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Simple Harmonic Motion
Physics 202Professor Vogel (Professor Carkner’s
notes, ed)Lecture 2
Simple Harmonic Motion Any motion that repeats itself in a sinusoidal
fashion e.g. a mass on a spring
A mass that moves between +xm and -xm with period T
Properties vary from a positive maximum to a negative minimum Position (x) Velocity (v) Acceleration (a)
The system undergoing simple harmonic motion (SHM) is a simple harmonic oscillator (SHO)
SHM Snapshots
Key Quantities Frequency (f) -- number of complete
oscillations per unit time Unit=hertz (Hz) = 1 oscillation per second = s-1
Period (T) -- time for one complete oscillation T=1/f
Angular frequency () -- = 2f = 2/T Unit = radians per second (360 degrees = 2
radians) We use angular frequency because the
motion cycles
Equation of Motion
What is the position (x) of the mass at time (t)?
The displacement from the origin of a particle undergoing simple harmonic motion is:
x(t) = xmcos(t + ) Amplitude (xm) -- the maximum displacement
from the center Phase angle () -- offset due to not starting at
x=xm (“start” means t=0) Remember that (t+) is in radians
SHM Formula Reference
SHM in Action Consider SHM with =0:
x = xmcos(t) Remember =2/T
t=0, t=0, cos (0) = 1 x=xm
t=1/2T, t=, cos () = -1 x=-xm
t=T, t=2, cos (2) = 1 x=xm
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
Amplitude, Period and Phase
Velocity If we differentiate the equation for
displacement w.r.t. time, we get velocity: v(t)=-xmsin(t + )
Why is velocity negative?Since the particle moves from +xm to -xm the
velocity must be negative (and then positive in the other direction)
Velocity is proportional to High frequency (many cycles per second)
means larger velocity
Acceleration
If we differentiate the equation for velocity w.r.t. time, we get acceleration
a(t)=-xmcos(t + )This equation is similar to the
equation for displacementMaking a substitution yields:
a(t)=-2x(t)
x, v and a Consider SMH with =0:
x = xmcos(t) v = -xmsin(t) = -vmsin(t)
a = -xmcos(t) = -amcos(t) When displacement is
greatest (cos(t)=1), velocity is zero and acceleration is maximum Mass is momentarily at rest,
but being pulled hard in the other direction
When displacement is zero (cos(t)=0), velocity is maximum and acceleration is zero Mass coasts through the middle
at high speed
Force Remember that: a=-2x But, F=ma so,
F=-m2x Since m and are constant we can write the
expression for force as: F=-kx
Where k=m2 is the spring constant This is Hooke’s Law Simple harmonic motion is motion where force is
proportional to displacement but opposite in sign Why is the sign negative?
Linear Oscillator
A simple 1-dimensional SHM system is called a linear oscillator Example: a mass on a spring
In such a system, k=m2
We can thus find the angular frequency and the period as a function of m and k
mk
ωkm
2πT
Linear Oscillator
Application of the Linear Oscillator: Mass in Free
Fall A normal spring scale does not work in the absence of gravity
However, for a linear oscillator the mass depends only on the period and the spring constant:
T=2(m/k)0.5
m/k=(T/2)2
m=T2k/42
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
SHM Energy Conservation
Potential Energy
Potential energy is the integral of force
From our expression for xU=½kxm
2cos2(t+)
2kx21kxdxFdxU
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
Next Time
Read: 15.4-15.6