Assertion (A): | \(y=\text{sin}\omega t+\text{cos}2\omega t\) is not a simple harmonic function even though it is periodic. | The combination of
Reason (R): | \( \dfrac{d^{2} y}{d t^{2}}=-k y \). | All periodic functions satisfy the relation
1. | Both (A) and (R) are True and (R) is the correct explanation of (A). |
2. | Both (A) and (R) are True but (R) is not the correct explanation of (A). |
3. | (A) is True but (R) is False. |
4. | Both (A) and (R) are False. |
1. | \(\dfrac{\pi}{\omega}\) | 2. | \(\dfrac{2\pi}{\omega}\) |
3. | \(\dfrac{1}{\omega}\) | 4. | \(\dfrac{\omega}{2\pi}\) |
1. | a straight line and is periodic. |
2. | a circle and is non-periodic. |
3. | an ellipse and is periodic. |
4. | a parabola and is non-periodic. |
When a periodic force \(\vec{F_1}\) acts on a particle, the particle oscillates according to the equation \(x=A\sin\omega t\). Under the effect of another periodic force \(\vec{F_2}\), the particle oscillates according to the equation \(y=B\sin(\omega t+\frac{\pi}{2})\). The amplitude of oscillation when the force (\(\vec{F_1}+\vec{F_2}\)) acts are:
1. | \(A+B\) | 2. | \(\sqrt{A^2+B^2}\) |
3. | \(\large\frac{\sqrt{A^2+B^2}}{2}\) | 4. | \(\sqrt{AB}\) |
The total mechanical energy of a linear harmonic oscillator is \(600~\text J.\) At the mean position, its potential energy is \(100~\text J.\) The minimum potential energy of the oscillator is:
1. \(50~\text J\)
2. \(500~\text J\)
3. \(0\)
4. \(100~\text J\)
1. | \(\sqrt{\dfrac{6}{5}} ~T \) | 2. | \(\sqrt{\dfrac{5}{6}} ~T\) |
3. | \(\sqrt{\dfrac{6}{7}}~T\) | 4. | \(\sqrt{\dfrac{7}{6}} ~T\) |
1. | \(T=2 \pi \sqrt{\dfrac{M}{k}}\) | 2. | \(T=2 \pi \sqrt{\dfrac{k}{M}}\) |
3. | \(T=\dfrac{1}{2 \pi} \sqrt{\dfrac{k}{M}}\) | 4. | \(T=2 \pi \sqrt{\dfrac{M}{k}} \sin \theta\) |
The acceleration-time graph of a particle undergoing SHM is shown in the figure. Then,
1. | the velocity of the particle at point 2 is zero |
2. | velocity at point 3 is zero |
3. | velocity at point 2 is +ve and maximum |
4. | both (2) & (3) |
The (displacement-time) graph of a particle executing SHM is shown in the figure. Then:
(a) | the force is zero at \(t=\dfrac{3T}{4}\) |
(b) | the acceleration is maximum at \(t=\dfrac{4T}{4}\) |
(c) | the velocity is maximum at \(t=\dfrac{T}{4}\) |
(d) | the potential energy is equal to the kinetic energy of oscillation at \(t=\dfrac{T}{2}\) |
1. | (a), (b) and (d) only | 2. | (a), (b) and (c) only |
3. | (b), (c) and (d) only | 4. | (c) and (d) only |