The initial number of beats observed is 8 in a time interval of 2 seconds. The initial beat frequency ($f_{beat1}$) is calculated as:
$f_{beat1} = \frac{\text{Number of beats}}{\text{Time interval}} = \frac{8}{2\text{ s}} = 4\text{ Hz}$
The beat frequency is the absolute difference between the frequencies of two tuning forks ($f_A$ and $f_B$). Given the frequency of tuning fork B ($f_B$) is $380\text{ Hz}$ and the initial beat frequency ($f_{beat1}$) is $4\text{ Hz}$, we have:
$|f_A - f_B| = f_{beat1}$
Substituting the known values:
$|f_A - 380\text{ Hz}| = 4\text{ Hz}$
This equation yields two possible values for the original frequency of tuning fork A ($f_A$):
Loading a tuning fork with wax adds mass, which slightly decreases its natural frequency. Let the new frequency of tuning fork A after loading be $f_A'$. Therefore, $f_A' < f_A$.
After loading, the new beat frequency ($f_{beat2}$) is observed as 4 beats in 2 seconds:
$f_{beat2} = \frac{4}{2\text{ s}} = 2\text{ Hz}$
The new relationship between the frequencies is:
$|f_A' - f_B| = f_{beat2}$
Substituting the known values:
$|f_A' - 380\text{ Hz}| = 2\text{ Hz}$
This equation yields two possible values for the new frequency $f_A'$:
We need to determine which of the initial possibilities for $f_A$ ($384\text{ Hz}$ or $376\text{ Hz}$) is consistent with the frequency decrease upon loading and the observed change in beat frequency.
Therefore, the original frequency of tuning fork A must be $384\text{ Hz}$.
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)