To solve this problem, we need to understand the concept of resonance in air columns that are closed at one end. In a closed pipe, the fundamental frequency of vibration is determined by the formula:
f = \frac{v}{4L}
where f is the frequency, v is the velocity of sound, and L is the length of the air column.
Let's denote L_1 = 100 \text{ cm} = 1 \text{ m} and L_2 = 120 \text{ cm} = 1.2 \text{ m}. The frequencies of these two columns in their fundamental modes are:
f_1 = \frac{v}{4 \times 1} = \frac{v}{4}
f_2 = \frac{v}{4 \times 1.2} = \frac{v}{4.8}
The problem states that these two frequencies produce 15 beats per second:
|f_1 - f_2| = 15
Substitute the expressions for f_1 and f_2:
\left|\frac{v}{4} - \frac{v}{4.8}\right| = 15
Calculate the difference inside the absolute value:
\frac{v}{4} - \frac{v}{4.8} = \frac{v \cdot 4.8 - v \cdot 4}{4 \cdot 4.8}
\frac{v(4.8 - 4)}{19.2} = \frac{0.8v}{19.2} = \frac{v}{24}
Therefore, the equation becomes:
\frac{v}{24} = 15 \quad \Rightarrow \quad v = 15 \times 24 = 360 \text{ m/s}
Thus, the velocity of sound in the air column is 360 m/s.
The correct answer is 360 \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 :

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)
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 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 :