Problem Analysis: The question involves calculating the frequency of a tuning fork based on the number of beats heard when sounded with a sonometer wire at two different lengths. The key concepts are the phenomenon of beats and the relationship between the frequency of a sonometer wire and its length.
Beats occur when two sound waves of slightly different frequencies interfere. The number of beats per second is equal to the absolute difference between the two frequencies. For a sonometer wire, the fundamental frequency ($f$) is inversely proportional to its length ($L$), assuming tension ($T$) and linear density ($m$) are constant. Mathematically, $f \propto 1/L$.
Let $f_f$ be the frequency of the tuning fork. Let $f_{w1}$ be the frequency of the sonometer wire when its length is $L_1 = 0.95$ m. Let $f_{w2}$ be the frequency of the sonometer wire when its length is $L_2 = 1$ m.
Since frequency is inversely proportional to length, a shorter length produces a higher frequency. Thus, $f_{w1} > f_{w2}$.
We are given that 5 beats/second are heard in both cases. This means:
From these two equations, we can infer that the tuning fork's frequency $f_f$ must lie exactly midway between the two wire frequencies $f_{w1}$ and $f_{w2}$. This implies:
$f_f = \frac{f_{w1} + f_{w2}}{2}$
Also, the difference between the wire frequencies is twice the beat frequency:
$f_{w1} - f_{w2} = 2 \times 5 = 10$ Hz
We know $f_w = k/L$, where $k$ is a constant related to tension and linear density.
$f_{w1} = k / 0.95$
$f_{w2} = k / 1$
Substitute these into the difference equation:
$\frac{k}{0.95} - \frac{k}{1} = 10$
$k \left( \frac{1}{0.95} - 1 \right) = 10$
$k \left( \frac{1 - 0.95}{0.95} \right) = 10$
$k \left( \frac{0.05}{0.95} \right) = 10$
$k = 10 \times \frac{0.95}{0.05} = 10 \times 19 = 190$
Now, calculate $f_{w1}$ and $f_{w2}$:
$f_{w1} = \frac{190}{0.95} = 200$ Hz
$f_{w2} = \frac{190}{1} = 190$ Hz
Check: $f_{w1} - f_{w2} = 200 - 190 = 10$ Hz. This is consistent.
Use the formula derived earlier:
$f_f = \frac{f_{w1} + f_{w2}}{2}$
$f_f = \frac{200 \text{ Hz} + 190 \text{ Hz}}{2}$
$f_f = \frac{390 \text{ Hz}}{2}$
$f_f = 195$ Hz
Verify the beats:
$|f_f - f_{w1}| = |195 - 200| = |-5| = 5$ beats/sec
$|f_f - f_{w2}| = |195 - 190| = |5| = 5$ beats/sec
Both conditions are satisfied.
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)