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Oscillations: motions that repeat themselves

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Title: PHYS 342: Modern Physics Author: Sonya and Bob Kaye Last modified by: megan pickett Created Date: 1/10/2003 7:53:36 PM Document presentation format – PowerPoint PPT presentation

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Title: Oscillations: motions that repeat themselves


1
XII. Periodic Motion
  • Introduction
  • Oscillations motions that repeat themselves
  • a) Swinging chandeliers, boats bobbing at anchor,
    oscillating guitar strings, pistons in car
    engines
  • Understanding periodic motion essential for later
    study of waves, sound, alternating electric
    currents, and light
  • 3. An object in periodic motion experiences
    restoring forces or torques that bring it back
    toward an equilibrium position
  • 4. Those same forces cause the object to
    overshoot the equilibrium position

2
XII.B. Simple Harmonic Motion (SHM)
  • 1. Definitions
  • Frequency (f) number of
  • oscillations that are completed
  • each second
  • f hertz Hz 1 oscillation per sec 1 s1
  • Period time for one complete oscillation (or
    cycle)
  • T 1/f (XII.B.1)

3
XII.B. Simple Harmonic Motion (SHM)
  • 2. Displacement x(t)
  • x(t) xmcos(wt f), where (XII.B.2)
  • xm Amplitude of the motion
  • (wt f) Phase of the motion
  • f Phase constant (or phase angle) depends
    on the initial displacement and velocity
  • w Angular frequency 2p/T 2pf
    (rad/s) (XII.B.3)
  • 3. Simple harmonic motion periodic motion is a
    sinusoidal function of time (represented by sine
    or cosine function)

4
XII.B. Simple Harmonic Motion (SHM)
  • 4. velocity of a particle moving with SHM
  • 5. The acceleration for SHM

(XII.B.4)
(XII.B.5)
5
XII.C. Force Law for SHM
  • From Newtons 2nd Law
  • F ma mw2x (XII.C.1)
  • This result (a restoring force that is
    proportional to the displacement but opposite in
    sign) is the same as Hookes Law for a spring
  • F kx, where k mw2 (XII.C.2)

(XII.C.4)
(XII.C.3)
6
XII.D. Energy in SHM
  • 1. Elastic potential energy
  • U 1/2kx2 1/2kxm2cos2(wt f) (XII.D.1)
  • 2. Kinetic energy
  • K 1/2mv2 1/2kxm2sin2(wt f) (XII.D.2)
  • Total mechanical energy E U K
  • E 1/2kxm2cos2(wt f) 1/2 kxm2sin2(wt f)
  • 1/2kxm2 (XII.D.3)

7
XII.E. Pendula
  1. A simple pendulum consists of a particle of mass
    m (bob) suspended from one end of an
    unstretchable, massless string of length L that
    is fixed at the other end
  • Consider the Forces acting on the bob
  • Fq mgsinq mg(s/L) with
  • sinq s/L (XII.E.1)
  • If q is small (? 150 or so) then sinq ? q
  • Fq mgq mgs/L. (XII.E.2)

q
L
s

q
q
W mg
8
XII.E. Pendula
  1. A simple pendulum consists of a particle of mass
    m (bob) suspended from one end of an
    unstretchable, massless string of length L that
    is fixed at the other end
  • c) This equation is the angular equivalent of the
    condition for SHM (a w2 x), so
  • w (mg/L/ m)1/2 (g/L)1/2 and
    (XII.E.3)
  • T 2p(L/g)1/2 (XII.E.4)

9
Example Problem 12
  • A pendulum bob swings a total distance of 4.0 cm
    from end to end and reaches a speed of 10.0 cm/s
    at the midpoint. Find the period of oscillation.
  • xm 0.02 m vm 0.10 m/s
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