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solution of damped oscillation D.E.

 
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Jul29-12, 02:03 PM   #1
 

solution of damped oscillation D.E.


d2x + 2Kdx + w0 2 x(t) = 0
dt dt


while solving this we assume the solution to be of form x = f(t)e-kt

why is this exponential taken???
 
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Aug1-12, 06:42 AM   #2
 
Because the solution to the equation is known to be of this form! You are, if you like, assuming the form of the answer in advance! This is quite a common procedure in 'solving' differential equations.

If your physical intuition is good, you could identify the [itex]2k\frac{dx}{dt}[/itex] term as due to a resistive force, and guess that there'd be an exponential decay factor in the solution.

Once you've made the substitution [itex]x = e^{-kt} f(t)[/itex], you have a differential equation for [itex]f(t)[/itex], which is just the ordinary shm equation with angular frequency [itex]\omega[/itex] given by [itex]\omega^2 = \omega_0^2 - k^2[/itex], provided that [itex]\omega > k[/itex]. So the solution can be seen immediately, by elementary methods, to be the product of sinusoidally oscillating, and exponential damping, factors. [If [itex]\omega < k[/itex] we have a non-oscillatory fall-off in x with time.]

Making the substitution [itex]x = e^{-kt} f(t)[/itex] involves a bit of drudgery and, imo, one might as well go the whole hog and (if [itex]\omega > k[/itex]) make the substitution [itex]x=Ae^{-kt}sin ({\omega t + \epsilon})[/itex] at the outset. You'll find that this expression does fit, provided that [itex]\omega^2 = \omega_0^2 - k^2[/itex].

If you're happy with complex numbers, and the idea of linear combinations, there is a very slick method which simply requires you to substitute [itex]x=Ae^{-\alpha t}[/itex]. Alpha turns out to be complex if [itex]\omega > k[/itex], and you need to form a linear combinations of two solutions. The mathematics is a bit more advanced than that needed for the substitution [itex]x = e^{-kt} f(t)[/itex] or [itex]x=Ae^{-kt}sin ({\omega t + \epsilon})[/itex].
 
Aug4-12, 06:11 AM   #3
 
In previous post [itex]\omega > k[/itex] should read [itex]\omega_0 > k[/itex], and [itex]\omega < k[/itex] should read [itex]\omega_0 < k[/itex]. Sorry.
 
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