Each and every object possesses energy, either while moving or at rest. In the simple harmonic motion, the object moves to and fro along the same path. Do you think an object possesses energy while travelling the same path again and again? Yes, it is energy in simple harmonic motion. Let’s learn how to calculate this energy and understand its properties.

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## Energy in Simple Harmonic Motion

The total energy that a particle possesses while performing simple harmonic motion is energy in simple harmonic motion. Take a pendulum for example. When it is at its mean position, it is at rest. When it moves towards its extreme position, it is in motion and as soon as it reaches its extreme position, it comes to rest again. Therefore, in order to calculate the energy in simple harmonic motion, we need to calculate the kinetic and potential energy that the particle possesses.

**Download the Cheat Sheet of Oscillations below**

**Browse more Topics under Oscillations**

- Simple Harmonic Motion
- Damped Simple Harmonic Motion
- Forced Simple Harmonic Motion
- Force Law for Simple Harmonic Motion
- Velocity and Acceleration in Simple Harmonic Motion
- Some Systems executing Simple Harmonic Motion
- Energy in Simple Harmonic Motion
- Periodic and Oscillatory Motion

### Kinetic Energy (K.E.) in S.H.M

Kinetic energy is the energy possessed by an object when it is in motion. Let’s learn how to calculate the kinetic energy of an object. Consider a particle with mass *m* performing simple harmonic motion along a path AB. Let O be its mean position. Therefore, OA = OB = a.

The instantaneous velocity of the particle performing S.H.M. at a distance x from the mean position is given by

v= ±ω √a^{2} – x^{2}

∴ v^{2 }= ω^{2} ( a^{2 } – x^{2})

∴ Kinetic energy= 1/2 mv^{2 } = 1/2 m ω^{2} ( a^{2 } – x^{2})

As, k/m = ω^{2 }

∴ k = m ω^{2}

Kinetic energy= 1/2 k ( a^{2 } – x^{2}) . The equations Ia and Ib can both be used for calculating the kinetic energy of the particle.

Learn how to calculate Velocity and Acceleration in Simple Harmonic Motion.

### Potential Energy(P.E.) of Particle Performing S.H.M.

Potential energy is the energy possessed by the particle when it is at rest. Let’s learn how to calculate the potential energy of a particle performing S.H.M. Consider a particle of mass *m* performing simple harmonic motion at a distance x from its mean position. You know the restoring force acting on the particle is F= -kx where k is the force constant.

Now, the particle is given further infinitesimal displacement dx against the restoring force F. Let the work done to displace the particle be dw. Therefore, The work done dw during the displacement is

dw = – fdx = – (- kx)dx = kxdx

Therefore, the total work done to displace the particle now from 0 to x is

∫dw=_{ }∫kxdx = k ∫x dx

Hence Total work done = 1/2 K x^{2} = 1/2 m ω^{2}x^{2}

The total work done here is stored in the form of potential energy.

Therefore Potential energy = 1/2 kx^{2} = 1/2 m ω^{2}x^{2 }

Equations IIa and IIb are equations of potential energy of the particle. Thus, potential energy is directly proportional to the square of the displacement, that is P.E. α x^{2}.

Learn the Difference between Periodic and Oscillatory Motion.

## Total Energy in Simple Harmonic Motion (T.E.)

The total energy in simple harmonic motion is the sum of its potential energy and kinetic energy.

Thus, T.E. = K.E. + P.E. = 1/2 k ( a^{2 } – x^{2}) + 1/2 K x^{2 }= 1/2 k a^{2}

Hence, T.E.= E = 1/2 m ω^{2}a^{2}

Equation III is the equation of total energy in a simple harmonic motion of a particle performing the simple harmonic motion. As ω^{2 },^{ }a^{2 }are constants, the total energy in the simple harmonic motion of a particle performing simple harmonic motion remains constant. Therefore, it is independent of displacement x.

As ω= 2πf , E= 1/2 m ( 2πf )^{2}a^{2 }

∴ E= 2mπ^{2}f ^{2}a^{2}

As 2 and π^{2 }constants, we have T.E. ∼ m, T.E. ∼ f ^{2}, and T.E. ∼ a^{2}

Thus, the total energy in the simple harmonic motion of a particle is:

- Directly proportional to its mass
- Directly proportional to the square of the frequency of oscillations and
- Directly proportional to the square of the amplitude of oscillation.

The law of conservation of energy states that energy can neither be created nor destroyed. Therefore, the total energy in simple harmonic motion will always be constant. However, kinetic energy and potential energy are interchangeable. Given below is the graph of kinetic and potential energy vs instantaneous displacement.

In the graph, we can see that,

- At the mean position, the total energy in simple harmonic motion is purely kinetic and at the extreme position, the total energy in simple harmonic motion is purely potential energy.
- At other positions, kinetic and potential energies are interconvertible and their sum is equal to 1/2 k a
^{2}. - The nature of the graph is parabolic.

Learn how Damped Simple Harmonic Motion is different than Linear Simple Harmonic Motion.

## Here’s a Solved Question for You

Q:** **At the mean position, the total energy in simple harmonic motion is ________

a) purely kinetic b) purely potential c) zero d) None of the above

Answer: a) purely kinetic. At the mean position, the velocity of the particle in S.H.M. is maximum and displacement is minimum, that is, x=0. Therefore, P.E. =1/2 K x^{2 }= 0 and K.E. = 1/2 k ( a^{2 } – x^{2}) = 1/2 k ( a^{2 } – o^{2}) = 1/2 ka^{2}. Thus, the total energy in simple harmonic motion is purely kinetic.