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Classical Mechanics

  1. Jun 29, 2005 #1
    A mass m is move in potential

    U(x) = -a/x+b/x^2

    I can solve this problem to find force F(x), stable point, turnning point
    but i can't to find the equation of period of the mass for boundaring movement
    please help
     
  2. jcsd
  3. Jun 29, 2005 #2
    How about just using an analogy with the case for a spring:

    F(x)=kx, etc. :smile:
     
  4. Jun 29, 2005 #3
    w(omega) = sqrt(k/m) is correct?.
    if correct how can to find values k?. please explain
     
  5. Jun 29, 2005 #4

    robphy

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    Following Berislav 's suggestion,
    U(x)=(1/2)kx^2 for a spring.

    Hopefully, you *know* what force law F(x) corresponds to this potential energy function. How do you get F(x) from U(x)?

    What characterizes [in terms of U(x)] the position of the stable equilibrium point?

    Given a suitable total energy E (a constant), what is the range of positions available to the particle? If you can setup a differential equation for the conservation of energy, you can obtain an expression for t as a function of E and U(x).

    If you can successfully do this for this potential energy function, you should [in principle] be able to apply the same ideas to your potential energy function.
     
  6. Jun 30, 2005 #5
    [itex]F= - \frac {dU}{dX}[/itex]

    Put above equal to kx and get k , use some math.

    BJ
     
  7. Jun 30, 2005 #6
    how would you get k from that? Seems like you need to know what x is... :smile: Is that what you mean by "use some math"?
     
  8. Jun 30, 2005 #7
    danai_pa:

    Did you get an answer to this problem? I don't believe you will need to solve any cubic equations. Do what robphy said...set up the equation

    E = (1/2)mv^2 + U(x), where v = dx/dt

    and solve for dt. Integrate from one turning point to the other. That's half a period. This gives you the exact period even if the oscillation is not small. If you are allowed to assume the oscillation is small, you can expand the potential energy about a stable point and then apply the F = -kx technique.
     
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