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Views Read Edit View history. As long as the system has no energy loss, the mass continues to oscillate. When the mass moves closer to the equilibrium position, the restoring force decreases.


The motion is sinusoidal in time and demonstrates a single resonant frequency. This page was last edited on 29 Decemberat The area enclosed depends on the amplitude and the maximum momentum.

The above equation is also valid in the case when an additional constant force is being applied on the mass, i. A net restoring force then slows it down until its velocity reaches zero, whereupon it is dolutions back to the equilibrium position again.

Retrieved from ” https: Simple harmonic motion can serve as a mathematical model for a variety of motions, such as the oscillation of a spring. A mass m attached to a spring of spring constant k exhibits simple harmonic motion in closed space.

The equation for describing the period. For simple harmonic motion to be an accurate model for a analttical, the net force on the object at the end of the pendulum must be proportional to the displacement.

If the system is left at rest at the equilibrium position then there is no net force acting on the mass. Simple harmonic motion can be considered the one-dimensional projection of uniform circular motion.


Simple harmonic motion provides a basis for the characterization of more complicated motions through the techniques of Fourier analysis.

This is a good approximation when the angle of the swing is small. A Scotch yoke mechanism can be used to convert between rotational motion and linear reciprocating motion.


The motion of an undamped pendulum approximates to simple harmonic motion if the angle of oscillation is small. The linear motion can take various forms depending on the shape of the slot, but the basic yoke with a constant rotation speed produces a linear motion that is simple harmonic in form. From Wikipedia, the free encyclopedia. Other valid formulations are: In the diagram, a simple harmonic oscillatorconsisting fosles a weight attached to one end of a spring, is shown.

In Newtonian mechanicsfor one-dimensional simple harmonic motion, the equation of motion, which is a second-order linear ordinary differential equation with constant coefficients, can be obtained by means of Newton’s 2nd law and Hooke’s law for a mass on a spring.

An undamped spring—mass system undergoes simple analyytical motion. However, if the mass is displaced from the equilibrium position, the spring exerts a restoring elastic force that obeys Hooke’s law.

The following physical systems are some examples of simple harmonic oscillator. Simple harmonic motion is typified by the motion of a mass on a spring when it is subject to the linear elastic restoring force given by Hooke’s Law.

Simple harmonic motion

Thus simple harmonic motion is a type of periodic motion. Note if the real space and phase space diagram are not co-linear, the phase space motion becomes elliptical. At the equilibrium position, the net restoring force vanishes. In other projects Wikimedia Commons. As a result, it accelerates and starts going back to the equilibrium position. By definition, if a mass m is under SHM qnd acceleration is directly proportional to displacement.

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The motion of a particle moving along a straight line with an acceleration whose direction is always towards a fixed point on the line and whose magnitude is proportional to the distance from the fixed point is called simple harmonic motion [SHM]. The other end of the spring is connected to a rigid support such as a wall. In mechanics and physicssimple harmonic motion is a special type of periodic motion or oscillation motion where the restoring force is directly proportional to the displacement and acts in the direction opposite to that of displacement.

In the solution, c 1 and c 2 are two constants determined by the initial conditions, and the origin is set to be the equilibrium position. Therefore it can be simply defined as the periodic motion of a body along a straight line, such that the anf is directed towards the center of the motion and also proportional to the displacement from that point.

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