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⚡️College Physics III – Thermodynamics, Electricity, and Magnetism Unit 2 Review

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2.4 Distribution of Molecular Speeds

2.4 Distribution of Molecular Speeds

Written by the Fiveable Content Team • Last updated August 2025
Written by the Fiveable Content Team • Last updated August 2025
⚡️College Physics III – Thermodynamics, Electricity, and Magnetism
Unit & Topic Study Guides

Gases are made up of tiny particles zipping around at different speeds. The Maxwell-Boltzmann distribution describes how fast these particles move in an ideal gas. It's a key concept in understanding gas behavior at the molecular level.

This distribution helps us calculate important speeds like the most probable, average, and root-mean-square speed of gas molecules. Temperature plays a big role, affecting how fast the particles move and how their speeds are spread out.

Distribution of Molecular Speeds in Ideal Gases

Maxwell-Boltzmann distribution of speeds

  • Probability distribution of molecular speeds in an ideal gas at thermal equilibrium assumes no intermolecular interactions and elastic collisions between molecules (billiard balls)
  • Probability density function f(v)f(v) gives the probability of finding a molecule with a specific speed vv
    • f(v)=4π(m2πkBT)3/2v2emv22kBTf(v) = 4\pi \left(\frac{m}{2\pi k_B T}\right)^{3/2} v^2 e^{-\frac{mv^2}{2k_B T}}, where mm is molecular mass, kBk_B is Boltzmann constant, and TT is absolute temperature (Kelvin)
  • Distribution is asymmetric and positively skewed with a long tail at high speeds (right-skewed)
    • Most molecules have speeds close to the most probable speed with fewer molecules at very low or very high speeds (bell curve)

Calculation of molecular speeds

  • Most probable speed vmpv_{mp} is the speed at which Maxwell-Boltzmann distribution reaches its maximum value
    • vmp=2kBTmv_{mp} = \sqrt{\frac{2k_B T}{m}}
  • Average speed vˉ\bar{v} is the mean speed of all molecules in the gas
    • vˉ=8kBTπm\bar{v} = \sqrt{\frac{8k_B T}{\pi m}}
  • Root-mean-square (rms) speed vrmsv_{rms} is the square root of the average of the squares of molecular speeds
    • vrms=3kBTmv_{rms} = \sqrt{\frac{3k_B T}{m}}
  • Relationship between these speeds: vmp<vˉ<vrmsv_{mp} < \bar{v} < v_{rms}
    • Most probable speed is lower than average speed which is lower than rms speed
  • These speeds are inversely proportional to the square root of molecular mass, affecting the distribution of speeds for different gases
Maxwell-Boltzmann distribution of speeds, Maxwell–Boltzmann distribution - Wikipedia

Temperature effects on speed distribution

  • As temperature increases, Maxwell-Boltzmann distribution shifts to the right and becomes broader (higher speeds)
    • Peak of distribution (most probable speed) moves to higher speeds
    • Proportion of molecules with higher speeds increases (more high-speed molecules)
  • Average, most probable, and rms speeds all increase with square root of absolute temperature
    • Doubling absolute temperature increases these speeds by factor of 2\sqrt{2} (41% increase)
  • At higher temperatures, distribution of molecular speeds becomes more spread out with larger standard deviation (wider distribution)
  • Changes in temperature do not affect shape of distribution, only its position and width (still bell-shaped)

Kinetic Theory of Gases and Thermal Equilibrium

  • Kinetic theory of gases explains macroscopic properties of gases using the motion of their constituent particles
  • Thermal equilibrium is achieved when a system's temperature is uniform and not changing with time
  • Mean free path is the average distance a molecule travels between collisions, affecting the rate of energy transfer in the gas
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