Chapter 13 Lecture Slide 13-1 Essential University Physics Richard Wolfson 2 nd Edition © 2012 Pearson Education, Inc. Oscillatory Motion
Chapter 13 Lecture
Slide 13-1
Essential University Physics Richard Wolfson
2nd Edition
© 2012 Pearson Education, Inc.
Oscillatory Motion
Slide 13-2 © 2012 Pearson Education, Inc.
In this lecture you’ll learn
• To describe the conditions
under which oscillatory
motion occurs
• To describe oscillatory motion
quantitatively in terms of
frequency, period, and
amplitude
• To explain simple harmonic
motion and why it occurs
universally in both natural and
technological systems
• To explain damped harmonic
motion and resonance
Slide 13-3 © 2012 Pearson Education, Inc.
Oscillatory Motion
• A system in oscillatory motion undergoes repeating,
periodic motion about a point of stable equilibrium.
• Oscillatory motion is characterized by – Its frequency f or period T=1/f.
– Its amplitude A, or maximum excursion from equilibrium.
• Shown here are position-versus-time graphs for two different oscillatory motions with the same period and amplitude.
Slide 13-4 © 2012 Pearson Education, Inc.
– The paradigm example is a mass
m on a spring of spring constant k.
• The angular frequency
= 2p for this system is
– In SHM, displacement is a
sinusoidal function of time:
– Any amplitude A is possible.
• In SHM, frequency doesn’t depend on amplitude.
Simple Harmonic Motion
• Simple harmonic motion (SHM) results when the force
or torque that tends to restore equilibrium is directly
proportional to the displacement from equilibrium.
w = k m
( ) cosx t A t
2
2
d xm kx
dt
Slide 13-5 © 2012 Pearson Education, Inc.
Quantities in Simple Harmonic Motion
• Angular frequency, frequency, period:
• Phase
– Describes the starting time of the displacement-versus-
time curve in oscillatory motion:
x(t) = Acos(t + )
w =
k
mf =
w
2p=
1
2p
k
mT =
1
f= 2p
m
k
Slide 13-6 © 2012 Pearson Education, Inc.
Velocity and Acceleration in SHM
• Velocity is the rate of
change of position:
• Acceleration is the rate of
change of velocity:
( ) sindx
v t A tdt
2( ) cosdv
a t A tdt
Slide 13-7 © 2012 Pearson Education, Inc.
Other Simple Harmonic Oscillators
• The torsional oscillator
– A fiber with torsional constant
provides a restoring torque.
– Frequency depends on and
rotational inertia:
w = k I
• Simple pendulum
– Point mass on massless cord of
length L:
w = g L
2
2sin
dI mgL mgL
dt
2I mL for point mass
Slide 13-8 © 2012 Pearson Education, Inc.
SHM and Circular Motion
• Simple harmonic motion can be viewed as one
component of uniform circular motion.
– Angular frequency in SHM is the same as angular
velocity in circular motion.
As the position vector traces out a
circle, its x– and y– components are
sinusoidal functions of time.
r
Slide 13-9 © 2012 Pearson Education, Inc.
Energy in Simple Harmonic Motion
• In the absence of nonconservative
forces, the energy of a simple
harmonic oscillator does not
change.
– But energy is transfered back and
forth between kinetic and potential
forms.
Slide 13-10 © 2012 Pearson Education, Inc.
Simple Harmonic Motion is Ubiquitous!
• That’s because most systems near stable
equilibrium have potential-energy curves that are
approximately parabolic.
– Ideal spring:
– Typical potential-energy curve of an arbitrary system: U = 1
2kx2 = 1
2mw 2x2
Slide 13-11 © 2012 Pearson Education, Inc.
Damped Harmonic Motion
• With nonconservative forces present, SHM gradually damps
out:
– Amplitude declines exponentially toward zero:
– For weak damping b, oscillations still occur at approximately the
undamped frequency
– With stronger damping, oscillations cease.
• Critical damping brings the system to equilibrium most quickly.
w = k m.
2( ) cos( )
bt mx t Ae t
(a) Underdamped, (b) critically damped,
and (c) overdamped oscillations.
2
2
d x dxm kx b
dt dt
Slide 13-12 © 2012 Pearson Education, Inc.
Driven Oscillations
• When an external force acts on an oscillatory system, we
say that the system is undergoing driven oscillation.
• Suppose the driving force is F0cosdt, where d is the
driving frequency, then Newton’s law is
• The solution is
where
0
k
m : natural frequency
0
2 2 2 2 2 2
0
( )( ) /d d
FA
m b m
2
02cos d
d x dxm kx b F t
dt dt
( ) cos( )dx t A t
Slide 13-13 © 2012 Pearson Education, Inc.
Resonance
• When a system is driven by an external force at near its
natural frequency, it responds with large-amplitude
oscillations.
– This is the phenomenon of resonance.
– The size of the resonant response increases as damping
decreases.
– The width of the resonance curve (amplitude versus
driving frequency) also narrows with lower damping.
Resonance curves for several
damping strengths; 0 is the
undamped natural frequency k/m.
Slide 13-14 © 2012 Pearson Education, Inc.
• Oscillatory motion is periodic motion that results from a
force or torque that tends to restore a system to
equilibrium.
• In simple harmonic motion (SHM), the restoring force or
torque is directly proportional to displacement.
– The mass-spring system is the paradigm simple harmonic
oscillator.
– Damped harmonic motion occurs when nonconservative forces act on the oscillating system.
– Resonance is a high-amplitude oscillatory response of a system driven at near its natural oscillation frequency.
Summary
w = k m
( ) cosx t A t