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 $384\text{ Hz}$.
A particle is subjected to two simple harmonic motions as :
$x_1 = \sqrt{7} \sin 5t \text{ cm}$ and $x_2 = 2\sqrt{7} \sin \left(5t + \frac{\pi}{3}\right) \text{ cm}$
where x is displacement and t is time in seconds. The maximum acceleration of the particle is $x \times 10^{-2} \text{ ms}^{-2}$. The value of x is :
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
In an open organ pipe $\nu_3$ and $\nu_6$ are $3^{\text{rd}}$ and $6^{\text{th}}$ harmonic frequencies, respectively. If $\nu_6 - \nu_3 = 2200 \text{ Hz}$ then length of the pipe is _________ mm.
(Take velocity of sound in air is $330 \text{ m/s}$.)
A particle is subjected to two simple harmonic motions as :
$x_1 = \sqrt{7} \sin 5t \text{ cm}$ and $x_2 = 2\sqrt{7} \sin \left(5t + \frac{\pi}{3}\right) \text{ cm}$
where x is displacement and t is time in seconds. The maximum acceleration of the particle is $x \times 10^{-2} \text{ ms}^{-2}$. The value of x is :
The displacement of a plane progressive wave in a medium, travelling towards positive x-axis with velocity 4 m/s at t = 0 is given by \(y = 3\sin 2\pi\left(-\dfrac{x}{3}\right)\). Then the expression for the displacement at a later time t = 4 sec will be