364228 Two simple harmonic motions are represented by the equations \(y_{1}=0.1 \sin \left(100 \pi t+\dfrac{\pi}{3}\right)\) and \(y_{1}=0.1 \cos \pi t\). The phase difference of the velocity of particle 1 with respect to the velocity of particle 2 is

364229 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 \(X_{0}\left(X_{0}>A\right)\). If the maximum separation between them is \(A\), the phase difference between thier motion is:

364230 In SHM phase difference between displacement and velocity is \(\phi_{1}\) and that between displacement and acceleration is \(\phi_{2}\), then

364231 Two simple pendulum of length \(1\;m\) and \(4\;m\) respectively are given small linear displacement in one direction at the same time. They will again be in the phase when the pendulum of shorter length has completed oscillations \(\left[n T_{1}=(n-1) T_{2}\right.\), where \(T_{1}\) is time period of shorter length \({T_2}\) be time period of longer wavelength and \(n\) are no. of oscillations completed]

364228 Two simple harmonic motions are represented by the equations \(y_{1}=0.1 \sin \left(100 \pi t+\dfrac{\pi}{3}\right)\) and \(y_{1}=0.1 \cos \pi t\). The phase difference of the velocity of particle 1 with respect to the velocity of particle 2 is

364229 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 \(X_{0}\left(X_{0}>A\right)\). If the maximum separation between them is \(A\), the phase difference between thier motion is:

364230 In SHM phase difference between displacement and velocity is \(\phi_{1}\) and that between displacement and acceleration is \(\phi_{2}\), then

364231 Two simple pendulum of length \(1\;m\) and \(4\;m\) respectively are given small linear displacement in one direction at the same time. They will again be in the phase when the pendulum of shorter length has completed oscillations \(\left[n T_{1}=(n-1) T_{2}\right.\), where \(T_{1}\) is time period of shorter length \({T_2}\) be time period of longer wavelength and \(n\) are no. of oscillations completed]

364228 Two simple harmonic motions are represented by the equations \(y_{1}=0.1 \sin \left(100 \pi t+\dfrac{\pi}{3}\right)\) and \(y_{1}=0.1 \cos \pi t\). The phase difference of the velocity of particle 1 with respect to the velocity of particle 2 is

364229 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 \(X_{0}\left(X_{0}>A\right)\). If the maximum separation between them is \(A\), the phase difference between thier motion is:

364230 In SHM phase difference between displacement and velocity is \(\phi_{1}\) and that between displacement and acceleration is \(\phi_{2}\), then

364231 Two simple pendulum of length \(1\;m\) and \(4\;m\) respectively are given small linear displacement in one direction at the same time. They will again be in the phase when the pendulum of shorter length has completed oscillations \(\left[n T_{1}=(n-1) T_{2}\right.\), where \(T_{1}\) is time period of shorter length \({T_2}\) be time period of longer wavelength and \(n\) are no. of oscillations completed]

364228 Two simple harmonic motions are represented by the equations \(y_{1}=0.1 \sin \left(100 \pi t+\dfrac{\pi}{3}\right)\) and \(y_{1}=0.1 \cos \pi t\). The phase difference of the velocity of particle 1 with respect to the velocity of particle 2 is

364229 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 \(X_{0}\left(X_{0}>A\right)\). If the maximum separation between them is \(A\), the phase difference between thier motion is:

364230 In SHM phase difference between displacement and velocity is \(\phi_{1}\) and that between displacement and acceleration is \(\phi_{2}\), then

364231 Two simple pendulum of length \(1\;m\) and \(4\;m\) respectively are given small linear displacement in one direction at the same time. They will again be in the phase when the pendulum of shorter length has completed oscillations \(\left[n T_{1}=(n-1) T_{2}\right.\), where \(T_{1}\) is time period of shorter length \({T_2}\) be time period of longer wavelength and \(n\) are no. of oscillations completed]