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15 • Oscillatory Motion - ECHSPhysics

15 • Oscillatory Motion - ECHSPhysics

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oscillator is at the equilibrium position x 0. The magnitude of the acceleration is a<br />

maximum at the turning points and zero at the equilibrium position.<br />

The kinetic energy and potential energy for a simple harmonic oscillator vary with<br />

time and are given by<br />

(<strong>15</strong>.19)<br />

(<strong>15</strong>.20)<br />

The total energy of a simple harmonic oscillator is a constant of the motion and is<br />

given by<br />

(<strong>15</strong>.21)<br />

The potential energy of the oscillator is a maximum when the oscillator is at its turning<br />

points and is zero when the oscillator is at the equilibrium position. The kinetic energy<br />

is zero at the turning points and a maximum at the equilibrium position.<br />

A simple pendulum of length L moves in simple harmonic motion for small angular<br />

displacements from the vertical. Its period is<br />

(<strong>15</strong>.26)<br />

For small angular displacements from the vertical, a physical pendulum moves in<br />

simple harmonic motion about a pivot that does not go through the center of mass.<br />

The period of this motion is<br />

(<strong>15</strong>.28)<br />

where I is the moment of inertia about an axis through the pivot and d is the distance<br />

from the pivot to the center of mass.<br />

If an oscillator experiences a damping force R b v, its position for small damping<br />

is described by<br />

where<br />

(<strong>15</strong>.32)<br />

(<strong>15</strong>.33)<br />

If an oscillator is subject to a sinusoidal driving force F(t) F 0 sin t, it exhibits<br />

resonance, in which the amplitude is largest when the driving frequency matches the<br />

natural frequency of the oscillator.<br />

QUESTIONS<br />

K 1<br />

2 mv 2 1<br />

2 m 2A2 sin2 (t )<br />

U 1<br />

2 kx 2 1<br />

2 kA 2 cos2 (t )<br />

T 2 √ L<br />

g<br />

T 2 √ I<br />

mgd<br />

b<br />

<br />

x Ae 2m t cos(t )<br />

√ k<br />

E 1<br />

2 kA2<br />

m<br />

b<br />

2m 2<br />

1. Is a bouncing ball an example of simple harmonic motion?<br />

Is the daily movement of a student from home to school<br />

and back simple harmonic motion? Why or why not?<br />

2.<br />

If the coordinate of a particle varies as x A cos t,<br />

what is the phase constant in Equation <strong>15</strong>.6? At what position<br />

is the particle at t 0?<br />

3. Does the displacement of an oscillating particle between<br />

t 0 and a later time t necessarily equal the position of<br />

the particle at time t ? Explain.<br />

4. Determine whether or not the following quantities can be<br />

in the same direction for a simple harmonic oscillator:<br />

(a) position and velocity, (b) velocity and acceleration,<br />

(c) position and acceleration.<br />

Questions 475<br />

5. Can the amplitude A and phase constant be determined<br />

for an oscillator if only the position is specified at t 0?<br />

Explain.<br />

6. Describe qualitatively the motion of a block–spring system<br />

when the mass of the spring is not neglected.<br />

7. A block is hung on a spring, and the frequency f of the oscillation<br />

of the system is measured. The block, a second<br />

identical block, and the spring are carried in the Space<br />

Shuttle to space. The two blocks are attached to the ends<br />

of the spring, and the system is taken out into space on a<br />

space walk. The spring is extended, and the system is released<br />

to oscillate while floating in space. What is the frequency<br />

of oscillation for this system, in terms of f ?

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