Topic 4 – Oscillations and Waves
4.2 Damped and Forced Harmonic Motion
Damped
● In SHM there is only the one restoring force
acting in the line of the displacement.
● In damped harmonic motion (DHM) an
additional damping force acts in the opposite
direction to the velocity of the object to
dissipate energy and stop the vibrations.
Damping Forces
● The damping force acts so as to cause the amplitude of the
vibrations to decay naturally dissipating energy.
● The general equation of this decay is A=A0
e-ˠt
● Here ˠ is a damping factor.
● The system can be under-damped
● This means the system can make more than one full oscillation
before it comes to a stop.
● The system can be over-damped
● The system comes to a stop before it completes one oscillation
● The system can be critically-damped
● The system completes exactly one oscillation before stopping.
Damping Forces
Damping Forces (beyond Syllabus)
● The general equations governing the motion of
a damped harmonic oscillation are:
x=x0 e
−γ t
cos(ωt+ ϕ)
v=−x0(γ e
−γ t
cos(ωt+ ϕ)+ ωe
−γ t
sin(ωt+ ϕ))
a=−x0 (−γ2
e−γ t
cos(ωt+ ϕ)+ ω2
e− γt
cos(ωt+ ϕ))
Natural Frequency
● The frequency with which a system oscillates if
it is started and allowed to move freely is called
its natural frequency.
● Simple harmonic motion occurs at the natural
frequency.
● Often, extra energy is imparted into the system
each oscillation by another external periodic
force.
● This is like a child pushing a swing to keep it going.
● Such a system is said to be a forced harmonic
oscillator.
Forced Harmonic Motion
● The equation for forced harmonic motion (with
some damping) would be:
● Here the first part of the equation is the normal
SHM equation with natural frequency ω0
and
amplitude x0
● The second part of the equation is due to the
forcing (driving) force of magnitude F and
driving frequency ω
x=x0e
− γt
cos(ω0t)+
F
mω
2
cos(ωt)
Forced Harmonic Motion and Resonance
● As the driving frequency of the system
approaches the natural frequency of the
system, the amplitude of the system increases
dramatically.
● The force adds energy to each swing making
the amplitude continue to increase and
increase.
● When the two frequencies are identical, then
the system is said to be at resonance.
Resonance
● The state in which the frequency of the
externally applied periodic force equals the
natural frequency of the system is called
resonance.
● This causes oscillations with large amplitudes.
● Damping causes the maximum amplitude to be
limited.
Resonance
-5 0
1 9 5 0
3 9 5 0
5 9 5 0
7 9 5 0
9 9 5 0
1 1 9 5 0
1 3 9 5 0
0 5 1 0 1 5 2 0 2 5 3 0 3 5 4 0 4 5 5 0
MaximumAmplitude
D r iv in g F r e q u e n c y
V e r y L ig h t d a m p in g
L ig h t d a m p in g
M e d iu m D a m p in g
H e a v y D a m p in g
Dangerous Resonance
● Resonance can be
disastrous
● If a bridge happens to
have a natural frequency
that is in the range of the
frequencies that can be
generated by the wind
then the bridge can
oscillate.
● The bridge can then
vibrate it can collapse!
● This is resonance at its
worst!!!
Useful Resonance
● Resonance can be useful.
● A radio is tuned by causing a quartz crystal to
resonate at a particular frequency.
● Wind instruments rely on the resonance of a
vibrating air column to make an audible sound.
– Because of the sharp spike on the frequency response
curve, other frequencies are cancelled out and not heard.

4.2 damped harmonic motion

  • 1.
    Topic 4 –Oscillations and Waves 4.2 Damped and Forced Harmonic Motion
  • 2.
    Damped ● In SHMthere is only the one restoring force acting in the line of the displacement. ● In damped harmonic motion (DHM) an additional damping force acts in the opposite direction to the velocity of the object to dissipate energy and stop the vibrations.
  • 3.
    Damping Forces ● Thedamping force acts so as to cause the amplitude of the vibrations to decay naturally dissipating energy. ● The general equation of this decay is A=A0 e-ˠt ● Here ˠ is a damping factor. ● The system can be under-damped ● This means the system can make more than one full oscillation before it comes to a stop. ● The system can be over-damped ● The system comes to a stop before it completes one oscillation ● The system can be critically-damped ● The system completes exactly one oscillation before stopping.
  • 4.
  • 5.
    Damping Forces (beyondSyllabus) ● The general equations governing the motion of a damped harmonic oscillation are: x=x0 e −γ t cos(ωt+ ϕ) v=−x0(γ e −γ t cos(ωt+ ϕ)+ ωe −γ t sin(ωt+ ϕ)) a=−x0 (−γ2 e−γ t cos(ωt+ ϕ)+ ω2 e− γt cos(ωt+ ϕ))
  • 6.
    Natural Frequency ● Thefrequency with which a system oscillates if it is started and allowed to move freely is called its natural frequency. ● Simple harmonic motion occurs at the natural frequency. ● Often, extra energy is imparted into the system each oscillation by another external periodic force. ● This is like a child pushing a swing to keep it going. ● Such a system is said to be a forced harmonic oscillator.
  • 7.
    Forced Harmonic Motion ●The equation for forced harmonic motion (with some damping) would be: ● Here the first part of the equation is the normal SHM equation with natural frequency ω0 and amplitude x0 ● The second part of the equation is due to the forcing (driving) force of magnitude F and driving frequency ω x=x0e − γt cos(ω0t)+ F mω 2 cos(ωt)
  • 8.
    Forced Harmonic Motionand Resonance ● As the driving frequency of the system approaches the natural frequency of the system, the amplitude of the system increases dramatically. ● The force adds energy to each swing making the amplitude continue to increase and increase. ● When the two frequencies are identical, then the system is said to be at resonance.
  • 9.
    Resonance ● The statein which the frequency of the externally applied periodic force equals the natural frequency of the system is called resonance. ● This causes oscillations with large amplitudes. ● Damping causes the maximum amplitude to be limited.
  • 10.
    Resonance -5 0 1 95 0 3 9 5 0 5 9 5 0 7 9 5 0 9 9 5 0 1 1 9 5 0 1 3 9 5 0 0 5 1 0 1 5 2 0 2 5 3 0 3 5 4 0 4 5 5 0 MaximumAmplitude D r iv in g F r e q u e n c y V e r y L ig h t d a m p in g L ig h t d a m p in g M e d iu m D a m p in g H e a v y D a m p in g
  • 11.
    Dangerous Resonance ● Resonancecan be disastrous ● If a bridge happens to have a natural frequency that is in the range of the frequencies that can be generated by the wind then the bridge can oscillate. ● The bridge can then vibrate it can collapse! ● This is resonance at its worst!!!
  • 12.
    Useful Resonance ● Resonancecan be useful. ● A radio is tuned by causing a quartz crystal to resonate at a particular frequency. ● Wind instruments rely on the resonance of a vibrating air column to make an audible sound. – Because of the sharp spike on the frequency response curve, other frequencies are cancelled out and not heard.