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Eohlas
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Homework Statement
A particle of mass m= 1.18kg is attached between two identical springs on a frictionless, horizontal tabletop. Both springs have spring constant k and are initially unstressed, and the particle is at x=0.
a) The particle is pulled a distance x along a direction perpendicular to the initial configuration of the springs as shown. Show that the force exerted by the springs on the particle is F = -2kx(1- L/ (sq rt (x2+L2)) in the i (or x) direction.
http://imageshack.us/a/img690/1021/20130308194200.jpg
Homework Equations
ΔU= - W = -1/2kx^2
Partial derivatives of U
Force = dU/dX
The Attempt at a Solution
Considering that the length of an unstressed spring is L, and that the particle was pulled a distance x away from x=0, I calculated the length of a stretched spring to be √(x^2 + L^2).
Additionally, in the initial position of the system, the particle was not moving, and the springs were unstressed, so the initial kinetic energy and potential energy both are 0. As the particle was moved away, the potential energy increased. The change in potential energy would be -1/2kx^2. I wasn't sure if the particle being pulled away would be considered to be kinetic energy, so I assumed that the final kinetic energy was also zero.
Seeing as force = dU/dX (or dU/dx + dU/dy for two dimensional problems like this problem), I performed a partial derivation on -1/2 kx^2, which resulted in -kx i + 0 j .(would this be why there is no j-component force acting on the particle?)
So now I have -kx i, which I multiplied by 2 since there are two springs in the system, which leads to -2kx i. This is where I am stuck. I don't understand where (1 - L/√(x^2 + L^2)) came from, although I do recognize L/ √(x^2 + L^2) to be the sine of the triangle. (I hope the picture will help clarify what I am talking about)
Any hints and corrections to my reasoning would be appreciated. :)
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