Two vibrating strings of the same material but of lengths Land \(2 \mathrm{~L}\) have radii \(2 \mathrm{r}\) and \(\mathrm{r}\) respectively. They are stretched under the same tension. Both the string vibrate in their fundamental modes. The one of length \(\mathrm{L}\) with frequency \(\mathrm{U}_{1}\) and the other with frequency \(\mathrm{U}_{2}\). What is the ratio $\left(\mathrm{U}_{1} / \mathrm{U}_{2}\right)$ ? (A) 8 (B) 2 (C) 1 (D) 4

Short Answer

Expert verified
The ratio \(\frac{U_{1}}{U_{2}}\) is 2. (B)

Step by step solution

01

Understand the properties of the two strings

We are given two vibrating strings with the following properties: String 1: Length L, radius 2r, fundamental frequency U1 String 2: Length 2L, radius r, fundamental frequency U2 Both strings are of the same material and are stretched under the same tension.
02

Recall the formula for the fundamental frequency of a vibrating string

The fundamental frequency of a vibrating string is given by: \[ \, f = \frac{1}{2L} \sqrt{\frac{T}{\mu}} \, \] Where \(f\) is the frequency, \(L\) is the length of the string, \(T\) is the tension, and \(\mu\) is the linear mass density.
03

Express linear mass density in terms of radius

The linear mass density, \(\mu\), is defined as the mass per unit length: \[ \mu = \frac{m}{L} \] For a string with radius \(r\) and length \(L\), its volume is given by: \[ V=r^2 L\pi \] Mass can be expressed as a product of volume and density: \[ m = \rho V \] Substituting volume into the mass equation, we get: \[ m = \rho\pi r^2 L \] Now, we can express the linear mass density in terms of radius: \[ \mu = \frac{m}{L} = \rho\pi r^2 \]
04

Calculate the fundamental frequencies for both strings

To find the fundamental frequencies of both strings, we need to apply the formula we derived earlier: For String 1, use the values \(L\), \(2r\) for radius, and the same tension \(T\). \[ f_1 = \frac{1}{2L} \sqrt{\frac{T}{\rho\pi(2r)^2}} \] For String 2, use the values \(2L\), \(r\) for radius, and the same tension \(T\). \[ f_2 = \frac{1}{4L} \sqrt{\frac{T}{\rho\pi r^2}} \]
05

Calculate the ratio U1 / U2

We need to find the ratio of the fundamental frequencies: \[ \frac{f_1}{f_2}=\frac{\left(\frac{1}{2L} \sqrt{\frac{T}{\rho\pi(2r)^2}}\right)}{\left(\frac{1}{4L} \sqrt{\frac{T}{\rho\pi r^2}}\right)} \] Simplify: \[ \frac{f_1}{f_2}=\frac{\left(\frac{1}{2L} \sqrt{\frac{T}{4\rho\pi r^2}}\right)}{\left(\frac{1}{4L} \sqrt{\frac{T}{\rho\pi r^2}}\right)} \] Cancel out common factors, and the ratio becomes: \[ \frac{f_1}{f_2}=\frac{2 \sqrt{\frac{1}{4}}}{\sqrt{1}}=\frac{1}{2} \] However, the question asks for the ratio \(\frac{U_{1}}{U_{2}}\), which is the inverse of the ratio \(\frac{f_1}{f_2}\). So, taking the inverse of the ratio we calculated: \[ \frac{U_{1}}{U_{2}}=\frac{1}{\frac{1}{2}}=2 \] The ratio U1 / U2 is 2, so the correct answer is (B) 2.

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Most popular questions from this chapter

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 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 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) \(10 \mathrm{~g}\)

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) \(93.75\)

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