Period of oscillation (potential energy equation given)

In summary, the potential energy of a particle is given by U(x) = U0(1-cos(ax)), where U0 and a are constants. The period of small oscillations performed by the particle about its equilibrium position can be found using the equation T = 2π√(m/a2U0). The motion is relevant to forced oscillations, as an external time-dependent force is needed for forced oscillation. In addition, there are two sufficient conditions to prove something is a simple harmonic oscillator: F = -kx or Etotal = \frac{1}{2}Av2+\frac{1}{2}Bq2, where A and B are constants and q is a coordinate. For the second
  • #1
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0

Homework Statement


Let the potential energy of particle depend upon coordinate x as:
U(x) = U0(1-cos(ax)). Where "U0" and "a" are constants. Find the period of small oscillations that particle performs about its equilibrium position.

2. Given Answer

T = 2∏√(m/a2U0)

The Attempt at a Solution



It can be seen from the equation that equilibrium will be at x = 0, where forces acting are zero. Also after integrating the equation with dx, it is seen that the motion is relevant to forced oscillations.
 
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  • #2
U(x) is the potential function. Why do you integrate it?
The motion is not forced oscillation. For that, an external time dependent force is needed.

ehild
 
  • #3
There a two sufficient conditions to prove something is simple harmonic oscillator
F = -kx
or
Etotal = [itex]\frac{1}{2}[/itex]Av2+[itex]\frac{1}{2}[/itex]Bq2. Where A and B are some constants and, q is some coordinate (in your case ax). Then the period is T = 2π√(A/B) Also since it says small oscillations, I would use the small angle approximation for cosine.
 
  • #4
therealnihl said:
Etotal = [itex]\frac{1}{2}[/itex]Av2+[itex]\frac{1}{2}[/itex]Bq2. Where A and B are some constants and, q is some coordinate (in your case ax). Then the period is T = 2π√(A/B) Also since it says small oscillations, I would use the small angle approximation for cosine.

Thanks for that. But this questions has two parts which I didn't mention.
The part-2 of the problem has the equation:
U(x)= a/x2 - b/x
How to deal with this one ?
I mean in above equation x has powers -2 and -1. So how to form its differential equation?
 
  • #5
Well assuming the kinetic energy is of the form: [itex]\frac{1}{2}[/itex]mv2, the the period for small oscillations is 2π√(k/m) where, k is the second derivative of the potential energy function evaluated at the equilibrium position (you might have to take the limit as it goes to the equilibrium position in this case...)
 

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