How does the speed of sound in a gas change when you raise the temperature from0°CTO20°C ? Explain briefly.

Short Answer

Expert verified

The speed of sound increases as the temperature of the gas increases and vice-versa is also true.

Step by step solution

01

Understanding the sound speed

In this problem, the concept of sound speed will be used to determine the dependency of sound speed on a variable like a temperature, etc. For the movement of a sound wave, the requirement of a specific medium is compulsory.

02

Evaluating how the speed of sound in a gas changes when you raise temperature from 0°C to 20°C.

The speed of sound is the distance travelled per unit of time by a sound wave as

it propagates through an elastic medium.

The speed of sound in an ideal gas depends only on its temperature and composition. The speed has a weak dependence on the frequency and pressure in ordinary air, deviating slightly from ideal behaviour.

The mathematical expression to evaluate the sound speed at different temperature is expressed as follows:

v=γRT

Here, V represents the speed of sound, γ represents the ratio of specific heats of medium (ideal gas), R represents the gas constant and T represents the absolute temperature of medium (ideal gas).

Thus, it is reasonable that the speed of sound in a gas depend on the square root of temperature. For air, atrole="math" localid="1655487640043" 0°C the speed of sound is 331 m/s, whereas at 20°Cit is 343 m/s, less than an increment of 4%.

Thus, the speed of sound varies in a direct proportion of the square root of absolute temperature of the gas.

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Most popular questions from this chapter

A block of copper (one mole has a mass of 63.5 g ) at a temperature of 35°is put in contact with a 100 gblock of aluminum (molar mass 27 g) at a temperature of20°C. The blocks are inside an insulated enclosure, with little contact with the walls. At these temperatures, the high-temperature limit is valid for the specific heat. Calculate the final temperature of the two blocks. Do NOT look up the specific heats of aluminum and copper; you should be able to figure them out on your own.

Verify that this equation gives the correct number of ways to arrange 0, 1, 2, 3, or 4 quanta among 3 one-dimensional oscillators, given in earlier tables (1, 3, 6, 10, 15).






Q1

Q2

#ways1

#ways2

#ways1

#ways2

0

4

1

15

15

1

3

3

10

30

2

2

6

6

36

3

1

10

3

30

4

0

15

1

15






Calculate vmsfor a helium atom and for a nitrogen molecule ( N2; molecular mass 28g/mol) in the room you’re in (whose temperature is probably about 293K).

The entropy S of a certain object (not an Einstein solid) is the following function of the internal energy E:S=bE1/2, where b is a constant. (a) Determine the internal energy of this object as a function of the temperature.

(b) What is the specific heat of this object as a function of the temperature?

The reasoning developed for counting microstates applies to many other situations involving probability. For example, if you flip a coin 5 times, how many different sequences of 3 heads and 2 tails are possible? Answer: 10 different sequences, such as HTHHT or TTHHH. In contrast, how many different sequences of 5 heads and 0 tails are possible? Obviously only one, HHHHH, and our equation gives , using the standard definition thatis defined to equal 1.

If the coin is equally likely on a single throw to come up heads or tails, any specific sequence like HTHHT or HHHHH is equally likely. However, there is only one way to get HHHHH, while there are 10 ways to get 3 heads and 2 tails, so this is 10 times more probable than getting all heads.

Use the expression to calculate the number of ways to get 0 heads, 1 head, 2 heads, 3 heads, 4 heads, or 5 heads in a sequence of 5 coin tosses. Make a graph of the number of ways vs. the number of heads.

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