What is a simple harmonic oscillator

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SUMMARY

A simple harmonic oscillator is defined as a mass attached to a spring, exhibiting sinusoidal motion over time. The governing equation for its motion is x(t)=A\sin(\omega t)+B\cos(\omega t), where A and B are constants determined by initial conditions. The angular frequency, ω, is calculated using the formula ω=\sqrt{\frac{k}{m}}, linking the spring constant k and mass m. This foundational concept is rooted in Hooke's law and Newton's second law of motion.

PREREQUISITES
  • Understanding of Hooke's Law
  • Familiarity with Newton's Second Law of Motion
  • Basic knowledge of differential equations
  • Concept of sinusoidal functions
NEXT STEPS
  • Explore the derivation of the motion equations for damped harmonic oscillators
  • Learn about the applications of simple harmonic motion in real-world systems
  • Investigate the relationship between simple harmonic motion and wave phenomena
  • Study the impact of varying spring constants on oscillation frequency
USEFUL FOR

Students of physics, engineers working with mechanical systems, and anyone interested in the principles of oscillatory motion will benefit from this discussion.

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Definition/Summary

An object (typically a "mass on a spring") which has a position (or the appropriate generalization of position) which varies sinusoidally in time.

Equations

<br /> x(t)=A\sin(\omega t)+B\cos(\omega t)<br />

<br /> \omega^2 =\frac{k}{m}<br />

Extended explanation

According to Hooke's law and Newton's 2nd Law, a point mass of mass m attached to a spring of spring constant k obeys the equation
<br /> m\frac{d^2 x}{dt^2}=-kx\;,\qquad(1)<br />
where x is the position of the point mass.

The solution of equation (1) is given by
<br /> x(t)=A\sin(\omega t)+B\cos(\omega t)\;,\qquad(2)<br />
where A and B are constants that may be chosen so that x(t) satisfies the appropriate initial conditions, and
where
<br /> \omega=\sqrt{\frac{k}{m}}\;.<br />

For example, in terms of the initial position x_0 and initial velocity v_0, equation (2) can be written as
<br /> x(t)=\frac{v_0}{\omega}\sin(\omega t)+x_0\cos(\omega t)\;.<br />

* This entry is from our old Library feature. If you know who wrote it, please let us know so we can attribute a writer. Thanks!
 
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I understand that a sinusoidal oscillator is an object (usually a mass on a spring) that has a position that varies sinusoidally in time. The equation for the motion of this oscillator is given by x(t)=A\sin(\omega t)+B\cos(\omega t). Furthermore, we can derive the frequency of the oscillations as \omega=\sqrt{\frac{k}{m}}.
 

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