/*! 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} Problem 6 A man strikes one end of a thin ... [FREE SOLUTION] | 91Ó°ÊÓ

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A man strikes one end of a thin rod with a hammer. The speed of sound in the rod is 15 times the speed of sound in air. A woman, at the other end with her ear close to the rod, hears the sound of the blow twice with a \(0.12\) s interval between; one sound comes through the rod and the other comes through the air alongside the rod. If the speed of sound in air is \(343 \mathrm{~m} / \mathrm{s}\), what is the length of the rod?

Short Answer

Expert verified
The length of the rod is approximately 70.57 meters.

Step by step solution

01

Understand the Sound Speed Relationship

The speed of sound in the rod is given as 15 times the speed of sound in air. So, if the speed of sound in air is 343 m/s, then the speed of sound in the rod is \(15 \times 343 = 5145\, \text{m/s}\).
02

Determine the Time Intervals for Sound

The time it takes for the sound to travel through the rod and the air results in a 0.12-second interval between the two sounds. Let the time taken for sound through air be \(t_{air}\) and through the rod be \(t_{rod}\). We have \(t_{air} - t_{rod} = 0.12 \text{ s}\).
03

Set Up the Equations for the Times

The distances traveled by both sounds are equal to the length of the rod, \(L\). Thus, \(L = v_{air} \times t_{air}\) for air and \(L = v_{rod} \times t_{rod}\) for the rod. Substitute the given speed values: \(L = 343 \times t_{air}\) and \(L = 5145 \times t_{rod}\).
04

Express Time for Each Medium

From the equations in the previous step, we have \(t_{air} = \frac{L}{343}\) and \(t_{rod} = \frac{L}{5145}\).
05

Solve for Length Using the Time Difference

Substitute the expressions for \(t_{air}\) and \(t_{rod}\) into the time difference equation: \(\frac{L}{343} - \frac{L}{5145} = 0.12\).
06

Solve the Length Equation

This simplifies to \(L \left(\frac{1}{343} - \frac{1}{5145}\right) = 0.12\). Calculate the fractional difference: \(\frac{1}{343} - \frac{1}{5145} = \frac{5145 - 343}{343 \times 5145}\). Evaluate it and solve for \(L\), resulting in \(L \approx 70.57 \text{ meters}\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Speed of Sound
The speed of sound is an essential concept in physics, describing how quickly sound waves travel through different media. Typically, the speed of sound is faster in solid materials like metal rods than in gases like air. This is because molecules in solids are packed more closely together, allowing sound waves to travel more efficiently from one molecule to the next.
This exercise highlights that the speed of sound in the rod is much higher than in air, quantified as 15 times higher.
  • Speed in air: 343 m/s
  • Speed in rod: 5145 m/s (which is 15 times the speed in air)
Understanding these speed differences is crucial to solve problems involving sound propagation through multiple media.
Time Intervals
The time interval, in this context, refers to the difference in time between two events—in this case, the arrival of sounds through two different paths. The hammer strike creates two sound waves: one travels through the rod, and the other travels through the air.
The problem states there's a 0.12-second interval between these sounds reaching the listener. This time difference arises because of the different speeds at which sound travels through air and the rod. To calculate this, we denote:
  • The time for sound through air as \(t_{air}\)
  • The time for sound through the rod as \(t_{rod}\)
The relationship between these times is given as \(t_{air} - t_{rod} = 0.12\, \text{s}\). Understanding how to parse these intervals helps to determine the length of the rod or the time taken for sound travel.
Sound Waves
Sound waves are practically energy traveling through a medium, be it air, water, or solid materials like rods. They are mechanical waves that require a medium to travel and are characterized by their speed, frequency, and wavelength.
Sound waves transmitted through the rod and air exhibit different characteristics due to their respective speeds. When a hammer strikes the rod, it creates a vibration that turns into two separate traveling waves—one through the rod and one through the air. The physical properties of the rod and air directly influence these waves' behavior.
  • Molecules in the rod (a solid medium) are denser and convey the energy faster.
  • Air molecules are less dense, resulting in slower wave propagation.
This understanding is key to solving the rod length problem, as the distinction between wave travel in different media causes the time interval experienced.
Mathematical Equations
Mathematical equations allow us to quantify the relationships between physical phenomena like sound travel. In this problem, the goal is to solve for the rod's length using time and speed equations. To solve, we express the length of the rod, \(L\), in terms of time:
  • For air: \(L = v_{air} \times t_{air}\)
  • For the rod: \(L = v_{rod} \times t_{rod}\)
Plugging the speed values gives us:
  • \(L = 343 \times t_{air}\)
  • \(L = 5145 \times t_{rod}\)
From here, you use the known time interval \(t_{air} - t_{rod} = 0.12\) to express \(t_{air}\) and \(t_{rod}\) as \(\frac{L}{343}\) and \(\frac{L}{5145}\), respectively.By substituting these into the time difference equation, \(\frac{L}{343} - \frac{L}{5145} = 0.12\), one can solve the linear equation for \(L\). Careful handling of these equations reveals the rod length, about 70.57 meters. Understanding such mathematical frameworks is essential for accurately solving physics problems.

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Most popular questions from this chapter

Two loud speakers are located \(3.35 \mathrm{~m}\) apart on an outdoor stage. A listener is \(18.3 \mathrm{~m}\) from one and \(19.5 \mathrm{~m}\) from the other. During the sound check, a signal generator drives the two speakers in phase with the same amplitude and frequency. The transmitted frequency is swept through the audible range \((20 \mathrm{~Hz}\) to \(20 \mathrm{kHz}) .\) (a) What is the lowest frequency \(f_{\min , 1}\) that gives minimum signal (destructive interference) at the listener's location? By what number must \(f_{\min , 1}\) be multiplied to get (b) the second lowest frequency \(f_{\min 2}\) that gives minimum signal and (c) the third lowest frequency \(f_{\min , 3}\) that gives minimum signal? (d) What is the lowest frequency \(f_{\max , 1}\) that gives maximum signal (constructive interference) at the listener's location? By what number must \(f_{\max , 1}\) be multiplied to get (e) the second lowest frequency \(f_{\max , 2}\) that gives maximum signal and (f) the third lowest frequency \(f_{\max , 3}\) that gives maximum signal?

Ultrasound, which consists ultrasour of sound waves with frequencies above the human audible range, can Artery be used to produce an image of the interior of a human body. Moreover, ultrasound can be used to measure Figure 17-47 Problem \(83 .\) the speed of the blood in the body; it does so by comparing the frequency of the ultrasound sent into the body with the frequency of the ultrasound reflected back to the body's surface by the blood. As the blood pulses, this detected frequency varies. Suppose that an ultrasound image of the arm of a patient shows an artery that is angled at \(\theta=20^{\circ}\) to the ultrasound's line of travel (Fig. 17-47). Suppose also that the frequency of the ultrasound reflected by the blood in the artery is increased by a maximum of \(5495 \mathrm{~Hz}\) from the original ultrasound frequency of \(5.000000 \mathrm{MHz} .\) (a) In Fig. \(17-47\), is the direction of the blood flow rightward of leftward? (b) The speed of sound in the human arm is \(1540 \mathrm{~m} / \mathrm{s}\). What is the maximum speed of the blood? (Hint: The Doppler effect is caused by the component of the blood's velocity along the ultrasound's direction of travel.) (c) If angle \(\theta\) were greater, would the reflected frequency be greater or less?

A sound source moves along an \(x\) axis, between detectors \(A\) and \(B .\) The wavelength of the sound detected at \(A\) is \(0.500\) that of the sound detected at \(B .\) What is the ratio \(v_{s} / v\) of the speed of the source to the speed of sound?

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