What is realy the idea of damped simple harmonic motion?

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SUMMARY

Damped simple harmonic motion (SHM) describes oscillating systems where dissipative forces cause amplitude reduction over time. The mathematical representation of damped motion is given by the equation Ae^(-(b/m)t) cos(w’t + phi), where "b" is the damping factor. Critical damping occurs when b equals 2sqrt(km), resulting in no oscillation and a return to equilibrium, which is crucial for systems like automobile suspensions. Understanding these concepts is essential for analyzing real-world oscillatory systems.

PREREQUISITES
  • Understanding of basic harmonic motion principles
  • Familiarity with exponential decay functions
  • Knowledge of damping factors in mechanical systems
  • Basic algebra and calculus for manipulating equations
NEXT STEPS
  • Study the mathematical derivation of damped harmonic motion equations
  • Explore critical damping and its applications in engineering
  • Learn about the role of damping in automobile suspension systems
  • Investigate the differences between underdamping, overdamping, and critical damping
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Students of physics, mechanical engineers, and anyone interested in the dynamics of oscillating systems and their practical applications in real-world scenarios.

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i am finding damped SHM difficult to understand can anyone give sugestion as to what coul .do
 
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Damped functions

Nearly all real world oscillating systems have some dissipatives forces. Therefore, their oscillations die out over time-unless we provide some means for replacing the dissipating mechanism. The decrease in amplitude caused by these frictional forces is called damping-and the corresponding motion is called damped oscillation.

One can view the automobile suspension system as an oscillating system, which if not damped, would keep bobbing up and down for ever, whenever it bumped. The damped function would be an “exponential rate of decay equation x cos (w’t + phi).”

ie Ae^(-(b/m)t) cos (w’t + phi) (1)

Where w = sqrt (k/m – b^2/4m^2) (2)

w’ is the angular frequency.

The exp rate of decay is the amplitude (friction) and decreases with time because of the exponential factor e^(-(b/m)t). Note the negative sign in eq 1.

“b” is the damping factor here. We want to make it large in this case. Look at the b^2 fraction. As b becomes large, eg the shocks pads wear out, the system: cos (sqrt (k/m – b^2/4m^2)t + phi) returns to equilibrium: cos (sqrt (k/m )).

w becomes zero when b becomes large. (k/m – b^2/4m^2)=0
ie b=2sqrt(km)

When eq 2 is in 1, it is called critical damping. The system no longer oscillates when it is disturbed (eg car goes over a bump.) So we want critical damping, or underdamping for best passagenger safety.

If b is greater than 2sqrt(km) = overdamping, no oscill. just a return to equilibrium more slowly.

Hope this is a start.
 
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