Question:

The rms speed of a gas having diatomic molecules at temperature T (in Kelvin) is 200 m/s. If the temperature is increased to 4T and the molecules dissociate into monoatomic atoms,the rms speed will become:

Updated On: Apr 7, 2025
  •  400 m/s

  •  200 m/s

  •  800 m/s

  •  200\(\sqrt{2}\) m/s

  •  400\(\sqrt{2}\) m/s

Hide Solution
collegedunia
Verified By Collegedunia

The Correct Option is

Approach Solution - 1

Initial conditions: \[ v_{rms} = 200\,\text{m/s at temperature } T \text{ for diatomic gas} \]

RMS speed formula: \[ v_{rms} = \sqrt{\frac{3RT}{M}} \]

After changes:

  • Temperature becomes 4T
  • Molecules dissociate into monoatomic atoms (mass becomes M/2)

 

New rms speed calculation: \[ v'_{rms} = \sqrt{\frac{3R(4T)}{M/2}} = \sqrt{8 \times \frac{3RT}{M}} \] \[ v'_{rms} = \sqrt{8} \times v_{rms} = 2\sqrt{2} \times 200 \] \[ v'_{rms} = 400\sqrt{2}\,\text{m/s} \]

Thus, the correct option (E) \(400\sqrt{2}\,\text{m/s}\).

Was this answer helpful?
1
4
Hide Solution
collegedunia
Verified By Collegedunia

Approach Solution -2

1. Recall the formula for rms speed:

The root-mean-square (rms) speed (vrms) of gas molecules is given by:

\[v_{rms} = \sqrt{\frac{3kT}{m}} = \sqrt{\frac{3RT}{M}}\]

where:

  • k is the Boltzmann constant
  • R is the universal gas constant
  • T is the temperature in Kelvin
  • m is the mass of one molecule
  • M is the molar mass

2. Set up the initial and final conditions:

Initial conditions (diatomic, temperature T):

\[v_{rms1} = \sqrt{\frac{3kT}{m_1}} = 200 \, m/s\]

Final conditions (monoatomic, temperature 4T, mass is halved since molecules dissociate):

\[v_{rms2} = \sqrt{\frac{3k(4T)}{m_2}}\] Since the diatomic molecules dissociate into monoatomic atoms, the mass of each atom is half the mass of the diatomic molecule: \(m_2 = \frac{m_1}{2}\). \[v_{rms2} = \sqrt{\frac{3k(4T)}{m_1/2}} = \sqrt{8 \frac{3kT}{m_1}} \]

3. Relate the final rms speed to the initial rms speed:

\[v_{rms2} = \sqrt{8} \sqrt{\frac{3kT}{m_1}} = 2\sqrt{2} v_{rms1} \]

Since \(v_{rms1} = 200 \, m/s\):

\[v_{rms2} = 2\sqrt{2}(200 \, m/s) = 400\sqrt{2} \, m/s\]

Final Answer: The final answer is \(\boxed{E}\)

Was this answer helpful?
0
0

Top Questions on kinetic theory

View More Questions

Concepts Used:

Behaviour of Real Gases

Real gases are gases that do not follow the ideal gas law, which assumes that gas particles have negligible volume and no intermolecular forces. In reality, gas particles do have volume and interact with each other, leading to deviations from ideal gas behavior.

The behavior of real gases can be described using various gas laws, such as the van der Waals equation and the virial equation. These equations take into account the effects of gas particle size and intermolecular forces on gas behavior.

One important property of real gases is compressibility. Real gases are more compressible than ideal gases, meaning that they can be compressed to a smaller volume at the same pressure. This is due to the fact that gas particles occupy a finite amount of space and are subject to intermolecular forces that can cause them to come closer together.

Also Read: Derivation from Ideal Gas Behavior

Another property of real gases is that their behavior is strongly affected by temperature and pressure. At high pressures and low temperatures, real gases tend to deviate more from ideal gas behavior. This is because the intermolecular forces become stronger and the gas particles are closer together.

Real gases also exhibit a phenomenon called condensation, where gas particles condense into a liquid or solid state when cooled or compressed sufficiently. This is due to the fact that the intermolecular forces become strong enough to overcome the kinetic energy of the gas particles, causing them to condense into a denser state.

Overall, the behavior of real gases is complex and influenced by various factors such as temperature, pressure, and intermolecular forces. Understanding the behavior of real gases is important in many scientific and industrial applications, such as in chemical reactions, power generation, and refrigeration.