In this problem, we are dealing with resonance in two air columns that are closed at one end. The lengths of these air columns are 100 cm and 120 cm. They both produce sounds in their respective fundamental modes and produce 15 beats per second. We need to find the velocity of sound in these air columns.
To solve this, we start by using the formula for the frequency of a closed-end air column in its fundamental mode:
\(f = \frac{v}{4L}\)
where:
Let the frequencies of the air columns be \(f_1\) and \(f_2\) for lengths 100 cm and 120 cm respectively. Then, we have:
Given that they produce 15 beats per second, the difference in frequency is:
\(|f_1 - f_2| = 15\)
Substituting the expressions for \(f_1\) and \(f_2\):
\(\left|\frac{v}{400} - \frac{v}{480}\right| = 15\)
By simplifying the difference:
\(\frac{v}{400} - \frac{v}{480} = 15\)
Find a common denominator (2400 in this case) to combine the fractions:
\(\frac{6v}{2400} - \frac{5v}{2400} = 15\)
This simplifies to:
\(\frac{v}{2400} = 15\)
Multiplying through by 2400 gives:
\(v = 15 \times 2400 = 36000 \; \text{cm/s} = 360 \; \text{m/s}\)
Therefore, the velocity of sound in the air columns is 360 m/s. This corresponds to the given option: 360 m/s.
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,

Two resistances of 100Ω and 200Ω are connected in series with a battery of 4V and negligible internal resistance. A voltmeter is used to measure voltage across the 100Ω resistance, which gives a reading of 1V. The resistance of the voltmeter must be _____ Ω.
What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)