/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q11E Question: A 60.0-m-long brass r... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

Question:A 60.0-m-long brass rod is struck at one end. A person at the other end hears two sounds as a result of two longitudinal waves, one traveling in the metal rod and the other traveling in air. What is the time interval between the two sounds? (The speed of sound in air is 344 m/s; see Tables 11.1 and 12.1 for relevant information about brass.)

Short Answer

Expert verified

The time interval between two sounds is 0.1559 s.

Step by step solution

01

Given data

The given data can be listed below as,

  • The length of the brass rod is,\(l = 60\;{\rm{m}}\).
  • The sounds are heard by the person; one is traveling in metal, and the second is traveling in the air.
02

Concept

When a sound wave is moving in a medium, the type of medium will affect the properties or characteristics of the respective sound wave. Two sound waves traveling in two different mediums will have different values of physical quantities associated with them.

03

Determination of the time interval of two sounds

For metal brass:

The wave is traveling in brass.

The velocity of the wave can be calculated as,

\(v = \sqrt {\frac{Y}{\rho }} \)

Here\(Y\)is the young modulus of the elasticity of brass metal and \(\rho \)is the density of brass.

From tables 11.1 and 12.1, we can obtain,

\(Y = 9 \times {10^{10}}\;{\rm{Pa}}\)and\(\rho = 8600\;{\rm{kg/}}{{\rm{m}}^{\rm{3}}}\).

Substitute these values in the above expression, and we get,

\(\begin{array}{c}{v_{{\rm{brass}}}} = \sqrt {\frac{{9 \times {{10}^{10}}\;{\rm{Pa}}}}{{8600\;{\rm{kg/}}{{\rm{m}}^{\rm{3}}}}}} \\ = \sqrt {\frac{{9 \times {{10}^{10}}}}{{8600}} \cdot \left( {\frac{{1\;{\rm{Pa}}}}{{1\;{\rm{kg/}}{{\rm{m}}^{\rm{3}}}}} \times \frac{{1\;{\rm{kg}} \cdot {\rm{m}} \cdot {{\rm{s}}^{ - {\rm{2}}}}}}{{1\;{\rm{N}}}} \times \frac{{1\;{\rm{N}} \cdot {{\rm{m}}^{ - 2}}}}{{1\;{\rm{Pa}}}}} \right)} \\ = \sqrt {10465116.28 \cdot {{\left( {1\;{\rm{m/s}}} \right)}^2}} \\ = 3234.98\;{\rm{m/s}}\end{array}\)

The time taken by the sound wave to reach the distance of 60 m can be calculated as,

\({t_1} = 60\;{\rm{m}}/{v_{{\rm{brass}}}}\)

Substitute the value in the above expression, and we get,

\(\begin{array}{c}{t_1} = 60\;{\rm{m}}/3234.98\;{\rm{m/s}}\\{t_1} = {\rm{0}}{\rm{.0185}}\;{\rm{s}}\end{array}\) (1)

For Air:

The velocity of the sound wave in the air is 344 m/s.

The time taken by the sound wave to reach the distance of 60 m can be calculated as,

\(\begin{array}{c}{t_2} = 60\;{\rm{m}}/344\;{\rm{m/s}}\\{t_2} = 0.1744\;{\rm{s}}\end{array}\) (2)

The time interval between two sounds can be calculated as,

\(\Delta t = {t_2} - {t_1}\)

Substitute the values from equations 1 and 2 in the above expression, and we get,

\(\begin{array}{c}\Delta t = 0.1744\;{\rm{s}} - {\rm{0}}{\rm{.0185}}\;{\rm{s}}\\ = 0.1559\;{\rm{s}}\end{array}\)

Thus, the time interval between two waves is 0.1559 s.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91Ó°ÊÓ!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

A uniform 165-Nbar is supported horizontally by two identical wires A and B (Fig. P16.62). A small 185-N cube of lead is placed three fourths of the way from A to B. The wires are each 75.0 cm long and have a mass of 5.50 g. If both of them are simultaneously plucked at the centre, what is the frequency of the beats that they will produce when vibrating in their fundamental?

The portion of the string of a certain musical instrument between the bridge and upper end of the finger board (that part of the string that is free to vibrate) is \(60.0\;{\rm{cm}}\) long, and this length of the string has mass \(2.00\;{\rm{g}}\). The string sounds an \({A_4}\) note (\(440\;{\rm{Hz}}\)) when played.

(a) Where must the player put a finger (what distance x from the bridge) to play a \({D_5}\) note (\(587\;{\rm{Hz}}\))? (See Fig. E15.45.) For both the \({A_4}\) and \({D_5}\) notes, the string vibrates in its fundamental mode.

(b) Without retuning, is it possible to play a \({G_4}\) note (\(392\;{\rm{Hz}}\)) on this string? Why or why not?

Interference of Triangular Pulses. Two triangular wave pulses are traveling toward each other on a stretched string as shown in Fig. E15.32. Each pulse is identical to the other and travels at \(2.00\;{{{\rm{cm}}} \mathord{\left/ {\vphantom {{{\rm{cm}}} {\rm{s}}}} \right. \\} {\rm{s}}}\). The leading edges of the pulses are \(1.00\;{\rm{cm}}\) apart at \(t = 0\). Sketch the shape of the string at \(t = 0.250\;{\rm{s}}\), \(t = 0.500\;{\rm{s}}\), \(t = 0.750\;{\rm{s}}\), \(t = 1.000\;{\rm{s}}\), and \(t = 1.250\;{\rm{s}}\)

On the planet Arrakis a male ornithoid is flying toward his mate at 25 m/swhile singing at a frequency of 1200 â¶Ä‰Hz. If the stationary female hears a tone of 1240 â¶Ä‰Hz, what is the speed of sound in the atmosphere of Arrakis?

You blow across the open mouth of an empty test tube and produce the fundamental standing wave of the air column inside the test tube. The speed of sound in air is 344 m/s and the test tube act as a stopped pipe. (a) If the length of the air column in the test tube is 14.0 cm, what is the frequency of this standing wave? (b) What is the frequency of the fundamental standing wave in the air column if the test tube is half filled with water?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.