The time period ($T$) of a simple pendulum depends on its length ($L$) and the acceleration due to gravity ($g$). The formula is:
$ T = 2\pi\sqrt{\frac{L}{g}} $
Let the initial time period be $T_0$ and the initial length be $L_0$. According to the formula:
$ T_0 = 2\pi\sqrt{\frac{L_0}{g}} $
The length of the pendulum is reduced to $\frac{1}{16}$ times its initial value. The new length ($L_1$) is:
$ L_1 = \frac{1}{16} L_0 $
The new time period ($T_1$) is calculated using the new length:
$ T_1 = 2\pi\sqrt{\frac{L_1}{g}} $
Substitute $L_1 = \frac{1}{16} L_0$ into the equation:
$ T_1 = 2\pi\sqrt{\frac{\frac{1}{16} L_0}{g}} $
Simplify the expression:
$ T_1 = 2\pi\sqrt{\frac{1}{16}} \sqrt{\frac{L_0}{g}} $
$ T_1 = 2\pi \left(\frac{1}{4}\right) \sqrt{\frac{L_0}{g}} $
$ T_1 = \frac{1}{4} \left( 2\pi\sqrt{\frac{L_0}{g}} \right) $
Since $T_0 = 2\pi\sqrt{\frac{L_0}{g}}$, we can substitute $T_0$ back into the equation for $T_1$:
$ T_1 = \frac{1}{4} T_0 $
When the length of the pendulum is reduced to $\frac{1}{16}$ times its initial value, the modified time period becomes $\frac{1}{4} T_0$. This corresponds to Option B.
Two simple harmonic motions, as shown below, are at right angles. They are combined to form lissajous figures.
$x(t) = A \sin (at + \delta)$
$y(t) = B \sin (bt)$
Identify the correct match below :
The motion of a mass on a spring, with spring constant K is as shown in figure.
The equation of motion is given by $x(t) = A\sin\omega t+B\cos\omega t$ with $\omega=\sqrt{\frac{K}{m}}$.
Suppose that at time $t = 0$, the position of mass is $x(0)$ and velocity $v(0)$, then its displacement can also be represented as $x(t) = C\cos(\omega t-\phi)$, where $C$ and $\phi$ are

A piston of mass $M$ is hung from a massless spring whose restoring force law goes as $F= -kx^3$, where $k$ is the spring constant of appropriate dimension. The piston separates the vertical chamber into two parts, where the bottom part is filled with 'n' moles of an ideal gas. An external work is done on the gas isothermally (at a constant temperature $T$) with the help of a heating filament (with negligible volume) mounted in lower part of the chamber, so that the piston goes up from a height $L_0$ to $L_1$, the total energy delivered by the filament is : (Assume spring to be in its natural length before heating)