A. T and v max both double. B. T remains the same and v max doubles.

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Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley An object on the end of a spring is oscillating in simple harmonic motion. If the amplitude of oscillation is doubled, how does this affect the oscillation period T and the object’s maximum speed v max ? A. T and v max both double. B. T remains the same and v max doubles. C. T and v max both remain the same. D. T doubles and v max remains the same. E. T remains the same and v max increases by a factor of . Q13.1

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Q13.1. An object on the end of a spring is oscillating in simple harmonic motion. If the amplitude of oscillation is doubled, how does this affect the oscillation period T and the object ’ s maximum speed v max ?. A. T and v max both double. B. T remains the same and v max doubles. - PowerPoint PPT Presentation

Transcript of A. T and v max both double. B. T remains the same and v max doubles.

Page 1: A.  T  and  v max  both double. B.  T  remains the same and  v max  doubles.

Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley

An object on the end of a spring is oscillating in simple harmonic motion. If the amplitude of oscillation is doubled, how does this affect the oscillation period T and the object’s maximum speed vmax?

A. T and vmax both double.

B. T remains the same and vmax doubles.

C. T and vmax both remain the same.

D. T doubles and vmax remains the same.

E. T remains the same and vmax increases by a factor of .

Q13.1

Page 2: A.  T  and  v max  both double. B.  T  remains the same and  v max  doubles.

Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley

An object on the end of a spring is oscillating in simple harmonic motion. If the amplitude of oscillation is doubled, how does this affect the oscillation period T and the object’s maximum speed vmax?

A. T and vmax both double.

B. T remains the same and vmax doubles.

C. T and vmax both remain the same.

D. T doubles and vmax remains the same.

E. T remains the same and vmax increases by a factor of .

A13.1

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Phase angle

Draw x(t) for a simple harmonic oscillator with A = 2m, T = 4s and the following three phase angles: f0 = 0, p/2, -p/2. Draw circular motion diagram to show initial conditions. Calculate the value of x(0) in the three situations to make sure your drawing is accurate.

Page 4: A.  T  and  v max  both double. B.  T  remains the same and  v max  doubles.

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This is an x-t graph for an object in simple harmonic motion.

A. t = T/4

B. t = T/2

C. t = 3T/4

D. t = T

Q13.2

At which of the following times does the object have the most negative velocity vx?

Page 5: A.  T  and  v max  both double. B.  T  remains the same and  v max  doubles.

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This is an x-t graph for an object in simple harmonic motion.

A. t = T/4

B. t = T/2

C. t = 3T/4

D. t = T

A13.2

At which of the following times does the object have the most negative velocity vx?

Page 6: A.  T  and  v max  both double. B.  T  remains the same and  v max  doubles.

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This is an x-t graph for an object in simple harmonic motion.

A. t = T/4

B. t = T/2

C. t = 3T/4

D. t = T

Q13.3

At which of the following times does the object have the most negative acceleration ax?

Page 7: A.  T  and  v max  both double. B.  T  remains the same and  v max  doubles.

Copyright © 2008 Pearson Education Inc., publishing as Pearson Addison-Wesley

This is an x-t graph for an object in simple harmonic motion.

A. t = T/4

B. t = T/2

C. t = 3T/4

D. t = T

A13.3

At which of the following times does the object have the most negative acceleration ax?

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SHO equations• A simple harmonic oscillator has an amplitude of 2 m and

oscillates with a period of 2s. What is its maximum velocity?• The SHO is started with a phase angle of f = p/2 with the same

period and amplitude. Draw the position vs. time graph.• The same SHO starts moving in the positive x direction starting

at x = 1m at t = 0s. What is the phase angle for this situation?

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Energy in SHM• Energy is conserved during SHM and the forms (potential and

kinetic) interconvert as the position of the object in motion changes.

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Energy in SHM II• Energy converts between kinetic and potential energy.

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A. t = T/8 B. t = T/4

C. t = 3T/8 D. t = T/2

E. more than one of the above

This is an x-t graph for an object connected to a spring and moving in simple harmonic motion.

Q13.7

At which of the following times is the kinetic energy of the object the greatest?

Page 12: A.  T  and  v max  both double. B.  T  remains the same and  v max  doubles.

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A. t = T/8 B. t = T/4

C. t = 3T/8 D. t = T/2

E. more than one of the above

This is an x-t graph for an object connected to a spring and moving in simple harmonic motion.

A13.7

At which of the following times is the kinetic energy of the object the greatest?

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Find velocity1) What is the velocity as a function of the position v(x) for a SHO glider with mass m and spring constant k?

Use conservation of energy

2) What is the maximum velocity of the glider? Compare this max velocity to your previous result to find w for a mass on a spring.

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Vibrations of molecules • Two atoms separated by their internuclear distance r can be

pondered as two balls on a spring. The potential energy of such a model is constructed many different ways. The Leonard–Jones potential shown as Equation 13.25 is sketched in Figure 13.20 below. The atoms on a molecule vibrate as shown in Example 13.7.

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Old carThe shock absorbers in my 1989 Mazda with mass 1000 kg are completely worn out (true). When a 980-N person climbs slowly into the car, the car sinks 2.8 cm. When the car with the person aboard hits a bump, the car starts oscillating in SHM. Find the period and frequency of oscillation.

How big of a bump (amplitude of oscillation) before you fly up out of your seat?

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Damped oscillations II

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Forced (driven) oscillations and resonance• A force applied “in synch” with a motion already in progress

will resonate and add energy to the oscillation (refer to Figure 13.28).

• A singer can shatter a glass with a pure tone in tune with the natural “ring” of a thin wine glass.

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Forced (driven) oscillations and resonance II• The Tacoma Narrows Bridge suffered spectacular structural failure after absorbing too much resonant energy (refer to Figure 13.29).