 # Simple Harmonic Motion and Uniform Circular Motion

Simple harmonic motion is a special kind of periodic motion, in which a particle moves to-and-fro repeatedly about a mean or an equilibrium position under a restoring force that is directed towards the mean position.

Consider a particle placed on the circumference of a circle.

Initially, the particle is at point X as you can see in the figure below:

As it moves from X to P, there is an angular displacement (an arc) which is equal to Θ and at time = t, the particle reaches from point OX to P.

The motion is along the circle with a constant angular velocity ω.

So, the angle subtended by a particle,  Θ = ωt

The mean position of the particle is at point O.

Now, we draw a perpendicular from P to a certain point on the diameter XOX’.

So the displacement from O to a certain point is, ‘x’.

The instantaneous acceleration will be directly proportional to this displacement.

a α x

Now, if we multiply m on both sides, we get

ma α mx

Or,     F α x

So, we concluded that one-dimensional motion of a particle in a uniform circular motion about its mean position is in simple harmonic motion.

Shm as a Projection of Uniform Circular Motion on Any Diameter

Consider a particle P moving with uniform speed along the circumference of a circle with radius a, having center O. This circle is considered as a circle of reference with particle P as the particle of reference.

Here, if you look at Fig.1, XOX’ and YOY’ are perpendicular diameters of the circle of reference.

As the reference particle moves from X to Y, its projection on diameter YOY’ moves from O to Y.

As this reference particle moves from Y to X’, its projection moves along the diameter from Y to O.

Similarly, when the reference particle moves on the circle from X’ to X via Y’, its projection moves along the diameter from O to Y’ and then from Y’ to O.

Thus, during the time the particle P goes around the circle and completes one revolution, its projection, ‘M’ oscillates about the point O along the diameter YOY’ and completes one vibration. Since the projection of the reference particle is in SHM, and the projection of M on diameter YOY’ is also a simple harmonic motion.

Therefore, simple harmonic motion is defined as the projection of uniform circular motion on any diameter of a circle of reference.

Shm as projection of uniform circular motion

Consider a reference particle moving on a circle of reference with radius, ‘a’ with uniform angular velocity, ‘ω’

From Fig.1

Let the particle at time t = 0, start from point X, and sweep an angular displacement Θ in time ‘t’ with angular velocity ω, equal to ωt.

Now, let the projection of the particle P on diameter YOY’ be at M.

Then the displacement in SHM at time t is given by,

OM = y

In ΔOPM,

SinΘ = OM/OP = y/a

Or,

 y = aSinΘ  = aSinωt ….(1)

Now,

In ΔONP,

CosΘ = ON/OP = x./a

Or,

 x = aCosΘ = aCosωt…(2)

From Fig. 3(a)

Now, if A is the starting position of the reference particle.

Here, ∠AOX = ф₀ and  ∠AOP = ωt and Θ  = ωt - ф₀

From eq(1) and (2)

y  = a Sin(ωt - ф₀)

x =  a Cos(ωt - ф₀)

Here, - ф₀ is called the initial phase of S.H.M.

Here, the phase is a physical quantity that is used to express the position and direction of motion of the particle at an instant concerning time represented by a sine or cosine function.

From Fig 3(b)

If we consider B as the starting position of the particle of reference.

If  ∠BOX = ф₀ and  ∠BOP = ωt

Then, ∠XOP =  ωt + ф₀

Now, from eq(1) and (2), we get

y  = a Sin(ωt + ф₀)

x =  a Cos(ωt + ф₀)

Here, + ф₀ is called the initial phase of S.H.M.

Shm Circular Motion

A reference particle moving along the circumference of a circle of reference makes a displacement.

Where the maximum displacement of a particle from its position is called the amplitude denoted by, ‘A’. It is equal to the radius of a circle.

If S is the span of S.H.M. Then,

 Amplitude A = S/2

Shm in Circular Motion

The velocity of a particle at an instant is the rate of change of displacement.

From (1),

y = a Sinωt

Differentiating both sides:

d(y)/dt = a d(Sinωt)/dt

V = a ω Cosωt =  a ω $\sqrt{(1-Sin²ωt)}$

= ω $\sqrt{(a² - y²)}$

At mean position, y = 0, then

V = a ω

At extreme position, y = a

V = 0

Thus, the maximum velocity in shm for a body in uniform circular motion is called the velocity amplitude.

Q1: What is a Circular Motion and Periodic Motion?

Ans:  A body that makes a circular locus can make a full circle or even a part of the circle while the body repeats itself after a fixed interval of time.

Such a circular motion can be a periodic motion if it repeats its motion after each 360° revolution.

Q2:  Is Circular Motion SHM?

Ans: Yes, one-dimensional circular motion can be described as simple harmonic motion. A particle P moves along the circle of reference with a constant velocity ω undergoing a uniform circular motion. Its projection on the x-axis undergoes a simple harmonic motion.

Q3: Is Rotational and Circular Motion the Same?

Ans: The difference between circular motion and rotational motion is outlined below:

The motion of a body around its center of mass is called the rotational motion,

while circular motion is a special case of rotational motion, where the distance between the body’s center of mass and the axis of rotation remains fixed.

Q4: Write Circular Motion Examples.

Ans: There are certain real-life examples of circular motion as outlined below:

1. The spinning of a ball on a string

2. Revolution of planets around the sun.

3. Turning a car through a curve in a race track.