Chapter VII Periodic Motions

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Chapter VII Periodic Motions A. Periodic Motion B. Simple Harmonic Motion C. Energy of The Simple Harmonic Oscillator D. Simple Pendulum

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Chapter VII Periodic Motions. Periodic Motion Simple Harmonic Motion Energy of The Simple Harmonic Oscillator Simple Pendulum. A. Periodic Motion. - PowerPoint PPT Presentation

Transcript of Chapter VII Periodic Motions

Page 1: Chapter VII Periodic Motions

Chapter VIIPeriodic MotionsA. Periodic MotionB. Simple Harmonic MotionC. Energy of The Simple Harmonic OscillatorD. Simple Pendulum

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A. Periodic Motion

The amplitude of the motion, denoted by A, is the maximum magnitude of displacement from equilibrium-that is, the maximum value of Ixl. It is always positive.

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• A complete vibration, or cycle, is one complete round trip say, from A to -A and back to A, or from 0 to A, back through 0 to -A, and back to O.

• The period, T, is the time for one cycle. It is always positive. The SI unit is the second, but it is sometimes expressed as "seconds per cycle."

• The frequency, f, is the number of cycles in a unit of time. It is always positive. The SI unit of frequency is the hertz.

1 hertz = I Hz = 1 cycle/s = 1 S-l

The angular frequency (rad/s), , is 2 times the frequency (cycle/s): = 2 f The number 2 as having units rad/cycle.

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B. Simple Harmonic Motion

The minus sign means the acceleration and displacemem always have opposite signs.

= phase angle(t + ) = Phase

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The frequency and period depend only on the mass of the block and on the force constant of the spring

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C. Energy of The Simple Harmonic Oscillator

• The total mechanical energy of a simple harmonic oscillator is a constant of the motion and is proportional to the square of the amplitude.

• Note, that U is small when K is large, and vice versa, because the sum must be constant.

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D. Simple Pendulum

x

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• The period and frequency of a simple pendulum depend only on the length of the string and the acceleration due to gravity.

• Because the period is independent of the mass, we conclude that all simple pendulums that are of equal length and are at the same location (so that g is constant) oscillate with the same period.