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Page 1: Damped Oscillations

Physics 1D03 - Lecture 35 1

Damped Oscillations

(Serway 15.6-15.7)

Page 2: Damped Oscillations

Physics 1D03 - Lecture 35 2

Simple Pendulum

L

θ T

Lg

dtd

2

2

mg

Recall, for a simple pendulum we have thefollowing equation of motion:

Which give us:Lg

Hence:2

2

2 4gTgL

Application - measuring height - finding variations in g → underground resources

or: 2

22 4

TLLg

-------------------------------------------------------------------------

Page 3: Damped Oscillations

Physics 1D03 - Lecture 35 3

t

x

x

t

SHM: x(t) = A cos ωt Motion continues indefinitely. Only conservative forces act, so the mechanical energy is constant.

Damped oscillator: dissipative forces (friction, air resistance, etc.) remove energy from the oscillator, and the amplitude decreases with time.

SHM and Damping

Page 4: Damped Oscillations

Physics 1D03 - Lecture 35 4

)cos()( 2

tAetxt

mb

For weak damping (small b), the solution is:

f = bv where b is a constant damping coefficient

x

t

A damped oscillator has external nonconservativeforce(s) acting on the system. A common example is a force that is proportional to the velocity.

eg: green water(weak damping)

A e-(b/2m)t

2

2

dtxdm

dtdxbkx F=ma give:

Page 5: Damped Oscillations

Physics 1D03 - Lecture 35 5

Without damping: the angular frequency is

22

0

2

22

mb

mb

mk

the amplitude gets smaller (decays exponentially) as time goes on:

mk0

With damping:

tmb

oeAtA 2)(

Effectively, the frequency ω is slower with damping, and

Page 6: Damped Oscillations

Physics 1D03 - Lecture 35 6

Example: A mass on a spring oscillates with initial amplitude 10 cm. After 10 seconds, the amplitude is 5 cm.

Question: What is the amplitude after 30 seconds?

Question: What is the value of b/(2m)?

Page 7: Damped Oscillations

Physics 1D03 - Lecture 35 7

Example: A pendulum of length 1.0 m has an initial amplitude 10°, but after a time of1000 s it is reduced to 5°. What is b/(2m)?

Page 8: Damped Oscillations

Physics 1D03 - Lecture 35 8

220 2

mb

water

axle grease?

Eg: Strong damping (b large): there is no oscillation when:

02

mb

Types of Damping

Since:

We can have different cases for the value underthe root: >0, 0 or <0. This leads to three types ofdamping !

Page 9: Damped Oscillations

Physics 1D03 - Lecture 35 9

02 mb

x(t)

t

overdamped

critical damping

underdamped

: “Overdamped”, no oscillation

: “Underdamped”, oscillations with decreasing amplitude

: “Critically damped”

Critical damping provides the fastest dissipation of energy.

02 mb

02 mb

Page 10: Damped Oscillations

Physics 1D03 - Lecture 35 10

Quiz: If you were designing a automobile suspensions:

Should they be:

a) Underdamped

b) Critically damped

c) Overdamped

d) I don’t need suspension !

Page 11: Damped Oscillations

Physics 1D03 - Lecture 35 11

Example:

Show that the time rate of change of mechanical energy for a damped oscillator is given by:

dE/dt=-bv2

and hence is always negative.

Page 12: Damped Oscillations

Physics 1D03 - Lecture 35 12

Damped Oscillations and Resonance

(Serway 15.6-15.7)

• Forced Oscillations• Resonance

Page 13: Damped Oscillations

Physics 1D03 - Lecture 35 13

Forced Oscillations

A periodic, external force pushes on the mass(in addition to the spring and damping):

tFtFext cos)( max

The frequency is set by the machine applying the force. The system responds by oscillating at the same frequency . The amplitude can be very large if the external driving frequency is close to the “natural” frequency of the oscillator.

This transfers energy into the system

Page 14: Damped Oscillations

Physics 1D03 - Lecture 35 14

is called the natural frequency or resonant frequency of the oscillation.m

k0

2

2

max cosdt

xdmdtdxbkxtFF

2

220

2

max

mb

mF

A

Newton’s 2nd Law:

Assume that : x = A cos (t + ) ; then the amplitude of a drive oscillator is given by:

Page 15: Damped Oscillations

Physics 1D03 - Lecture 35 15

So, as the amplitude, A, increases !

If the external “push” has the same frequency as the resonant frequency ω0. The driving force is said to be in resonance with the system.

0

0

A

2

220

2

max

mb

mF

A

Page 16: Damped Oscillations

Physics 1D03 - Lecture 35 16

Resonance occurs because the driving force changes direction at just the same rate as the “natural” oscillation would reverse direction, so the driving force reinforces the natural oscillation on every cycle.

Quiz: Where in the cycle should the driving force be at its maximum value for maximum average power?

A) When the mass is at maximum x (displacement)

B) When the mass is at the midpoint (x = 0)

C) It matters not

Page 17: Damped Oscillations

Physics 1D03 - Lecture 35 17

Example

A 2.0 kg object attached to a spring moves without friction and is driven by an external force given by:

F=(3.0N)sin(8πt)

If the force constant of the spring is 20.0N/m, determine

a) the period of the motion

b) the amplitude of the motion

Page 18: Damped Oscillations

Physics 1D03 - Lecture 35 18

Page 19: Damped Oscillations

Physics 1D03 - Lecture 35 19

Summary

• An oscillator driven by an external periodic force will oscillate with an amplitude that depends on the driving frequency. The amplitude is large when the driving frequency is close to the “natural” frequency of the oscillator.

•For weak damping, the system oscillates, and the amplitude decreases exponentially with time.• With sufficiently strong damping, the system returns smoothly to equilibrium without oscillation.