An open pipe is in resonance in \(2^{\text {nd }}\) harmonic with frequency \(\mathrm{f}_{1}\). Now one end of the tube is closed and frequency is increased to \(\mathrm{f}_{2}\) such that the resonance again occurs in nth harmonic. Choose the correct option. (A) \(\mathrm{n}=5, \mathrm{f}_{2}=(5 / 4) \mathrm{f}_{1}\) (B) \(\mathrm{n}=3, \mathrm{f}_{2}=(3 / 4) \mathrm{f}_{1}\) (C) \(\mathrm{n}=5, \mathrm{f}_{2}=(3 / 4) \mathrm{f}_{1}\) (D) \(\mathrm{n}=3, \mathrm{f}_{2}=(5 / 4) \mathrm{f}_{1}\)

Short Answer

Expert verified
The correct option is (B) with n = 3 and the relationship between f1 and f2 as \(f_2 = \frac{3}{4}f_1\).

Step by step solution

01

Resonance formula for an open pipe

For an open pipe, the resonance formula says that when a pipe is in resonance, the frequency is given by \[f = \frac{2n}{L} \times v\] where n is the harmonic number, L is the length of the pipe, and v is the speed of sound.
02

Given conditions for the open pipe

We are given that the open pipe is in resonance in the 2nd harmonic with frequency f1. Using the formula from Step 1, we can write the frequency equation for the open pipe: \[f_1 = \frac{4}{L} \times v\]
03

Resonance formula for a closed pipe

For a closed pipe, the resonance formula says that when a closed pipe is in resonance, the frequency is given by \[f = \frac{2n - 1}{4L} \times v\] where n is the harmonic number, L is the length of the pipe, and v is the speed of sound.
04

Given conditions for the closed pipe

We are given that the closed pipe is in resonance in the nth harmonic with frequency f2. Using the formula from Step 3, we can write the frequency equation for the closed pipe: \[f_2 = \frac{2n - 1}{4L} \times v\]
05

Relate f1 and f2

Now we need to find a relationship between f1 and f2 using the equations from Steps 2 and 4. We can do this by dividing the equation of f2 by the equation of f1: \[\frac{f_2}{f_1} = \frac{(2n - 1)/4L}{4/L}\]
06

Simplify the relationship

After simplifying the relationship from Step 5, we have: \[\frac{f_2}{f_1} = \frac{2n -1}{16}\]
07

Check for the correct answer

Now that we have a relationship between f1 and f2, we must check the provided options to find the correct one. For this, we need to plug in the given values of n and f2/f1 into the relationship from Step 6. Let's first plug the values from Option (A): \(n = 5, f_2 = (5/4)f_1\) \[\frac{5}{4} = \frac{2(5) - 1}{16} \implies \frac{5}{4} = \frac{9}{16}\] This is not correct. Now plug the values from Option (B): \(n = 3, f_2 = (3/4)f_1\) \[\frac{3}{4} = \frac{2(3) - 1}{16} \implies \frac{3}{4} = \frac{5}{16}\] This is correct. There is no need to check more options as we have already found the correct answer. The correct option is (B). So, n = 3, and the relationship between f1 and f2 is \[f_2 = \frac{3}{4}f_1\]

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Most popular questions from this chapter

An air column in a pipe, which is closed at one end will be in resonance with a vibrating tuning fork of frequency \(264 \mathrm{~Hz}\), What is the length of the column if it is in \(\mathrm{cm} ?\) (speed of sound in \(\operatorname{air}=330 \mathrm{~m} / \mathrm{s}\) ) (A) \(62.50\) (B) \(15.62\) (C) 125 (D) \(93.75\)

A tube, closed at one end and containing air, produces, when excited, the fundamental note of frequency \(512 \mathrm{~Hz}\). If the tube is opened at both ends what is the fundamental frequency that can be excited (in \(\mathrm{Hz}\) )? (A) 256 (B) 1024 (C) 128 (D) 512

A closed organ pipe of length \(\mathrm{L}\) and an open organ pipe contain gases of densities \(\rho_{1}\) and \(\rho_{2}\) respectively. The compressibility of gases are equal in both the pipes. Both the pipes are vibrating in their first overtone with same frequency. What is the length of the open organ pipe? (A) \(\left.(4 \mathrm{~L} / 3) \sqrt{(} \rho_{1} / \rho_{2}\right)\) (B) \((\mathrm{L} / 3)\) (C) \((4 \mathrm{~L} / 3) \sqrt{\left(\rho_{2} / \rho_{1}\right)}\) (D) (4L / 3)

A tuning fork of \(512 \mathrm{~Hz}\) is used to produce resonance in a resonance tube experiment. The level of water at first resonance is $30.7 \mathrm{~cm}\( and at second resonance is \)63.2 \mathrm{~cm}$. What is the error in calculating velocity of sound? Assume the speed of sound $330 \mathrm{~m} / \mathrm{s}$. (A) \(58(\mathrm{~cm} / \mathrm{s})\) (B) \(204.1(\mathrm{~cm} / \mathrm{s})\) (C) \(280(\mathrm{~cm} / \mathrm{s})\) (D) \(110(\mathrm{~cm} / \mathrm{s})\)

A hollow pipe of length \(0.8 \mathrm{~m}\) is closed at one end. At its open end a \(0.5 \mathrm{~m}\) long uniform string is vibrating in its second harmonic and it resonates with the fundamentals frequency of the pipe if the tension in the wire is \(50 \mathrm{~N}\) and the speed of sound is $320 \mathrm{~ms}^{-1}$, what is the mass of the string. (A) \(20 \mathrm{~g}\) (B) \(5 \mathrm{~g}\) (C) \(40 \mathrm{~g}\) (D) \(10 \mathrm{~g}\)

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