Finding the Special Initial Velocity in a kx Force System

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The discussion focuses on determining the special initial velocity for a particle under a linear force F(x) = kx. The general solution for the particle's position over time is given as x(t) = Ae^{\omega t} + Be^{-\omega t}, where ω = √(k/m). To prevent the particle from moving indefinitely away from the origin, the coefficient A must equal zero, which leads to the condition v₀ = -Bω. The derived initial velocity for this condition is v₀ = -x₀ω, ensuring the particle remains close to the origin. This analysis clarifies the relationship between initial conditions and particle behavior in a kx force system.
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Homework Statement


A particle of mass m is subject to a force F(x) = kx, with k > 0. What is the most general form of x(t)? If the particle starts out at x0, what is the one special value of the initial velocity for which the particle doesn't eventually get far away from the origin?

Homework Equations


m\ddot{x} = kx

The Attempt at a Solution


So the general solution is x(t) = Ae^{\omega t} + Be^{-\omega t}, with \omega = \sqrt{\frac{k}{m}} of course. My issue is with the second part of the question; as far as I understand it, it wants me to figure out for what value of v0 makes it so that the first term of the general solution doesn't dominate (since that term would see x increase to infinity, whereas the second term would see x approaching the x-axis). If that's what the question is asking, I'm not quite sure how I'd go about that! Any hints and help would be much appreciated. :smile:
 
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Yes, x will go indefinitely away from x_0 as long as A is not 0.

You have the initial values x(0)= x_0 and x'(0)= v_0. What value of v_0 gives A= 0?
 
Okay, so if A is going to be 0, I get
v_{0} = -B\omega.
Owing to the fact that x(0) = x_{0} = A + B, and seeing as how A = 0, this gives me a value of
v_{0} = -x_{0}\omega.
Does that sound right?
 
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