The frequency of vibration of a sonometer wire is given by:
\(f = \frac{1}{2L} \sqrt{\frac{T}{\mu}}\)
Calculating for initial tension:
\(f_1 = \frac{1}{2} \sqrt{\frac{6}{\mu}}\)
Calculating for new tension:
\(f_2 = \frac{1}{2} \sqrt{\frac{54}{\mu}}\)
Given:
\(f_2 - f_1 = 12\)
Ratio of frequencies:
\(\frac{f_1}{f_2} = \frac{1}{3}\)
Substituting values:
\(f_1 = 6 \, \text{Hz}\)
The problem requires finding the frequency of a tuning fork by analyzing its interaction with a sonometer wire under two different tension conditions: one of resonance and another that produces beats.
1. Frequency of a Stretched String: The fundamental frequency (\( f \)) of a string vibrating in one segment is given by the formula:
\[ f = \frac{1}{2L} \sqrt{\frac{T}{\mu}} \]where \( L \) is the length of the string, \( T \) is the tension, and \( \mu \) is the linear mass density (mass per unit length).
2. Proportionality: For a given sonometer wire of fixed length (\(L\)) and linear mass density (\(\mu\)), the frequency is directly proportional to the square root of the tension:
\[ f \propto \sqrt{T} \]3. Resonance: When the tuning fork resonates with the sonometer wire, their frequencies are equal.
4. Beats: When two sound sources of slightly different frequencies are sounded together, the beat frequency (\( f_{\text{beat}} \)) is the absolute difference between their individual frequencies:
\[ f_{\text{beat}} = |f_a - f_b| \]Step 1: Define the frequencies for the initial and final conditions.
Let the frequency of the tuning fork be \( f_{\text{fork}} \).
In the initial case, the tension is \( T_1 = 6 \, \text{N} \). Let the frequency of the sonometer wire be \( f_1 \). Since the wire resonates with the tuning fork, we have:
In the final case, the tension is changed to \( T_2 = 54 \, \text{N} \). Let the new frequency of the wire be \( f_2 \). The tuning fork produces 12 beats per second with the wire, so:
\[ |f_2 - f_{\text{fork}}| = 12 \, \text{Hz} \]Step 2: Find the relationship between the two frequencies of the wire, \( f_1 \) and \( f_2 \).
Using the proportionality \( f \propto \sqrt{T} \), we can write the ratio of the frequencies:
\[ \frac{f_2}{f_1} = \sqrt{\frac{T_2}{T_1}} \]Substitute the given tension values:
\[ \frac{f_2}{f_1} = \sqrt{\frac{54}{6}} = \sqrt{9} = 3 \]This gives us the relationship:
\[ f_2 = 3f_1 \]Step 3: Use the beat frequency equation to solve for the frequencies.
We have three relations: 1. \( f_1 = f_{\text{fork}} \) 2. \( |f_2 - f_{\text{fork}}| = 12 \) 3. \( f_2 = 3f_1 \)
Substitute (1) into (3):
\[ f_2 = 3f_{\text{fork}} \]Now substitute this into the beat frequency equation (2):
\[ |3f_{\text{fork}} - f_{\text{fork}}| = 12 \]Simplify the expression:
\[ |2f_{\text{fork}}| = 12 \]Since frequency must be a positive value, we can remove the absolute value bars.
\[ 2f_{\text{fork}} = 12 \] \[ f_{\text{fork}} = \frac{12}{2} = 6 \, \text{Hz} \]The frequency of the tuning fork is 6 Hz.
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,


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 : \(A_2 \rightleftharpoons 2A\)