364090 Assertion :
The graph of potential energy and kinetic energy of a particle in SHM with respect to position is a parabola.
Reason :
Potential energy and kinetic energy do not vary linearly with position.

364091 Figure shows the kinetic energy \({K}\) of a simple pendulum versus its angle \({\theta}\) from the vertical. The pendulum bob has mass \(0.2\,kg\). The length of the pendulum \({\left(g=10 {~m} / {s}^{2}\right)}\) is

364092 A linear harmonic oscillator of force constant \(2 \times {10^6}\;N{\rm{/}}m\) and amplitude \(0.01\;m\) has a total mechanical energy of \(160\;J\) its

364093 An oscillator of mass \(M\) is at rest in the equillibrium position in a potential
\(V=\dfrac{1}{2} k(x-X)^{2}\). A particle of mass \(m\) comes from right with speed \(u\) and collides completely inelastically with \(M\) and sticks to it. This process repeats every time the oscillator crosses its equillibrium position. The amplitude of oscillations after 13 collisions is:\((M=10, m=5, u=1, k=1)\)

364090 Assertion :
The graph of potential energy and kinetic energy of a particle in SHM with respect to position is a parabola.
Reason :
Potential energy and kinetic energy do not vary linearly with position.

364091 Figure shows the kinetic energy \({K}\) of a simple pendulum versus its angle \({\theta}\) from the vertical. The pendulum bob has mass \(0.2\,kg\). The length of the pendulum \({\left(g=10 {~m} / {s}^{2}\right)}\) is

364092 A linear harmonic oscillator of force constant \(2 \times {10^6}\;N{\rm{/}}m\) and amplitude \(0.01\;m\) has a total mechanical energy of \(160\;J\) its

364093 An oscillator of mass \(M\) is at rest in the equillibrium position in a potential
\(V=\dfrac{1}{2} k(x-X)^{2}\). A particle of mass \(m\) comes from right with speed \(u\) and collides completely inelastically with \(M\) and sticks to it. This process repeats every time the oscillator crosses its equillibrium position. The amplitude of oscillations after 13 collisions is:\((M=10, m=5, u=1, k=1)\)

364090 Assertion :
The graph of potential energy and kinetic energy of a particle in SHM with respect to position is a parabola.
Reason :
Potential energy and kinetic energy do not vary linearly with position.

364091 Figure shows the kinetic energy \({K}\) of a simple pendulum versus its angle \({\theta}\) from the vertical. The pendulum bob has mass \(0.2\,kg\). The length of the pendulum \({\left(g=10 {~m} / {s}^{2}\right)}\) is

364092 A linear harmonic oscillator of force constant \(2 \times {10^6}\;N{\rm{/}}m\) and amplitude \(0.01\;m\) has a total mechanical energy of \(160\;J\) its

364093 An oscillator of mass \(M\) is at rest in the equillibrium position in a potential
\(V=\dfrac{1}{2} k(x-X)^{2}\). A particle of mass \(m\) comes from right with speed \(u\) and collides completely inelastically with \(M\) and sticks to it. This process repeats every time the oscillator crosses its equillibrium position. The amplitude of oscillations after 13 collisions is:\((M=10, m=5, u=1, k=1)\)

364090 Assertion :
The graph of potential energy and kinetic energy of a particle in SHM with respect to position is a parabola.
Reason :
Potential energy and kinetic energy do not vary linearly with position.

364091 Figure shows the kinetic energy \({K}\) of a simple pendulum versus its angle \({\theta}\) from the vertical. The pendulum bob has mass \(0.2\,kg\). The length of the pendulum \({\left(g=10 {~m} / {s}^{2}\right)}\) is

364092 A linear harmonic oscillator of force constant \(2 \times {10^6}\;N{\rm{/}}m\) and amplitude \(0.01\;m\) has a total mechanical energy of \(160\;J\) its

364093 An oscillator of mass \(M\) is at rest in the equillibrium position in a potential
\(V=\dfrac{1}{2} k(x-X)^{2}\). A particle of mass \(m\) comes from right with speed \(u\) and collides completely inelastically with \(M\) and sticks to it. This process repeats every time the oscillator crosses its equillibrium position. The amplitude of oscillations after 13 collisions is:\((M=10, m=5, u=1, k=1)\)