Solving Simple Harmonic Motion: Find Angular Freq & Amp.

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SUMMARY

The discussion focuses on deriving the angular frequency and amplitude of a particle undergoing simple harmonic motion (SHM) based on given velocities and displacements. The established formulas are: angular frequency = √[(v2² - v1²)/(x1² - x2²)] and amplitude = √[(x1²*v2² - x2²*v1²)/(v2² - v1²)]. The participant inquired about the appropriateness of treating the solution as a sum of two separate solutions and the use of phase angle in the context of linear differential equations. The consensus suggests using two arbitrary constants in the general solution, either A cos(ωt + φ) or A cos(ωt) + B sin(ωt).

PREREQUISITES
  • Understanding of simple harmonic motion (SHM)
  • Familiarity with angular frequency and amplitude concepts
  • Knowledge of linear differential equations
  • Basic trigonometric identities and functions
NEXT STEPS
  • Study the derivation of angular frequency in simple harmonic motion
  • Explore the application of linear differential equations in physics
  • Learn about phase angles in oscillatory motion
  • Investigate the use of arbitrary constants in general solutions of differential equations
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Students and educators in physics, particularly those focusing on mechanics and oscillatory motion, as well as anyone looking to deepen their understanding of simple harmonic motion and its mathematical representations.

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Question: A particle undergoing simple harmonic motion has a velocity v1 when the displacement is x1 and a velocity v2 when the displacement is x2. Find the angular frequency and the amplitutde of the motion in terms of the given quantities. The answers given in the back of the book are: angular frequency = [(v2^2 - v1^2)/(x1^2 - x2^2)]^(1/2) and amplitude = [(x1^2*v2^2 - x2^2*v1^2)/(v2^2 - v1^2)]^(1/2).

I've tried approaching this several ways, but can't seem to get my answers to agree. Should I treat the solution as a sum of two separate solutions with two different amplittudes since this is a linear differential equation, such that x(t) = x1(t) + x2(t) = A*cos(w*t + phi) + B*cos(w*t + phi) and similarly with v(t) = v1(t) + v2(t) = -w*A*sin(w*t + phi) - w*B*sin(w*t + phi). Or is there an easier way? I'm not sure what is appropriate to generalize and what is not. For example, I've taken the phase angle phi to be zero which I believe is acceptable. Any other suggestions? Thanks.
 
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You only need two arbitrary constants in your general solution. You can use either

[tex]A \cos(\omega t + \phi)[/tex]
or
[tex]A \cos \omega t + B \sin \omega t[/tex].
 

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