Two particles are executing simple harmonic motion of the same amplitude $A$ and frequency $\omega$ along the $x-$axis. Their mean position is separated by distance $X_0(X_0 > A).$ If the maximum separation between them is $(X_0 + A)$, the phase difference between their motion is:
AIEEE 2011, Diffcult
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Equation of motion of particle 1 ,

$x_1=A \sin \left(\omega t+\phi_1\right) \text {...1 }$

Equation of motion of particle 2,

$x_2=A \sin \left(\omega t+\phi_2\right) \text {...2 }$

From (1) and (2)

$x_2-x_1=A \sin \left(\omega t+\phi_2\right)-A \sin \left(\omega t+\phi_1\right)$

$=A\left[\sin \left(\omega t+\phi_2\right)-\sin \left(\omega t+\phi_1\right)\right]$

Using, $\sin C-\sin D=2 \cos \left(\frac{C+D}{2}\right) \cdot \sin \left(\frac{C-D}{2}\right)$

$x_2-x_1=2 A \cos \left(\omega t+\frac{\phi_1+\phi_2}{2}\right) \cdot \sin \left(\frac{\phi_2-\phi_1}{2}\right)$

Given that, $\left(x_0+x_2-x_1\right)_{\max }=x_0+A$

$\Rightarrow\left(x_2-x_1\right)_{\max }=A$

$\text { To get }\left(x_2-x_1\right)_{\max } \text {, we }$

$\Rightarrow 2 A \sin \left(\frac{\phi_2-\phi_1}{2}\right)=A$

$\Rightarrow \sin \left(\frac{\phi_2-\phi_1}{2}\right)=\frac{1}{2} $

$\Rightarrow \frac{\phi_2-\phi_1}{2}=\frac{\pi}{6} \text { or } \frac{5 \pi}{6}$

$\Rightarrow \phi_2-\phi_1=\frac{\pi}{3} \text { or } \frac{5 \pi}{3}$

$\text { To get }\left(x_2-x_1\right)_{\max } \text {, we assume } \cos \left(\omega t+\frac{\phi_1+\phi_2}{2}\right)=1$

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