Simple Harmonic Oscillator and Damping

In summary, the conversation involves finding the ratio of the frequency of a damped harmonic oscillator after four cycles to its natural frequency, based on a given equation and assuming different damping forces. The solution is obtained by analyzing the amplitude of the oscillator and using the equations for underdamped, overdamped, and critically damped oscillators. However, the equations provided by the student were incorrect and needed to be corrected before finding the solution.
  • #1
Levi Tate
122
0

Homework Statement



After four cycles the amplitude of a damped harmonic oscillator has dropped to 1/e of it's initial value. Find the ratio of the frequency of this oscillator to that of it's natural frequency (undamped value)

Homework Equations



x'' +(√k/m) = 0

x'' = d/dt(dx/dt)

x'' + 2βx' + Wo^2= 0

Here we are assuming a damping force linear in v,

f = -bv

2β is defined as b/m where b is a constant.

Wo^2 = k/m

The Attempt at a Solution



Since the problem statement makes no mention of whether this is underdamped (β then than Wo), overdamped (β greater than Wo), or critically damped (β= Wo), I can only conclude that it does not matter what the case is.

Two of the solutions can be expressed as sines and cosines and would be periodic with 2∏, but one of the solutions is simply two exponential terms, which does not make sense to me.

That's kind of where I'm stuck, any thoughts would be helpful. Thanks.
 
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  • #2
Well, it tells you that it oscillates 4 times before amplitude decreases by a factor of e.
Could this be over-damped oscillator?

I don't think you need to find the solution from scratch here. Don't you have it in your notes or textbook? It contains a product of a cosine (or sine) and an exponentially decreasing term.
 
  • #3
Yeah mate I have all the solutions, that isn't my problem. I am thinking it must be the underdamped oscillator, because the overdamping case doesn't oscillate harmonically, it is real, so the solution is just two exponentials. With critical damping, the solutions are imaginary so I am pretty sure it is underdamping..

Excuse me with underdamping the solution is imaginary and can be wrote as

x(t) = Ae^-ßt cos(w1t -ø)

Where W1 = (Wo^2+ß^2)^1/2

Since it says 4 cycles, I am thinking 8 pie, but it's just tough to put together the mathematics here.
 
  • #4
Isn't there a minus in that last formula?
The damping decreases the frequency.

It's good to have all the formulas. Now you need to understand them as well.
Looking at the formula for x(t), after how long the amplitude decreases to A/e?
You can take the initial phase (∅) equal to zero. You don't have to but it may help to understand what is going on.
 
  • #5
Yes that is a minus, sorry. I was thinking about putting the phase equal to zero. I have the solution, i got the problem wrong, I just thought it would be helpful to talk about it and try to solve it on my own before looking at it. Right now I'm caught up in the Lagrangian but I will return to that problem at some point in the night. I will try to set the phase equal to zero and reanalyze. Thanks.
 
  • #6
Your equations for the oscillator are not correct. They should be

x'' +(√k/m)x = 0

x'' + 2βx' + Wo^2x= 0

As the oscillator makes oscillations (after four has its amplitude dropped to 1/e of its initial value), it can not be critically damped or overdamped.

You have the equation x(t) = Ae^-ßt cos(w1t -ø). Ae^-ßt is the amplitude of the cosine factor.
As you know that the amplitude Ae^-ßt decreases to[STRIKE] A/4[/STRIKE] A/e in 4 cycles, you can determine β, by replacing t=4T. You do not need to worry about the cosine factor. How is the period T related to the angular frequency w1? If you know β you can get w1 in terms wo.

ehild
 
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  • #7
It decreases to A/e and not A/4.

But anyway, he is busy with other problems now. :smile:
 
  • #8
nasu said:
It decreases to A/e and not A/4.

But anyway, he is busy with other problems now. :smile:

Yes, stupid of me :redface:

ehild
 
  • #9
Yes sorry I was onto other problems, it was just my teacher solved it very strangely by taking ratios, so I just let it go. Thank you for your help though.
 

FAQ: Simple Harmonic Oscillator and Damping

What is a simple harmonic oscillator?

A simple harmonic oscillator is a type of periodic motion that occurs when a restoring force is proportional to the displacement from an equilibrium position. This means that the object moves back and forth around the equilibrium position, with a constant period and amplitude.

What is damping in a simple harmonic oscillator?

Damping is the process of reducing the amplitude of oscillations over time. In a simple harmonic oscillator, damping can be caused by external forces, such as friction or air resistance, or by internal factors, such as the material of the object or its shape.

How is damping represented in a simple harmonic oscillator?

Damping is represented by a damping coefficient, which is a measure of the rate at which the amplitude of the oscillations decreases. This coefficient is often denoted by the symbol "b" and is included in the equation for a damped simple harmonic oscillator.

What is the difference between underdamping, overdamping, and critical damping?

In an underdamped system, the damping coefficient is less than the critical damping coefficient, resulting in an oscillation with a decreasing amplitude over time. In an overdamped system, the damping coefficient is greater than the critical damping coefficient, causing the oscillations to quickly reduce to zero. In a critically damped system, the damping coefficient is equal to the critical damping coefficient, resulting in the fastest possible return to equilibrium without any oscillations.

How is the period of a damped simple harmonic oscillator affected?

The period of a damped simple harmonic oscillator is affected by the damping coefficient. As the damping coefficient increases, the period also increases. This means that the oscillations take longer to complete and the system reaches equilibrium at a slower rate.

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