More Oscillations Physics 202 Professor Vogel (Professor Carkner’s notes, ed) Lecture 3.
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Transcript of More Oscillations Physics 202 Professor Vogel (Professor Carkner’s notes, ed) Lecture 3.
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More Oscillations
Physics 202Professor Vogel (Professor Carkner’s
notes, ed)Lecture 3
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Amplitude, Period and Phase
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Phase The phase of SHM is the quantity
in parentheses, i.e. cos(phase) The difference in phase between 2
SHM curves indicates how far out of phase the motion is
The difference/2 is the offset as a fraction of one period Example: SHO’s = & =0 are offset
1/2 period They are phase shifted by 1/2 period
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SHM and Energy
A linear oscillator has a total energy E, which is the sum of the potential and kinetic energies (E=U+K)U and K change as the mass oscillatesAs one increases the other decreasesEnergy must be conserved
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SHM Energy Conservation
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Potential Energy
Potential energy is the integral of force
From our expression for xU=½kxm
2cos2(t+)
2kx21kxdxFdxU
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Kinetic Energy
Kinetic energy depends on the velocity,
K=½mv2 = ½m2xm2 sin2(t+)
Since 2=k/m, K = ½kxm
2 sin2(t+)The total energy E=U+K which will
give:E= ½kxm
2
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Pendulums
A mass suspended from a string and set swinging will oscillate with SHM We will first consider a simple pendulum
where all the mass is concentrated in the mass at the end of the string
Consider a simple pendulum of mass m and length L displaced an angle from the vertical, which moves it a linear distance s from the equilibrium point
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The Period of a Pendulum
The the restoring force is:F = -mg sin
For small angles sin We can replace with s/L
F=-(mg/L)s Compare to Hooke’s law F=-
kx k for a pendulum is (mg/L)
Period for SHM is T = 2 (m/k)½
T=2(L/g)½
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Pendulum and Gravity
The period of a pendulum depends only on the length and g, not on mass A heavier mass requires more force to
move, but is acted on by a larger gravitational force
A pendulum is a common method of finding the local value of g Friction and air resistance need to be
taken into account
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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 attached to weights that try to
turn it The gear is stopped by a toothed mechanism
attached to a pendulum of period = 2 seconds The mechanism disengages when the
pendulum is in the equilibrium position and so allows the second hand to move twice per cycle
Since the period is 2 seconds the second hand advances once per second
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Physical Pendulum
Real pendulums do not have all of their mass at one point
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:
T=2(I/mgh)½
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Non-Simple Pendulum
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Uniform Circular Motion
Simple harmonic motion is uniform circular motion seen edge on
Consider a particle moving in a circle with the origin at the center Viewed edge-on the particle seems to be
moving back and forth between 2 extremes around the origin
The projection of the displacement, velocity and acceleration onto the edge-on circle are described by the SMH equations
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Uniform Circular Motion and SHM
x-axis
y-axis
xm angle =t+
Particle movingin circle of radius xm
viewed edge-on:
cos (t+)=x/xm
x=xm cos (t+) x(t)=xm cos (t+)
Particle at time t
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Observing the Moons of Jupiter
Galileo was the first person to observe the sky with a telescope in a serious way
He discovered the 4 inner moons of Jupiter Today known as the Galilean moons
He (and we) saw the orbit edge-on
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Jupiter and Moons
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Apparent Motion of Callisto