Question:

The speed of sound through oxygen gas at $T \, K$ is $v \,m \,s^{-1}$. If the temperature becomes $2T$ and oxygen gas dissociated into atomic oxygen, the speed of sound

Updated On: Mar 19, 2024
  • remains the same
  • becomes $2v$
  • becomes $\sqrt{2} v$
  • none of these
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The Correct Option is D

Solution and Explanation

The speed of sound in a gas at $T\, K$ is given by $\upsilon = \sqrt{\frac{\gamma RT}{M}}$ where $\gamma$ is the ratio of specific heat, $R$ is the universal gas constant and $M$ is the molecular mass of a gas. For oxygen gas $\upsilon = \sqrt{\frac{\frac{7}{5}RT}{M_{O_2}}}$ Since $O_2$ is a diatomic gas, so For diatomic gas $\gamma = \frac{7}{5}$ [For no vibrational mode] For atomic oxygen $\upsilon' = \sqrt{\frac{\frac{5}{3}R\left(2T\right)}{M_{O}}} $ $ \therefore \:\:\: \frac{\upsilon'}{\upsilon} = \sqrt{\frac{5}{3} \frac{\left(2RT\right)}{M_{O}}} \times \sqrt{\frac{5M_{O_2}}{7RT}}\qquad$ $ \frac{\upsilon'}{\upsilon} = \sqrt{\frac{50}{21} \frac{M_{O_2}}{M_{O}}}$ $= \sqrt{\frac{50(2)}{21}} \left[ \because \:\:M_O = \frac{M_{O_2}}{2} \therefore \frac{M_{O_2}}{M_O} = 2 \right]$ $ \sqrt{\frac{100}{21}}$ $ \upsilon' = \frac{10}{\sqrt{21}} \upsilon$
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Concepts Used:

Sound

Sound is a vibration that propagates the mechanical wave of displacement and pressure, through a medium can be of any matter. In other words, the sound is the thin line between Music sound and Noise.

Types of Sounds:

Sound can be divided into two types depending on its frequency. The following are:-

Infrasonic Waves:

  • Infrasonic waves have a frequency lower than 20 Hz. Since it is below the human hearing range, it is inaudible to humans.
  • However, several other living organisms use these waves to communicate, whales, sharks, elephants, hippopotamus, etc. these waves are also used in the scientific field, it is used to study upcoming earthquakes, volcanic eruptions, human heart rates, rock formation stages, etc.

Ultrasonic waves:

  • Ultrasonic waves have a frequency higher than 20 kHz. Since it is above the human hearing range, it is inaudible to humans.
  • These waves are used in the scientific field, it is used to study human heart rates, to take sonograms, navigation of directions, imaging things, uniform sample mixing, communication, testing of samples, etc.