I Does the Amplitude of an Undamped Driven Oscillator Stay Constant Over Time?

AI Thread Summary
The discussion centers on the behavior of an undamped driven oscillator and whether its amplitude remains constant over time. It is established that when a driving force is applied, the amplitude can instantaneously become large, particularly as the driving frequency approaches the natural frequency. However, the amplitude is not an instantaneous quantity; it gradually increases until reaching a maximum value, influenced by initial conditions. In the absence of damping, the oscillations theoretically persist indefinitely, but in practical scenarios, damping affects the final energy level and amplitude stabilization. Ultimately, the relationship between driving frequency and natural frequency plays a crucial role in determining the oscillator's behavior over time.
adamjts
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The equations I'm getting when I solve the differential equations seem to imply that the amplitude of oscillation does not vary in time.

For example, if I have

x'' + ω02x = cos(ωt)

If we suppose that ω≠ω0,

then the general solution should look something like:

x(t) = c1cos(ω0t) + c2sin(ω0t) + (1/(ω022))cos(ωt)

This is okay with me mostly. But then thinking about what happens when ω→ω0 AND ω≠ω0, then obviously the amplitude of the oscillator should be huge. However, It would seem that the amplitude does not depend on time. Which is to say, that the exact moment that we introduce this driving force, the amplitude of the oscillator instantaneously becomes enormous. Which is hard to believe, because I would expect the object to start deviating from its simple oscillations more slowly and grow in time.

I know that when ω=ω0 that there is a factor of t in the amplitude, but that is not the case here.

The only explanation that I can think of so far is that the superposition of the two sinusoids makes it seem like the initial amplitudes are small. So when the driving force is introduced, the waves align such that the oscillating body does not seem to have a huge amplitude. But over some time, the waves will align such that the body does have evidently huge oscillations. This would imply, though, that the oscillations would become small again. In other words, we would expect long beats. Is this correct?

Or, maybe after the driver begins, the motion converges onto that of the driven oscillation?
 
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adamjts said:
If we suppose that ω≠ω0,
I'm in doubt of the terms. Do you mean that

  • ω0 is the undamped frequency
  • ω is the damped frequency
If the system is undamped , ω = ω0. If you "drive" the system ( add/subtract energy ), the system is not undamped any longer.

And, yes, if you add energy to an undamped system, the accumulated energy will result in an enormous amplitude, and ω ≠ ω0.
 
adamjts said:
Which is to say, that the exact moment that we introduce this driving force, the amplitude of the oscillator instantaneously becomes enormous. Which is hard to believe, because I would expect the object to start deviating from its simple oscillations more slowly and grow in time.
The amplitude is not an instantaneous quantity. If the initial conditions are x=0 and v=0, then displacement increases gradually until it reaches a maximum value. That maximum value is the amplitude.
If you have damping, the oscillation stabilizes after a while to a steady state with the frequency of the driving force.
If there is no damping the transients (oscillations with natural frequency) should stay forever, theoretically.
 
adamjts said:
It would seem that the amplitude does not depend on time. Which is to say, that the exact moment that we introduce this driving force, the amplitude of the oscillator instantaneously becomes enormous.
No. If there is no damping and the exciting frequency is exactly the same as the natural frequency (it would have to be), the energy in the resonator will be growing at the rate of the Power of signal that's being supplied to it.
In a real situation, there will be finite damping and the final level achieved for the energy in the resonator will be related to the Q (Quality factor or 'sharpness' of the response of the resonator) of the circuit and, when this level is finally reached, the power lost in the damping will be the same as the power being supplied.
 
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