The velocity of sound in air at N.T.P is $ 330{\text{ m }}{{\text{s}}^{ - 1}} $ . What will be its value when temperature is doubled and pressure is halved?
$ {\text{(i) 65 m }}{{\text{s}}^{ - 1}} $
$ {\text{(ii) 330 m }}{{\text{s}}^{ - 1}} $
$ {\text{(iii) 330 }}\sqrt 2 {\text{ m }}{{\text{s}}^{ - 1}} $
$ {\text{(iv) }}\dfrac{{330}}{{\sqrt 2 }}{\text{ m }}{{\text{s}}^{ - 1}} $
Answer
527.4k+ views
Hint: The speed of sound under N.T.P is given as $ 330{\text{ m }}{{\text{s}}^{ - 1}} $ , we will use the Newton’s formula for finding the velocity of sound and then find the dependencies of velocity of sound. Also we will double the temperature and reduce the pressure, thus we will find the ratio of them.
$ v{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $
Where, $ \gamma $ is adiabatic constant, $ R $ is gas constant, $ T $ is the temperature of a medium and $ M $ is the molecular mass of a given gas or medium.
Complete step by step answer:
According to Newton the speed or velocity of sound in any medium can be calculated by using the formula as:
$ v{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $ ____________ $ (1) $
From the above formula we can observe that velocity of sound does not depend on pressure of gas but it depend on temperature of gas as,
$ v{\text{ }} \propto {\text{ }}\sqrt T $
Let $ {v_1} $ be the velocity of sound at N.T.P which is given as $ 330{\text{ m }}{{\text{s}}^{ - 1}} $ . We can write equation $ (1) $ for velocity $ {v_1} $ as:
$ {v_1}{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $ _______________ $ (2) $
Now when temperature gets doubled, equation $ (1) $ can be written as,
$ v{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $
$ v{\text{ = }}\sqrt {\dfrac{{\gamma R{\text{ }} \times {\text{ 2}}T}}{M}} $
$ v{\text{ = }}\sqrt 2 {\text{ }} \times {\text{ }}\sqrt {\dfrac{{\gamma RT}}{M}} $
Now using the value from equation $ (2) $ we can get the speed of sound as,
$ v{\text{ = }}\sqrt 2 {\text{ }} \times {\text{ }}{v_1} $
We know that $ {v_1} $ is the velocity of sound at N.T.P which is given as $ 330{\text{ m }}{{\text{s}}^{ - 1}} $ . Therefore,
$ v{\text{ = }}\left( {\sqrt 2 {\text{ }} \times {\text{ 330}}} \right){\text{ m }}{{\text{s}}^{ - 1}} $
Hence the correct option is $ {\text{(iii) 330 }}\sqrt 2 {\text{ m }}{{\text{s}}^{ - 1}} $ .
Note:
The velocity of sound does depend on pressure of medium or gas. This is because it has no effect of change in pressure on velocity of sound. We can also find the speed of sound by directly using the relation $ v{\text{ }} \propto {\text{ }}\sqrt T $ . The answer would be the same in both situations. There is no need to substitute the value of $ R $ as it would be replaced at the end.
$ v{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $
Where, $ \gamma $ is adiabatic constant, $ R $ is gas constant, $ T $ is the temperature of a medium and $ M $ is the molecular mass of a given gas or medium.
Complete step by step answer:
According to Newton the speed or velocity of sound in any medium can be calculated by using the formula as:
$ v{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $ ____________ $ (1) $
From the above formula we can observe that velocity of sound does not depend on pressure of gas but it depend on temperature of gas as,
$ v{\text{ }} \propto {\text{ }}\sqrt T $
Let $ {v_1} $ be the velocity of sound at N.T.P which is given as $ 330{\text{ m }}{{\text{s}}^{ - 1}} $ . We can write equation $ (1) $ for velocity $ {v_1} $ as:
$ {v_1}{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $ _______________ $ (2) $
Now when temperature gets doubled, equation $ (1) $ can be written as,
$ v{\text{ = }}\sqrt {\dfrac{{\gamma RT}}{M}} $
$ v{\text{ = }}\sqrt {\dfrac{{\gamma R{\text{ }} \times {\text{ 2}}T}}{M}} $
$ v{\text{ = }}\sqrt 2 {\text{ }} \times {\text{ }}\sqrt {\dfrac{{\gamma RT}}{M}} $
Now using the value from equation $ (2) $ we can get the speed of sound as,
$ v{\text{ = }}\sqrt 2 {\text{ }} \times {\text{ }}{v_1} $
We know that $ {v_1} $ is the velocity of sound at N.T.P which is given as $ 330{\text{ m }}{{\text{s}}^{ - 1}} $ . Therefore,
$ v{\text{ = }}\left( {\sqrt 2 {\text{ }} \times {\text{ 330}}} \right){\text{ m }}{{\text{s}}^{ - 1}} $
Hence the correct option is $ {\text{(iii) 330 }}\sqrt 2 {\text{ m }}{{\text{s}}^{ - 1}} $ .
Note:
The velocity of sound does depend on pressure of medium or gas. This is because it has no effect of change in pressure on velocity of sound. We can also find the speed of sound by directly using the relation $ v{\text{ }} \propto {\text{ }}\sqrt T $ . The answer would be the same in both situations. There is no need to substitute the value of $ R $ as it would be replaced at the end.
Recently Updated Pages
Master Class 11 Social Science: Engaging Questions & Answers for Success

Master Class 11 Chemistry: Engaging Questions & Answers for Success

Master Class 9 General Knowledge: Engaging Questions & Answers for Success

Master Class 9 Maths: Engaging Questions & Answers for Success

Master Class 9 Science: Engaging Questions & Answers for Success

Master Class 9 English: Engaging Questions & Answers for Success

Trending doubts
One Metric ton is equal to kg A 10000 B 1000 C 100 class 11 physics CBSE

Difference Between Prokaryotic Cells and Eukaryotic Cells

Two of the body parts which do not appear in MRI are class 11 biology CBSE

1 ton equals to A 100 kg B 1000 kg C 10 kg D 10000 class 11 physics CBSE

Explain zero factorial class 11 maths CBSE

10 examples of friction in our daily life

