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© JParkinson 1
© JParkinson 2
© JParkinson 3
© JParkinson 4
ALL INVOLVE
SIMPLE HARMONIC MOTION
© JParkinson 5
A body will undergo SIMPLE HARMONIC MOTION when the force that tries to restore the object to its REST POSITION is PROPORTIONAL TO the DISPLACEMENT of the object.
A pendulum and a mass on a spring both undergo this type of motion which can be described by a SINE WAVE or a COSINE
WAVE depending upon the start position.
Displacement x
Time t
+ A
- A
ftAx 2cos
© JParkinson 6
SHM is a particle motion with an acceleration (a) that is directly proportional to the particle’s displacement (x) from a fixed point (rest point), and this acceleration always points towards the fixed point.
Rest point
x
AAx
xa or xa 2
© JParkinson 7
Displacement x
time
Amplitude ( A ): The maximum distance that an object moves from its rest position. x = A and x = - A .
+ A
- A
Period ( T ): The time that it takes to execute one complete cycle of its motion.Units seconds,
T
Frequency ( f ): The number or oscillations the object completes per unit time.Units Hz = s-1 .
Tf 1
Angular Frequency ( ω ): The frequency in radians per second, 2π per cycle.
Tf 22
© JParkinson 8
θr
Arc length s
IN RADIANSrs
FOR A FULL CIRCLE RADIANS 22
rr
© JParkinson 9
EQUATION OF SHM xa 2
x
a
Acceleration – Displacement graph xmy
Gradient = - ω2
+ A
- A
MAXIMUM ACCELERATION = ± ω2 A = ( 2πf )2 A
© JParkinson 10
EQUATION FOR VARIATION OF VELOCITY WITH DISPLACEMENT
+x-xx
v
222 xAfv
Maximum velocity, v = ± 2 π f A
Maximum Kinetic Energy, EK = ½ mv2 = ½ m ( 2 π f A )2
© JParkinson 11
Displacement x
Velocity v
Acceleration a
ftAx 2cos
t
t
t
txv
Velocity = gradient of displacement- time graph
Maximum velocity in the middle of the motion
ZERO velocity at the end of the motion
tva
Acceleration = gradient of velocity - time graph
Maximum acceleration at the end of the motion – where the restoring force is greatest!ZERO acceleration in the middle of the motion!
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THE PENDULUMThe period, T, is the time for one complete cycle.
glT 2
l
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MASS ON A SPRING
M
F = Mg = ke
e
Stretch & Release
A
kmT 2
geT 2k = the spring constant in N m-1
© JParkinson 14
http://www.explorelearning.com/index.cfm?method=cResource.dspView&ResourceID=44
The link below enables you to look at the factors that influence
the period of a pendulum and the period of a mass on a spring
© JParkinson 15
ENERGY IN SHM
potential
EP
Kinetic
EK
Potential
EP
PENDULUM SPRING
MM
M
potential
kineticpotential
If damping is negligible, the total energy will be constant
ETOTAL = Ep + EK
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Maximum velocity, v = ± 2 π f A
222 xAfvvelocity Energy in SHM
Maximum Kinetic Energy, EK = ½ m ( 2 π f A )2 = 2π2 m f2 A2
Hence TOTAL ENERGY = 2π2 m f2 A2
m
x = 0
F
For a spring,
m
x = A
energy stored = ½ Fx = ½ kx2, [as F=kx]
= MAXIMUM POTENTIAL ENERGY!
MAXIMUM POTENTIAL ENERGY = TOTAL ENERGY = ½ kA2
© JParkinson 17
Energy in SHM
Energy Change with POSITION
= kinetic = potential = TOTAL ENERGY, E
Energy Change with TIME
x-A +A0
energy E
energy
timeTT/2
N.B. Both the kinetic and the potential energies reach a maximum TWICE in on cycle.
E
© JParkinson 18
time
DAMPING
DISPLACEMENT
INITIAL AMPLITUDE
THE AMPLITUDE DECAYS EXPONENTIALLY WITH TIME