknown gas. The tube is 190 cm in length and 3.0 cm in diameter. By using different tuning forks, it is found that resonances can be excited at frequencies of 315 Hz, 420 Hz, and 525 Hz, and at no frequencies in between these.

a. What is the speed of sound in this gas?b. Can you determine the amplitude of the wave? If so, what is it?

If not, why not?


Sample problem

� A tube, open at both ends, is filled with an unknown gas. The tube is 190 cm in length and 3.0 cm in diameter. By using different tuning forks, it is found that resonances can be excited at frequencies of 315 Hz, 420 Hz, and 525 Hz, and at no frequencies in between these.

What is the speed of sound in this gas? L=1.9 meters and fm = vm/2L315 = v m/2L

420 = v (m+1)/2L 525 = v (m+2)/2Lv/2L = 105 v = 3.8 x 105 m/s =400 m/s

b) Can you determine the amplitude of the wave? If so, what is it? If not, why not?

Answer: No, the sound intensity is required and this is not known.

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Sample Problem

� The picture below shows two pulses approaching each other on a stretched string at time t = 0 s. Both pulses have a speed of 1.0 m/s. Using the empty graph axes below the picture, draw a picture of the string at t = 4 s.


An example

� A heat engine uses 0.030 moles of helium as its working substance. The gas follows the thermodynamic cycle shown.

a. Fill in the missing table entriesb. What is the thermal efficiency of this engine?c. What is the maximum possible thermal efficiency of an engine

that operates between Tmax and Tmin?

B

A C

A: T= 400 K

B: T=2000 K

C: T= 1050 K

0 J0 JB�C

600 JNET-243 J-161 J0 JC�A

600 J0 J0 J600 JA�B∆EThWbyQLQH

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The Full Cyclic Process

� A heat engine uses 0.030 moles of helium as its working substance. The gas follows the thermodynamic cycle shown.

a. What is the thermal efficiency of this engine?b. What is the maximum possible thermal efficiency of an engine

that operates between Tmax and Tmin?(T = pV/nR, pVγ =const.)

B

A C

A: T= 400 K=1.01x105 10-3/ 0.030/8.3

B: T=2000 K

pBVBγ = pC VC

γ

(pBVBγ / pC )1/γ = VC

(5 (10-3)5/3 / 1)3/5 = VC = 2.6 x 10-3 m3

C: T= 1050 K


The Full Cyclic Process

B

A C

-355 J355 J0 J0 JB�C

0 J194 J404 J600 JNET -243 J-161 J404 J0 JC�A

600 J0 J0 J600 JA�B∆EThWbyQLQH

A: T= 400 K=1.01x105 10-3/ 0.030/8.3

B: T=2000 K

VC = 2.6 x 10-3 m3

C: T= 1050 K

Q = n Cv ∆T = 0.030 x 1.5 x 8.3 ∆T

Q = 0.3735 ∆T

WC�A (by) = p ∆V = 1.01x105 1.6 x 10-3 J

η = Wby / QH = 194/ 600 = 0.32

ηCarnot = 1- TL / TH= 1- 400/2000 =0.80

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An example

� A monatomic gas is compressed isothermally to 1/8 of its original volume.

� Do each of the following quantities change? If so, does the quantity increase or decrease, and by what factor? If not, why not?

a. The rms speed vrms

b. The temperaturec. The mean free path d. The molar heat capacity CV


An example

� A creative chemist creates a small molecule which resembles a freely moving bead on a wire (rotaxanes are an example). The wire is fixed and the bead does not rotate.

� If the mass of the bead is 10-26 kg, what is the rms speed of the bead at 300 K?

Below is a rotaxane model with three “beads” on a short wire

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An example

� A creative chemist creates a small molecule which resembles a freely moving bead on a wire (rotaxanes are an example). Here the wire is a loop and rigidly fixed and the bead does not rotate.

� If the mass of the bead is 10-26 kg, what is the rms speed of the bead at 300 K?

� NOT for any exam but an interesting aside: If a molecular wire has a length of 20 nm and will break if the force exceeds 10-10

N, estimate the temperature at which it will break. (I get, 36000 K….covalent chemical bonds are very strong)

Classically there is ½ kBT of thermal energy per degree of freedom.

Here there is only one so:

½ mvrms2 = ½ kBoltzmannT

vrms=(kBoltzmannT/m)½ = 640 m/s


An example

� A small speaker is placed in front of a block of mass 4 kg. Themass is attached to a Hooke’s Law sping with sping constant 100 N/m. The mass and speaker have a mechanical energy of 200 J and are undergoing one dimensional simple harmonic motion. The speaker emits a 200 Hz tone.

� For a person is standing directly in front of the speaker, what range of frequencies does he/she hear?

� The closest the speaker gets to the person is 1.0 m. By how much does the sound intensity vary in terms of the ratio of the loudest to the softest sounds?

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An example

� A small speaker is placed in front of a block of mass 4 kg. Themass is attached to a Hooke’s Law sping with sping constant 100 N/m. The mass and speaker have a mechanical energy of 200 J and are undergoing one dimensional simple harmonic motion. The speaker emits a 200 Hz tone. (vsound = 340 m/s)

� For a person is standing directly in front of the speaker, what range of frequencies does he/she hear?

Emech=200 J = ½ mvmax2 = ½ kA2 � vmax=10 m/s

Now use expression for Doppler shift wherevsource= + 10 m/s and – 10 m/s


An example � A small speaker is placed in front of a block of mass 4 kg. The

mass is attached to a Hooke’s Law sping with sping constant 100 N/m. The mass and speaker have a mechanical energy of 200 J and are undergoing one dimensional simple harmonic motion. The speaker emits a 200 Hz tone. (vsound = 340 m/s)

� The closest the speaker gets to the person is 1.0 m. By how much does the sound intensity vary in terms of the ratio of the loudest to the softest sounds?

Emech=200 J = ½ mvmax2 = ½ kA2 � A = 2.0 m

Distance varies from 1.0 m to 1.0+2A or 5 meters whereP is the power emitted

Ratio � Iloud/Isoft= (P/4π rloud2)/(P/4π rsoft

2) = 52/12 = 25

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An example problem� In musical instruments the sound is based

on the number and relative strengths of the harmonics including the fundamental frequency of the note. Figure 1a depicts the first three harmonics of a note. The sum of the first two harmonics is shown in Fig. 1b, and the sum of the first 3 harmonics is shown in Fig. 1c.

Which of the waves shown has the shortest period?

a. 1st Harmonicb. 2nd Harmonicc. 3rd Harmonicd. Figure 1cAt the 2nd position(1st is at t=0) where the three

curves intersect in Fig. 1a, the curves are all:

a. in phaseb. out of phasec. at zero displacementd. at maximum displacement

time

a

b

c

Figure 1: Wave superposition

disp

lace

men

t

time

disp

lace

men

ttime

disp

lace

men

t


An example problemThe frequency of the waveform shown in Fig.

1c is

a. the same as that of the fundamental

b. the same as that of the 2nd harmonic

c. the same as that of the 3rd harmonic

d. sum of the periods of the 1st, 2nd & 3rd

harmonics

Which of the following graphs most accurately reflects the relative amplitudes of the harmonics shown in Fig. 1?

time

a

b

c

Figure 1: Wave superposition

disp

lace

men

t

time

disp

lace

men

t

time

disp

lace

men

t

b

1 2 3harmonic

ampl

itude

1 2 3harmonic

ampl

itude

1 2 3harmonic

ampl

itude

1 2 3harmonic

ampl

itude

a

c d

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Chapter 1


Important Concepts

Page 15



Chapter 2


Chapter 3

Page 16



Chapter 4


Chapter 4

Page 17



Chapter 5


Chapter 5 & 6

Page 18



Chapter 6

Chapter 7


Chapter 7

Page 19



Chapter 7 (Newton’s 3 rd Law) & Chapter 8


Chapter 8

Chapter 9

Page 20



Chapter 9


Chapter 10

Page 21



Chapter 10


Chapter 10

Page 22



Chapter 11


Chapter 11

Page 23



Chapter 12

and Center of Mass


Chapter 12

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Important Concepts


Chapter 12

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Angular Momentum


Hooke’s Law Springs and a Restoring Force

� Key fact: ω = (k / m)½ is general result where k reflects a constant of the linear restoring force and m is the inertial response

(e.g., the “physical pendulum” where ω = (κ / I)½

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Simple Harmonic Motion

Maximum kinetic energy

Maximum potential energy


Resonance and damping

� Energy transfer is optimal when the driving force varies at the resonant frequency.

� Types of motion� Undamped� Underdamped� Critically damped� Overdamped

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Fluid Flow


Density and pressure

Page 28



Response to forces

States of Matter and Phase Diagrams


Ideal gas equation of state

Page 29



pV diagrams

Thermodynamics


T can change!

Work, Pressure, Volume, Heat

Page 30



Chapter 18


Thermal Energy

Page 31



Relationships


Chapter 19

Page 32



Refrigerators


Carnot Cycles

Page 33



Work (by the system)


Chapter 20

Page 34



Displacement versus time and position


Sinusoidal Waves (Sound and Electromagnetic)

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Doppler effect


Chapter 21

Page 36



Standing Waves


Beats

/1|| /1||

)2cos()2cos(2),0(

avgavg2beatbeat21

22

21

2121

TfTfff

ttAtDff

ffff

=≡=≡−

=+

+− ππ

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Lecture 29, Dec. 10

•• AssignmentAssignment� HW12, Due Friday, Dec. 12th

I hope everyone does well on their finals!Have a great break!

Documents

Physics 207 – Lecture 29 Lecture 29, Dec. 10 Room 5208 ... · Page 10 Physics 207 – Lecture 29 Physics 207: Lecture 29, Pg 19 An example A monatomic gas is compressed isothermally