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Question: Projection of uniform circular motion on a diameter is A. Simple harmonic motion. B. Angular sim...

Projection of uniform circular motion on a diameter is
A. Simple harmonic motion.
B. Angular simple harmonic motion.
C. Both A and B.
D. None of these.

Explanation

Solution

Simple harmonic motion or linear simple harmonic motion occurs when a particle moving along a straight line with acceleration whose direction is always towards a fixed point on the line and whose magnitude is proportional to the distance from the fixed point. Angular simple harmonic motion occurs when a body’s angular acceleration is proportional to its angular displacement from a fixed angular position and directed towards that position

Complete step by step answer:

Let us consider a particle PP moving in a uniform circular motion about a point OO in the XYXY plane as shown in the above figure.
Let OP=rOP = r
Splitting into horizontal and vertical component we can write xx and yy as
x=rcosθx = rcos\theta and y=rsinθy = r\sin \theta ……….. (1)\left( 1 \right)
Since it is uniform circular motion then, θ\theta increase in constant rate.
Therefore, θ=ωt\theta = \omega t ……….. (2)\left( 2 \right)
Substituting equation (2)\left( 2 \right) in equation (1)\left( 1 \right) we can write xx and yy
x=rcosωtx = r\cos \omega t ………. (3)\left( 3 \right) and
y=rsinωty = r\sin \omega t ……….. (4)\left( 4 \right)
Differentiating equation (3)\left( 3 \right) two times that is on double differentiating with respect to tt , we get
d2xdt2=ω2rcosωt=ω2x\dfrac{{{d^2}x}}{{d{t^2}}} = - {\omega ^2}r\cos \omega t = - {\omega ^2}x ……….. (5)\left( 5 \right)
We know that acceleration is given by, d2xdt2=a\dfrac{{{d^2}x}}{{d{t^2}}} = a ………… (6)\left( 6 \right)
Where, aa is the acceleration along xx - axis
Comparing equation (5)\left( 5 \right) and (6)\left( 6 \right)
a=ω2xa = - {\omega ^2}x ………… (7)\left( 7 \right)
We know that according to Newton’s second law,
F=maF = ma ………….. (8)\left( 8 \right)
Substituting equation (7)\left( 7 \right) in equation(8)\left( 8 \right), we get
F=mω2xF = - m{\omega ^2}x
Let us assume, constant K=mω2K = m{\omega ^2}, then F=KxF = - Kx
This force is directly proportional to the displacement, then the motion is said to be simple harmonic motion (S H M).Therefore projection of uniform circular motion on any diameter is linear simple harmonic motion (S H M).

Hence, the correct option is A.

Note: It should be noted that if the projection of uniform circular motion on a diameter is angular simple harmonic motion the force will be equal to (T)=Kθ\left( T \right) = - K\theta .Where, TT is the torque acting on the body