Solution of damped oscillation D.E.

In summary, when solving the differential equation d2x + 2Kdx + w0 2 x(t) = 0/dt, we assume the solution to be of the form x = f(t)e-kt. This is done because the form of the answer is known in advance and it helps in solving the equation. By making this substitution, we get a differential equation for f(t), which can be solved using ordinary shm equation with angular frequency ω given by ω2 = ω0 2 - k2, provided that ω > k. Making the substitution x = e-kt f(t) involves some tedious work, but it can also be simplified by using the substitution x=Ae-kt sin
  • #1
uday1236
3
0
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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  • #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].
 
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  • #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.
 

Related to Solution of damped oscillation D.E.

1. What is the equation for damped oscillation?

The equation for damped oscillation is given by m¨+kx¨+bx′=0, where m is the mass of the oscillating object, k is the spring constant, b is the damping coefficient, x is the displacement, and ′ denotes the first derivative with respect to time.

2. What are the types of solutions for damped oscillation?

There are three types of solutions for damped oscillation: underdamped, critically damped, and overdamped. The type of solution depends on the value of the damping coefficient b in relation to the mass m and spring constant k.

3. How do you solve a damped oscillation differential equation?

The general solution for a damped oscillation differential equation can be found by using the characteristic equation mλ^2+kλ+b=0. Depending on the type of solution, the values of λ can be determined and used to find the specific solution.

4. What is the role of damping in damped oscillation?

The damping coefficient b controls the amount of energy dissipated per unit time in a damped oscillation system. This determines the rate of decay of the oscillations and ultimately affects the type of solution for the differential equation.

5. How does the amplitude of oscillation change with damping?

The amplitude of oscillation decreases with increasing damping. In an underdamped system, the amplitude decreases exponentially with time. In a critically damped system, the amplitude decreases in a more gradual manner, and in an overdamped system, the amplitude approaches zero without oscillation.

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