Simple harmonic motion: Difference between revisions

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Simple harmonic motion is a form of motion of an object/particle along a line subject to the constraint:
Simple harmonic motion is a form of motion of an object/particle along a line subject to the constraint:


<math>x''(t) = -\omega^2 x(t)</math>
<math>\! x''(t) = -\omega^2 x(t)</math>


where <math>x(t)</math> is the position coordinate of the particle at time <math>t</math> and <math>x''(t) = a(t)</math> is the acceleration (signed) of the particle at time <math>t</math>.
where <math>x(t)</math> is the position coordinate of the particle at time <math>t</math> and <math>x''(t) = a(t)</math> is the acceleration (signed) of the particle at time <math>t</math>.

Latest revision as of 13:32, 12 August 2011

Definition

In terms of the equation for position

Simple harmonic motion is defined as a form of periodic/oscillatory motion along a straight line, with the following form of equation describing the position coordinate as a function of time:

x=x(t)=x0+Asin(ωt+φ)

Here, x0 is the resting position or mean position, A is the amplitude of oscillation (in that it describes the maximum possible magnitude of displacement from the mean position), ω is a parameter controlling the frequency (in fact, ω is 2π times the frequency of completing one full oscillation), t is the time parameter, and φ is a phase angle.

As a consequence, we have the following descriptions of the velocity and acceleration functions:

v(t)=Aωcos(ωt+φ)

and

a(t)=Aω2sin(ωt+φ)

In terms of the differential equation it solves

Simple harmonic motion is a form of motion of an object/particle along a line subject to the constraint:

x(t)=ω2x(t)

where x(t) is the position coordinate of the particle at time t and x(t)=a(t) is the acceleration (signed) of the particle at time t.