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Damped and Forced Oscillations Introducing non- conservative forces § 14.7– 14.8

Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

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Page 1: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Damped and Forced Oscillations

Introducing non-conservative forces

§ 14.7–14.8

Page 2: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Damping Force

Such as viscous drag

v

Drag opposes motion: F = –bv

Page 3: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Poll Question

How does damping affect the oscillation frequency?

A. Damping increases the frequency.

B. Damping does not affect the frequency.

C. Damping decreases the frequency.

Page 4: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Damping Differential Equation

ma = –bv – kx

One general solution:

x(t) = Ae cos('t + )

–bt2m

where

' = km 4m2

b2–

Page 5: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Light Damping

x(t) = Ae cos('t + )

–bt2m

If ' > 0:

• Oscillates

• Frequency slower than undamped case

• Amplitude decreases over time

' = km 4m2

b2–

Page 6: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Critical Damping

If ' = 0:

x(t) = (C1 + C2t) e–at

• No oscillation

• If displaced, returns directly to equilibrium

' = km 4m2

b2–

Page 7: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Overdamping

• No oscillation

• If displaced, returns slowly to equilibrium

' = km 4m2

b2–

If ' is imaginary:

x(t) = C1 e–a t + C2 e–a t1 2

Page 8: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Energy in Damping

• Damping force –bv is not conservative

• Total mechanical energy decreases over time

• Power dE/dt = –bv2= F·v = –bv·v

Page 9: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Worksheet Problem

Your 1000-kg car is supported on four corners by identical springs with spring constant k = 10,000 N/m.

a) Find the natural frequency of oscillation of your car.

b) Find the damping constant your shock absorbers must have in order to critically damp its vibrations.

Page 10: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Forced Oscillation

Periodic driving force

F(t) = Fmax cos(dt)

Page 11: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Forced Oscillation

If no damping

If d = ', amplitude increases without bound

Page 12: Damped and Forced Oscillations Introducing non-conservative forces § 14.7–14.8

Resonance

If lightly damped:

greatest amplitude when d = '

Source: Young and Freedman, Fig. 13.28

Critical or over-damping (b ≥ 2 km):

no resonance