/*! 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 17 Two loud speakers are located \(... [FREE SOLUTION] | 91Ó°ÊÓ

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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?

Short Answer

Expert verified
(a) 142.92 Hz; (b) 3; (c) 5; (d) 285.83 Hz; (e) 2; (f) 3.

Step by step solution

01

Understanding the Concept of Interference

For destructive interference, the path difference must be an odd multiple of half the wavelength, i.e., \((2n+1)\frac{\lambda}{2}\) where \(n = 0, 1, 2, \ldots\). For constructive interference, the path difference is an integer multiple of the wavelength \(m\lambda\) where \(m = 0, 1, 2, \ldots\).
02

Calculate Path Difference

Find the path difference \(\Delta L\) using the distances from the listener to each speaker: \(\Delta L = 19.5 \text{m} - 18.3 \text{m} = 1.2 \text{m}\).
03

Frequency for Minimum Signal (Destructive Interference)

For the lowest frequency giving destructive interference: \(\Delta L = (2n+1)\frac{\lambda}{2}, n=0\). Using the speed of sound \(c = 343\text{ m/s}\), \(\lambda = \frac{c}{f}\). Set \(\Delta L = \frac{\lambda}{2}\): \[1.2 = \frac{343}{2f_{\min, 1}}\].Solve for \(f_{\min, 1}\): \[f_{\min, 1} = \frac{343}{2 \times 1.2} \approx 142.92 \text{Hz}\].
04

Further Destructive Interference Frequencies

For consecutive destructive frequencies: \(f_{\min, 2} = 3f_{\min, 1}\) and \(f_{\min, 3} = 5f_{\min, 1}\). Thus, the multipliers are 3 and 5.
05

Frequency for Maximum Signal (Constructive Interference)

Set \(\Delta L = m\lambda, m=1\): \[1.2 = \frac{343}{f_{\max, 1}}\].Solve for \(f_{\max, 1}\): \[f_{\max, 1} = \frac{343}{1.2} \approx 285.83 \text{Hz}\].
06

Further Constructive Interference Frequencies

For consecutive constructive frequencies: \(f_{\max, 2} = 2f_{\max, 1}\) and \(f_{\max, 3} = 3f_{\max, 1}\). Thus, the multipliers are 2 and 3.

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Key Concepts

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

Destructive Interference
Destructive interference occurs when two waves meet and effectively cancel each other out. This happens when the path difference between the two waves is such that they are out of phase. For destructive interference to occur, the path difference must be an odd multiple of half the wavelength, given by the formula \[(2n+1)\frac{\lambda}{2}\]where \(n\) is an integer (0, 1, 2, ...).

In the given problem, the path difference between the two waves is calculated as 1.2 meters. To determine the lowest frequency that results in destructive interference, the path difference is equated to half the wavelength. By using the speed of sound (343 m/s), you can solve for the frequency:
\[f_{\min, 1} = \frac{343}{2 \times 1.2} \approx 142.92 \text{ Hz}\]This frequency creates the first instance of destructive interference at the listener's location.
Constructive Interference
Constructive interference happens when two waves meet in phase and reinforce each other. The resulting wave amplitude is larger, leading to a maximum signal. For constructive interference, the path difference corresponds to a whole number multiple of the wavelength:\[m\lambda\]where \(m\) is an integer (0, 1, 2, ...).

In this problem, the path difference between the sound waves from the two speakers is also 1.2 meters. To find the lowest frequency for constructive interference, set the path difference equal to a full wavelength and solve for the frequency:
\[f_{\max, 1} = \frac{343}{1.2} \approx 285.83 \text{ Hz}\]This frequency gives the listener a maximum signal as the waves construct upon each other in phase.
Audible Frequency Range
The human ear is capable of hearing a wide range of frequencies, from 20 Hz to 20 kHz. This range is known as the audible frequency range. In this exercise, the sound frequency transmitted by the speakers is swept across this range. It's essential in practical applications, such as testing audio equipment or acoustics in architecture.

In the context of wave interference, only certain frequencies within this range will lead to noticeable destructive or constructive interference, given the listener's fixed position. Identifying these frequencies requires calculating based on the speaker's distance from the listener and the speed of sound.
Path Difference
The path difference is crucial in determining how waves interfere at a listener's location. It is the difference in distance traveled by two waves before they meet at a point. Path difference determines whether the interference will be constructive or destructive, based on relative phase differences of the waves.

In this scenario, the listener is 18.3 m from one speaker and 19.5 m from the other, resulting in a path difference of:\[\Delta L = 19.5 \text{ m} - 18.3 \text{ m} = 1.2 \text{ m}\]This constant path difference is used to find frequencies for which the interfering sound waves either cancel out (destructive) or strengthen (constructive) each other, determining the quality of the sound heard by the listener.

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Most popular questions from this chapter

Hot chocolate effect. Tap a metal spoon inside a mug of water and note the frequency \(f_{i}\) you hear. Then add a spoonful of powder (say, chocolate mix or instant coffee) and tap again as you stir the powder. The frequency you hear has a lower value \(f_{s}\) because the tiny air bubbles released by the powder change the water's bulk modulus. As the bubbles reach the water surface and disappear, the frequency gradually shifts back to its initial value. During the effect, the bubbles don't appreciably change the water's density or volume or the sound's wavelength.

Two identical piano wires have a fundamental frequency of \(600 \mathrm{~Hz}\) when kept under the same tension. What fractional increase in the tension of one wire will lead to the occurrence of \(6.0\) beats/s when both wires oscillate simultaneously?

A sperm whale (Fig. \(17-44 a\) ) vocalizes by producing a series of clicks. Actually, the whale makes only a single sound near the front of its head to start the series. Part of that sound then emerges from the head into the water to become the first click of the series. The rest of the sound travels backward through the spermaceti sac (a body of fat), reflects from the frontal sac (an air layer), and then travels forward through the spermaceti sac. When it reaches the distal sac (another air layer) at the front of the head, some of the sound escapes into the water to form the second click, and the rest is sent back through the spermaceti sac (and ends up forming later clicks). Figure \(17-44 b\) shows a strip-chart recording of a series of clicks. A unit time interval of \(1.0 \mathrm{~ms}\) is indicated on the chart. Assuming that the speed of sound in the spermaceti sac is \(1372 \mathrm{~m} / \mathrm{s}\), find the length of the spermaceti sac. From such a calculation, marine scientists estimate the length of a whale from its click series.

Organ pipe \(A\), with both ends open, has a fundamental frequency of \(300 \mathrm{~Hz}\). The third harmonic of organ pipe \(B\), with one end open, has the same frequency as the second harmonic of pipe \(A\). How long are (a) pipe \(A\) and (b) pipe \(B\) ?

Kundt's method for measuring the speed of sound. In Fig. \(17-51\), a rod \(R\) is clamped at its center; a disk \(D\) at its end projects into a glass tube that has cork filings spread over its interior. \(\mathrm{A}\) plunger \(P\) is provided at the other end of the tube, and the tube is filled with a gas. The rod is made to oscillate longitudinally at frequency \(f\) to produce sound waves inside the gas, and the location of the plunger is adjusted until a standing sound wave pattern is set up inside the tube. Once the standing wave is set up, the motion of the gas molecules causes the cork filings to collect in a pattern of ridges at the displacement nodes. If \(f=4.46 \times 10^{3} \mathrm{~Hz}\) and the separation between ridges is \(9.20 \mathrm{~cm}\), what is the speed of sound in the gas?

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