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Pendulums

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Physics 202 Professor Lee Carkner Lecture 4 The sweep of the pendulum had increased As a natural consequence its velocity was also much greater. – PowerPoint PPT presentation

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Title: Pendulums


1
Pendulums
  • Physics 202
  • Professor Lee Carkner
  • Lecture 4

The sweep of the pendulum had increased As a
natural consequence its velocity was also much
greater. --Edgar Allan Poe, The Pit and the
Pendulum
2
PAL 3 SHM
  • Equation of motion for SHM, pulled 10m from rest,
    takes 2 seconds to get back to rest
  • w 2p/T 0.79
  • How long to get ½ back
  • arccos(5/10)/0.79 t 1.3 seconds

3
PAL 3 SHM (cont.)
  • Max speed
  • v -wxm sin(wt)
  • v max when sin 1
  • Where is max v?
  • Max acceleration
  • a -w2xm cos(wt)
  • Where is max a?
  • The ends (max force from spring)

4
Simple Harmonic Motion
  • For motion with period T and angular frequency
    w 2p/T
  • v-wxmsin(wt f)
  • The force is represented as
  • where kspring constant mw2

5
SHM and Energy
  • A linear oscillator has a total energy E, which
    is the sum of the potential and kinetic energies
    (EUK)
  • As one goes up the other goes down

6
SHM Energy Conservation
7
Potential Energy
  • From our expression for x
  • U½kxm2cos2(wtf)

8
Kinetic Energy
  • K½mv2 ½mw2xm2 sin2(wtf)
  • K ½kxm2 sin2(wtf)
  • The total energy EUK which will give
  • E ½kxm2

9
Types of SHM
  • Every system of SHM needs a mass to store kinetic
    energy and something to store the potential
    energy (to provide the springiness)
  • There are three types of systems that we will
    discuss
  • Each system has an equivalent for k

10
Pendulums
  • A mass suspended from a string and set swinging
    will oscillate with SHM
  • Consider a simple pendulum of mass m and length L
    displaced an angle q from the vertical, which
    moves it a linear distance s from the equilibrium
    point

11
Pendulum Forces
12
Forces on a Pendulum
L
q
Tension
s
m
q
Restoring Force mg sin q
Gravity mg
13
The Period of a Pendulum
  • The the restoring force is
  • F -mg sin q
  • We can replace q with s/L
  • Compare to Hookes law F-kx
  • Period for SHM is T 2p (m/k)½
  • T2p(L/g)½

14
Pendulum and Gravity
  • The period of a pendulum depends only on the
    length and g, not on mass
  • A pendulum is a common method of finding the
    local value of g

15
The Pendulum Clock Invented in 1656 by Christiaan
Huygens, the pendulum clock was the first
timekeeping device to achieve an accuracy of 1
minute per day.
16
Application of a Pendulum Clocks
  • Since a pendulum has a regular period it can be
    used to move a clock hand
  • Consider a clock second hand attached to a gear
  • The gear is stopped by a toothed mechanism
    attached to a pendulum of period 2 seconds
  • Since the period is 2 seconds the second hand
    advances once per second

17
Physical Pendulum
  • Properties of a physical pendulum depend on its
    moment of inertia (I) and the distance between
    the pivot point and the center of mass (h),
    specifically
  • T2p(I/mgh)½

18
Non-Simple Pendulum
19
Torsion Pendulum
20
Torsion Pendulum
  • If the disk is twisted a torque is exerted to
    move it back due to the torsion in the wire
  • tkq
  • We can use this to derive the expression for the
    period
  • T2p(I/k)½
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