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What has the greatest effect on the speed of sound in air? a) temperature of the air b) frequency of the sound c) wavelength of the sound d) pressure of the atmosphere

Short Answer

Expert verified
Answer: a) temperature of the air

Step by step solution

01

Consider the properties of sound

A sound wave is a mechanical wave that propagates through a medium, such as air, by compressing and rarefying the molecules of the medium. The speed of sound depends on the properties of the medium it travels through, and in this case, we are focusing on air.
02

Understanding the speed of sound in air

The speed of sound in air can be calculated using the following formula: \(v = \sqrt{\frac{\gamma R T}{M}}\) where \(v\) is the speed of sound, \(\gamma\) is the adiabatic index (ratio of specific heats), \(R\) is the gas constant, \(T\) is the absolute temperature, and \(M\) is the molar mass of the gas. From this formula, we can see that the speed of sound in air depends on the temperature (\(T\)) and the properties of the medium (the constants \(\gamma\), \(R\), and \(M\)).
03

Analyzing the effect of temperature on the speed of sound

As the temperature of the air increases, the speed of sound also increases. This relationship can be understood intuitively as the increased temperature leads to more energy for the air molecules, resulting in faster movement and better transmission of the sound wave.
04

Analyzing the effect of frequency and wavelength on the speed of sound

Frequency and wavelength are related to speed, but they do not directly affect the speed of sound in a medium. The relationship between speed (\(v\)), frequency (\(f\)), and wavelength (\(\lambda\)) can be expressed as: \(v = f \lambda\) While frequency and wavelength do influence the speed of sound, they are more related to the properties of individual sound waves, not the overall speed of sound transmission in a medium.
05

Analyzing the effect of pressure on the speed of sound

In an ideal gas, the speed of sound does not depend on the pressure of the atmosphere. Although air is not an ideal gas, the variation in speed due to pressure changes is minimal compared to the effect of temperature. After analyzing each option, we can conclude that the greatest effect on the speed of sound in air is from: a) temperature of the air

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Most popular questions from this chapter

You are driving along a highway at \(30.0 \mathrm{~m} / \mathrm{s}\) when you hear a siren. You look in the rear-view mirror and see a police car approaching you from behind with a constant speed. The frequency of the siren that you hear is \(1300 \mathrm{~Hz}\). Right after the police car passes you, the frequency of the siren that you hear is \(1280 \mathrm{~Hz}\). a) How fast was the police car moving? b) You are so nervous after the police car passes you that you pull off the road and stop. Then you hear another siren, this time from an ambulance approaching from behind. The frequency of its siren that you hear is \(1400 \mathrm{~Hz}\). Once it passes, the frequency is \(1200 \mathrm{~Hz}\). What is the actual frequency of the ambulance's siren?

Standing on the sidewalk, you listen to the horn of a passing car. As the car passes, the frequency of the sound changes from high to low in a continuous manner; that is, there is no abrupt change in the perceived frequency. This occurs because a) the pitch of the sound of the horn changes continuously. b) the intensity of the observed sound changes continuously. c) you are not standing directly in the path of the moving car. d) of all of the above reasons.

Compare the intensity of sound at the pain level, \(120 \mathrm{~dB}\), with that at the whisper level, \(20 \mathrm{~dB}\).

When two pure tones with similar frequencies combine to produce beats, the result is a train of wave packets. That is, the sinusoidal waves are partially localized into packets. Suppose two sinusoidal waves of equal amplitude A, traveling in the same direction, have wave numbers \(\kappa\) and \(\kappa+\Delta \kappa\) and angular frequencies \(\omega\) and \(\omega+\Delta \omega\), respectively. Let \(\Delta x\) be the length of a wave packet, that is, the distance between two nodes of the envelope of the combined sine functions. What is the value of the product \(\Delta x \Delta \kappa ?\)

Electromagnetic radiation (light) consists of waves. More than a century ago, scientists thought that light, like other waves, required a medium (called the ether) to support its transmission. Glass, having a typical mass density of \(\rho=2500 \mathrm{~kg} / \mathrm{m}^{3},\) also supports the transmission of light. What would the elastic modulus of glass have to be to support the transmission of light waves at a speed of \(v=2.0 \cdot 10^{8} \mathrm{~m} / \mathrm{s} ?\) Compare this to the actual elastic modulus of window glass, which is \(5 \cdot 10^{10} \mathrm{~N} / \mathrm{m}^{2}\).

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