Characteristics of Sound Waves
PHXI15:WAVES

354665 Among the following velocity of sound depend in a gaseous medium

1 Intensity of sound
2 Amplitude and frequency of sound
3 Density and elasticity of medium
4 Wavelength of sound
PHXI15:WAVES

354666 The speed of sound in a mixture of 1 mole of He and 2 mole of \({O_2}\,{\text{at }}27\,^\circ C.\)

1 \(621\;m{s^{ - 1}}\)
2 \(480\;m{s^{ - 1}}\)
3 \(601\;m{s^{ - 1}}\)
4 \(401\;m{s^{ - 1}}\)
PHXI15:WAVES

354667 Two monoatomic ideal gases 1 and 2 of molecular masses \(m_{1}\) and \(m_{2}\) respectively are enclosed in separate containers kept at the same temperature. The ratio of the speed of sound in gas 1 to that in gas 2 is given by

1 \(\sqrt{\dfrac{m_{1}}{m_{2}}}\)
2 \(\sqrt{\dfrac{m_{2}}{m_{1}}}\)
3 \(\dfrac{m_{2}}{m_{1}}\)
4 \(\dfrac{m_{1}}{m_{2}}\)
PHXI15:WAVES

354668 The speed of sound in an ideal gas at a given temperature \(T\) is \(v\). The rms speed of gas molecules at that temperature is \(v_{r m s}\). The ratio of the velocities \(v\) and \(v_{r m s}\) for helium and oxygen gases are \(X\) and \(X^{\prime}\) respectively. Then \(\dfrac{X}{X^{\prime}}\) is equal to

1 \(\sqrt{\dfrac{5}{21}}\)
2 \(\dfrac{21}{5}\)
3 \(\dfrac{21}{\sqrt{5}}\)
4 \(\dfrac{5}{\sqrt{21}}\)
PHXI15:WAVES

354665 Among the following velocity of sound depend in a gaseous medium

1 Intensity of sound
2 Amplitude and frequency of sound
3 Density and elasticity of medium
4 Wavelength of sound
PHXI15:WAVES

354666 The speed of sound in a mixture of 1 mole of He and 2 mole of \({O_2}\,{\text{at }}27\,^\circ C.\)

1 \(621\;m{s^{ - 1}}\)
2 \(480\;m{s^{ - 1}}\)
3 \(601\;m{s^{ - 1}}\)
4 \(401\;m{s^{ - 1}}\)
PHXI15:WAVES

354667 Two monoatomic ideal gases 1 and 2 of molecular masses \(m_{1}\) and \(m_{2}\) respectively are enclosed in separate containers kept at the same temperature. The ratio of the speed of sound in gas 1 to that in gas 2 is given by

1 \(\sqrt{\dfrac{m_{1}}{m_{2}}}\)
2 \(\sqrt{\dfrac{m_{2}}{m_{1}}}\)
3 \(\dfrac{m_{2}}{m_{1}}\)
4 \(\dfrac{m_{1}}{m_{2}}\)
PHXI15:WAVES

354668 The speed of sound in an ideal gas at a given temperature \(T\) is \(v\). The rms speed of gas molecules at that temperature is \(v_{r m s}\). The ratio of the velocities \(v\) and \(v_{r m s}\) for helium and oxygen gases are \(X\) and \(X^{\prime}\) respectively. Then \(\dfrac{X}{X^{\prime}}\) is equal to

1 \(\sqrt{\dfrac{5}{21}}\)
2 \(\dfrac{21}{5}\)
3 \(\dfrac{21}{\sqrt{5}}\)
4 \(\dfrac{5}{\sqrt{21}}\)
PHXI15:WAVES

354665 Among the following velocity of sound depend in a gaseous medium

1 Intensity of sound
2 Amplitude and frequency of sound
3 Density and elasticity of medium
4 Wavelength of sound
PHXI15:WAVES

354666 The speed of sound in a mixture of 1 mole of He and 2 mole of \({O_2}\,{\text{at }}27\,^\circ C.\)

1 \(621\;m{s^{ - 1}}\)
2 \(480\;m{s^{ - 1}}\)
3 \(601\;m{s^{ - 1}}\)
4 \(401\;m{s^{ - 1}}\)
PHXI15:WAVES

354667 Two monoatomic ideal gases 1 and 2 of molecular masses \(m_{1}\) and \(m_{2}\) respectively are enclosed in separate containers kept at the same temperature. The ratio of the speed of sound in gas 1 to that in gas 2 is given by

1 \(\sqrt{\dfrac{m_{1}}{m_{2}}}\)
2 \(\sqrt{\dfrac{m_{2}}{m_{1}}}\)
3 \(\dfrac{m_{2}}{m_{1}}\)
4 \(\dfrac{m_{1}}{m_{2}}\)
PHXI15:WAVES

354668 The speed of sound in an ideal gas at a given temperature \(T\) is \(v\). The rms speed of gas molecules at that temperature is \(v_{r m s}\). The ratio of the velocities \(v\) and \(v_{r m s}\) for helium and oxygen gases are \(X\) and \(X^{\prime}\) respectively. Then \(\dfrac{X}{X^{\prime}}\) is equal to

1 \(\sqrt{\dfrac{5}{21}}\)
2 \(\dfrac{21}{5}\)
3 \(\dfrac{21}{\sqrt{5}}\)
4 \(\dfrac{5}{\sqrt{21}}\)
PHXI15:WAVES

354665 Among the following velocity of sound depend in a gaseous medium

1 Intensity of sound
2 Amplitude and frequency of sound
3 Density and elasticity of medium
4 Wavelength of sound
PHXI15:WAVES

354666 The speed of sound in a mixture of 1 mole of He and 2 mole of \({O_2}\,{\text{at }}27\,^\circ C.\)

1 \(621\;m{s^{ - 1}}\)
2 \(480\;m{s^{ - 1}}\)
3 \(601\;m{s^{ - 1}}\)
4 \(401\;m{s^{ - 1}}\)
PHXI15:WAVES

354667 Two monoatomic ideal gases 1 and 2 of molecular masses \(m_{1}\) and \(m_{2}\) respectively are enclosed in separate containers kept at the same temperature. The ratio of the speed of sound in gas 1 to that in gas 2 is given by

1 \(\sqrt{\dfrac{m_{1}}{m_{2}}}\)
2 \(\sqrt{\dfrac{m_{2}}{m_{1}}}\)
3 \(\dfrac{m_{2}}{m_{1}}\)
4 \(\dfrac{m_{1}}{m_{2}}\)
PHXI15:WAVES

354668 The speed of sound in an ideal gas at a given temperature \(T\) is \(v\). The rms speed of gas molecules at that temperature is \(v_{r m s}\). The ratio of the velocities \(v\) and \(v_{r m s}\) for helium and oxygen gases are \(X\) and \(X^{\prime}\) respectively. Then \(\dfrac{X}{X^{\prime}}\) is equal to

1 \(\sqrt{\dfrac{5}{21}}\)
2 \(\dfrac{21}{5}\)
3 \(\dfrac{21}{\sqrt{5}}\)
4 \(\dfrac{5}{\sqrt{21}}\)