Solve Classical Mechanics: Find Force, Stable & Turning Points

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SUMMARY

The discussion focuses on solving classical mechanics problems related to a mass m moving in a potential energy function defined as U(x) = -a/x + b/x^2. Participants detail how to derive the force F(x) from the potential energy, emphasizing the relationship F = -dU/dx. The conversation highlights the importance of establishing the total energy E and setting up a differential equation to find the period of oscillation. The method involves integrating the equation E = (1/2)mv^2 + U(x) to determine the motion of the mass and the period of oscillation.

PREREQUISITES
  • Understanding of potential energy functions in classical mechanics
  • Familiarity with the concept of force derived from potential energy
  • Knowledge of differential equations and energy conservation principles
  • Basic grasp of oscillatory motion and harmonic oscillators
NEXT STEPS
  • Study the derivation of force from potential energy using F = -dU/dx
  • Learn how to set up and solve differential equations for energy conservation
  • Explore the method of integrating to find the period of oscillation for non-linear systems
  • Investigate small oscillation approximations and their applications in harmonic motion
USEFUL FOR

Students and professionals in physics, particularly those studying classical mechanics, as well as engineers and researchers involved in dynamics and oscillatory systems.

danai_pa
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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
 
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How about just using an analogy with the case for a spring:

F(x)=kx, etc. :smile:
 
Berislav said:
How about just using an analogy with the case for a spring:

F(x)=kx, etc. :smile:

w(omega) = sqrt(k/m) is correct?.
if correct how can to find values k?. please explain
 
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.
 
F= - \frac {dU}{dX}

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

BJ
 
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"?
 
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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