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Whenever the force acting on an object is:
1. Proportional to the displacement
2. In the opposite direction,
the object exhibits simple harmonic motion
(SHM).
Examples
1. mass attached to a spring
2. simple pendulum.
Definitions of Terms
• Amplitude = A = the maximum displacement of
the moving object from its equilibrium position.
• Period = T = the time it takes the object to
complete one full cycle of motion.
• Frequency = f = the number of cycles or
vibrations per unit of time.
Vertical Spring
Mass Attached to a Spring
m x = 0 “Equilibrium Position”
x > 0
x < 0
x = displacement from
equilibrium
Period of an object on a vertical spring
exhibiting SHM is:
2
m
T
k


T = period
m = mass of object
K = spring constant
Force always opposite the displacement from equilibrium
 If we stretch a spring
with a mass on the end
and let it go, the mass
will oscillate back and
forth (if there is no
friction).
 This oscillation is called
Simple Harmonic
Motion, because F is a
restoring force.
Horizontal
Spring
F kx
 
As previously stated, a simple harmonic oscillator is any object
that oscillates and is subject to a restoring force. Example:
horizontal mass on the end of a spring. F is a linear restoring
force. Hooke’s law F= -kx applies
F
X
F kx
 
The frequency and period of the simple harmonic
oscillator are independent of the amplitude.
2
m
T
k


t
Sine or cosine curve representation of a restoring
force and simple harmonic motion.
2
m
T
k


Another View
2
m
T
k


Case 2 - The Simple Pendulum. A component of
the weight acts as the restoring force
Component of
weight restoring
mass to
equilibrium
mg sin
Period for The Simple Pendulum:
A pendulum is made by suspending a mass m at the end of a string
of length L. The period of oscillation for small displacements is
given by the following formula.
2
l
T
g


T = period
L = length
“g”= acceleration due to gravity
Period of a simple harmonic oscillator
representation in the form of a cosine curve.
T/4 = time for
quarter cycle
T/2 = time for
half cycle
3T/2 = time for three
quarters of a cycle
2
l
T
g


Simple Harmonic Motion and Circular Motion, compared
to circular motion
2
l
T
g


Energy in Simple Harmonic Motion
Simple Harmonic Motion.ppt

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Simple Harmonic Motion.ppt

  • 1. Whenever the force acting on an object is: 1. Proportional to the displacement 2. In the opposite direction, the object exhibits simple harmonic motion (SHM). Examples 1. mass attached to a spring 2. simple pendulum.
  • 2. Definitions of Terms • Amplitude = A = the maximum displacement of the moving object from its equilibrium position. • Period = T = the time it takes the object to complete one full cycle of motion. • Frequency = f = the number of cycles or vibrations per unit of time.
  • 3. Vertical Spring Mass Attached to a Spring m x = 0 “Equilibrium Position” x > 0 x < 0 x = displacement from equilibrium
  • 4. Period of an object on a vertical spring exhibiting SHM is: 2 m T k   T = period m = mass of object K = spring constant
  • 5. Force always opposite the displacement from equilibrium  If we stretch a spring with a mass on the end and let it go, the mass will oscillate back and forth (if there is no friction).  This oscillation is called Simple Harmonic Motion, because F is a restoring force. Horizontal Spring F kx  
  • 6. As previously stated, a simple harmonic oscillator is any object that oscillates and is subject to a restoring force. Example: horizontal mass on the end of a spring. F is a linear restoring force. Hooke’s law F= -kx applies F X F kx  
  • 7. The frequency and period of the simple harmonic oscillator are independent of the amplitude. 2 m T k  
  • 8. t Sine or cosine curve representation of a restoring force and simple harmonic motion. 2 m T k  
  • 10.
  • 11. Case 2 - The Simple Pendulum. A component of the weight acts as the restoring force Component of weight restoring mass to equilibrium mg sin
  • 12. Period for The Simple Pendulum: A pendulum is made by suspending a mass m at the end of a string of length L. The period of oscillation for small displacements is given by the following formula. 2 l T g   T = period L = length “g”= acceleration due to gravity
  • 13.
  • 14. Period of a simple harmonic oscillator representation in the form of a cosine curve. T/4 = time for quarter cycle T/2 = time for half cycle 3T/2 = time for three quarters of a cycle 2 l T g  
  • 15. Simple Harmonic Motion and Circular Motion, compared to circular motion 2 l T g  
  • 16. Energy in Simple Harmonic Motion