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Question: Three simple harmonic motions in the same direction having the same amplitude $A$ and same period ar...

Three simple harmonic motions in the same direction having the same amplitude AA and same period are superposed. If each differ in phase from the next by 6060^\circ, then choose the correct statement(s).

A

resultant amplitude is 2A

B

phase of the resultant motion relative to the motion having least phase is 6060^\circ

C

energy associated with the resulting motion is 4 times the energy associated with any single motion

D

resulting motion is not simple harmonic

Answer

Resultant amplitude is 2A, phase of the resultant motion relative to the motion having least phase is 6060^\circ, energy associated with the resulting motion is 4 times the energy associated with any single motion

Explanation

Solution

Let the three SHMs be:

x1=Acosωt,x2=Acos(ωt+60),x3=Acos(ωt+120).x_1=A\cos\omega t, \quad x_2=A\cos(\omega t+60^\circ), \quad x_3=A\cos(\omega t+120^\circ).

Representing them as phasors:

  • A1=A0\vec{A}_1 = A\angle 0^\circ
  • A2=A60\vec{A}_2 = A\angle 60^\circ
  • A3=A120\vec{A}_3 = A\angle 120^\circ

Step 1: Add the phasors

Break into components:

A1=A,A2=Acos60+iAsin60=A2+i3A2,A3=Acos120+iAsin120=A2+i3A2.\begin{aligned} \vec{A}_1 &= A,\\[1mm] \vec{A}_2 &= A\cos60^\circ + i\,A\sin60^\circ = \frac{A}{2} + i\frac{\sqrt{3}A}{2},\\[1mm] \vec{A}_3 &= A\cos120^\circ + i\,A\sin120^\circ = -\frac{A}{2} + i\frac{\sqrt{3}A}{2}. \end{aligned}

Summing:

Real part=A+A2A2=A,Imaginary part=3A2+3A2=3A.\begin{aligned} \text{Real part} &= A + \frac{A}{2} - \frac{A}{2} = A,\\[1mm] \text{Imaginary part} &= \frac{\sqrt{3}A}{2}+\frac{\sqrt{3}A}{2}= \sqrt{3}A. \end{aligned}

Thus, the resultant phasor is:

R=A+i3A.\vec{R} = A + i\sqrt{3}A.

Step 2: Resultant amplitude and phase

Magnitude (Amplitude):

R=A2+(3A)2=A2+3A2=2A.|\vec{R}|=\sqrt{A^2+( \sqrt{3}A)^2}=\sqrt{A^2+3A^2} =2A.

Phase:

ϕ=tan1(3AA)=60.\phi=\tan^{-1}\left(\frac{\sqrt{3}A}{A}\right)=60^\circ.

Step 3: Energy considerations

Energy in SHM ∝ (Amplitude)2^2. Hence, the energy of the resulting motion:

ER(2A)2=4A2,E_R\propto (2A)^2=4A^2,

which is 4 times that of any single motion (A2)(A^2).

Step 4: Nature of the resultant motion

Since the summation gives a single cosine function with amplitude 2A2A and phase 6060^\circ, the motion is indeed simple harmonic.