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Damped Harmonic
Oscillator
Kamran Ansari02–01-2018
Content
• Simple harmonic oscillator (SHM),
• Damped harmonic oscillator
• Over damped,
• Under damped,
• Critical damped
• Application of damped oscillator.
Simple harmonic oscillator
The spring exerts a restoring force for small
displacement x,
𝑭 = −𝑘𝒙
The equation of motion,
𝑥 +
𝑘
𝑚
𝑥 = 0
and the solution is,
𝑥 = 𝐴 𝑐𝑜𝑠(𝜔0 𝑡 + 𝜑)
𝜔0 = natural frequency =
𝑘
𝑚
𝜑 = phase difference
Damped harmonic oscillator
The spring’s restoring force and
frictional force exert opposite
force,
𝑭 = −𝑘𝒙 − 𝑏 𝒙
𝑚 𝒙 = −𝑘𝒙 − 𝑏 𝒙
The equation of motion,
𝒙 + 𝛾 𝑥 + 𝜔0
2
𝒙 = 0
γ = damping coefficient =
𝑏
𝑚
−𝒃 𝒙
Solution of the equation,
𝑥 𝑡 = 𝑐1 𝑒
−
𝛾
2
+
𝛾
2
2
−𝜔0
2 𝑡
+ 𝑐2 𝑒
−
𝛾
2
−
𝛾
2
2
−𝜔0
2 𝑡
(a) Over damped,
𝜸
𝟐
> 𝝎 𝟎
The system comes to its equilibrium state without oscillating,
𝒙
𝒙 𝟎
(b) Under damped,
𝜸
𝟐
< 𝝎 𝟎
The system comes to tis equilibrium state after some oscillations
𝑥 𝑡 = 𝑥0 𝑒−
𝛾
2
𝑡
cos(𝜔′ 𝑡 + 𝜑) 𝑤ℎ𝑒𝑟𝑒 𝜔′
= 𝜔0
2 −
𝛾
2
2
𝑒−
𝛾
2 𝑡
(c) Critically damped,
𝜸
𝟐
= 𝝎 𝟎
The system comes to its equilibrium state most quickly,
𝑥 𝑡 = (𝑐1 + 𝑐2 𝑡)𝑒−
𝛾
2 𝑡
𝒙
𝒙 𝟎
Application of Damped harmonic
oscillator
• Car suspension system
Thank you

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Damped harmonic oscillator

  • 2. Content • Simple harmonic oscillator (SHM), • Damped harmonic oscillator • Over damped, • Under damped, • Critical damped • Application of damped oscillator.
  • 3. Simple harmonic oscillator The spring exerts a restoring force for small displacement x, 𝑭 = −𝑘𝒙 The equation of motion, 𝑥 + 𝑘 𝑚 𝑥 = 0 and the solution is, 𝑥 = 𝐴 𝑐𝑜𝑠(𝜔0 𝑡 + 𝜑) 𝜔0 = natural frequency = 𝑘 𝑚 𝜑 = phase difference
  • 4. Damped harmonic oscillator The spring’s restoring force and frictional force exert opposite force, 𝑭 = −𝑘𝒙 − 𝑏 𝒙 𝑚 𝒙 = −𝑘𝒙 − 𝑏 𝒙 The equation of motion, 𝒙 + 𝛾 𝑥 + 𝜔0 2 𝒙 = 0 γ = damping coefficient = 𝑏 𝑚 −𝒃 𝒙
  • 5. Solution of the equation, 𝑥 𝑡 = 𝑐1 𝑒 − 𝛾 2 + 𝛾 2 2 −𝜔0 2 𝑡 + 𝑐2 𝑒 − 𝛾 2 − 𝛾 2 2 −𝜔0 2 𝑡 (a) Over damped, 𝜸 𝟐 > 𝝎 𝟎 The system comes to its equilibrium state without oscillating, 𝒙 𝒙 𝟎
  • 6. (b) Under damped, 𝜸 𝟐 < 𝝎 𝟎 The system comes to tis equilibrium state after some oscillations 𝑥 𝑡 = 𝑥0 𝑒− 𝛾 2 𝑡 cos(𝜔′ 𝑡 + 𝜑) 𝑤ℎ𝑒𝑟𝑒 𝜔′ = 𝜔0 2 − 𝛾 2 2 𝑒− 𝛾 2 𝑡
  • 7. (c) Critically damped, 𝜸 𝟐 = 𝝎 𝟎 The system comes to its equilibrium state most quickly, 𝑥 𝑡 = (𝑐1 + 𝑐2 𝑡)𝑒− 𝛾 2 𝑡 𝒙 𝒙 𝟎
  • 8.
  • 9. Application of Damped harmonic oscillator • Car suspension system
  • 10.