How does frequency depend on the potential energy?

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The discussion focuses on determining the frequency of a particle confined in a potential field U(x) between two points, a and b, where U(a) and U(b) equal the initial kinetic energy K_o. The force on the particle is derived from the negative gradient of the potential, F(x) = -dU/dx, allowing for the calculation of acceleration a(x) based on the particle's mass. By analyzing the total distance between points a and b, and knowing that the velocity at these points is zero, the time taken for the particle's motion can be established. This time, when doubled, provides the inverse of the system's frequency. Additionally, a Taylor expansion of U(x) can lead to an approximation of the potential energy as a simple harmonic oscillator with a specific spring constant k.
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Let's say you have a particle confined to one dimension in a potential field U(x). At t=0, the particles initial kinetic energy is K_o. U(x) is such that the particle is trapped between two points x=a and x=b; this means U(a) = U(b) = K_o, and the slopes of U(x) at a and b are such that the particle is kept between a and b. How would you find the frequency of this system?
 
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From -dU/dx, you know the force on the particle, F(x). With it's mass, you can find the acceleration a(x). From a(x) and the total distance, x = |b-a|, you can find the time taken, since you know v(a) = v(b) = 0. Twice this time is the inverse of the frequency.
 
By doing a Taylor expansion for U(x), you may also be able to approximate your potential energy function by "a simple harmonic oscillator with spring constant k".
 
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