Kinetic Theory of Gases - Summary

Kinetic Theory of Gases

Molecular Speeds and Ideal Gas Law

  • Ideal gas law: PV=nRTPV = nRT
  • PP: Force exerted by molecules on the wall during collisions.
  • VV: Available volume for molecules.
  • TT: Indicates the speed of molecules.
  • Gas molecules are in random and continuous motion.
  • Collisions redistribute speed among molecules.

Molecular Momentum and Force

  • Change in momentum for one molecule: Δ(mv<em>x)=2mv</em>xΔ(mv<em>x) = 2mv</em>x
  • Time between collisions: Δt=2lvxΔt = \frac{2l}{v_x}
  • Force due to a single molecule: F=mvx2lF = \frac{mv_x^2}{l}
  • Average force due to all molecules in x-direction: F<em>x=mlNv</em>x2F<em>x = \frac{m}{l}N \overline{v</em>x^2}
  • Mean-square of v<em>xv<em>x: v</em>x2=(v<em>x12+v</em>x22+v<em>x32++v</em>xN2)N\overline{v</em>x^2} = \frac{(v<em>{x1}^2 + v</em>{x2}^2 + v<em>{x3}^2 + … + v</em>{xN}^2)}{N}

Pressure and Mean Squared Speed

  • v2=v<em>x2+v</em>y2+v<em>z2=3v</em>x2\overline{v^2} = \overline{v<em>x^2} + \overline{v</em>y^2} + \overline{v<em>z^2} = 3\overline{v</em>x^2}
  • Pressure: P=FxA=13Nmv2VP = \frac{F_x}{A} = \frac{1}{3} \frac{Nm\overline{v^2}}{V}

Mean Translation Energy

  • PV=13Nmv2=23N(12mv2)PV = \frac{1}{3}Nm\overline{v^2} = \frac{2}{3}N(\frac{1}{2}m\overline{v^2})
  • Nm=nMNm = nM (N = number of molecules, m = mass of each molecule, n = number of moles, M = molar mass)
  • Mean translation energy: E<em>trans=32kTE<em>{trans} = \frac{3}{2}kT (per molecule), E</em>trans=32RTE</em>{trans} = \frac{3}{2}RT (per mole)

Root-Mean-Square (rms) Speed

  • vrms=3kTm=3RTMv_{rms} = \sqrt{\frac{3kT}{m}} = \sqrt{\frac{3RT}{M}}
  • Lighter molecules move at higher rms speed.
  • Different gases have different rms speeds at a given temperature.

Equipartition of Energy

  • Etrans=32kT=12kT+12kT+12kTE_{trans} = \frac{3}{2}kT = \frac{1}{2}kT + \frac{1}{2}kT + \frac{1}{2}kT (x, y, z directions)
  • Each degree of freedom contributes 12kT\frac{1}{2}kT to the energy.
  • Degrees of freedom: Translation, Vibration, Rotation.

Degrees of Freedom

  • Atom: 3 (translation)
  • Molecule (non-linear): 3 (translation), 3 (rotation), 3N-6 (vibration)
  • Molecule (linear): 3 (translation), 2 (rotation), 3N-5 (vibration)

Maxwell Speed Distribution

  • Molecular collisions redistribute speeds.
  • Maxwell distribution describes speeds in x, y, and z directions.

Boltzmann Distribution Law

  • P(h)=P0exp(mghkT)P(h) = P_0 \exp(-\frac{mgh}{kT}) relates air pressure with altitude.
  • Boltzmann factor: exp(EkT)\exp(-\frac{E}{kT}) relates the number of molecules in a given state with the energy of that state.
  • N<em>iN</em>j=exp(E<em>iE</em>jkT)\frac{N<em>i}{N</em>j} = \exp(-\frac{E<em>i - E</em>j}{kT})
  • Fraction of particles in the ith level: p(i)=N<em>iNexp(E</em>ikT)p(i) = \frac{N<em>i}{N} \propto \exp(-\frac{E</em>i}{kT})

Maxwell Speed Distribution (1D and 3D)

  • p(v<em>x)=Kexp(mv</em>x22kT)p(v<em>x) = K \exp(-\frac{m v</em>x^2}{2kT})
  • p(v<em>x,v</em>y,v<em>z)=(m2πkT)3/2exp(m(v</em>x2+v<em>y2+v</em>z2)2kT)p(v<em>x, v</em>y, v<em>z) = (\frac{m}{2\pi kT})^{3/2} \exp(-\frac{m(v</em>x^2 + v<em>y^2 + v</em>z^2)}{2kT})
  • p(v)dv=4π(m2πkT)3/2exp(mv22kT)v2dvp(v)dv = 4\pi (\frac{m}{2\pi kT})^{3/2} \exp(-\frac{m v^2}{2kT}) v^2 dv

Average Values

  • g(x)=p(x<em>j)g(x</em>j)g(x) = \sum p(x<em>j)g(x</em>j)
  • Most probable speed: vmp=2RTM=2kTmv_{mp} = \sqrt{\frac{2RT}{M}} = \sqrt{\frac{2kT}{m}}
  • Average speed: v=8kTmπ=8RTπM\overline{v} = \sqrt{\frac{8kT}{m\pi}} = \sqrt{\frac{8RT}{\pi M}}
  • Root-mean-square speed: vrms=3kTm=3RTMv_{rms} = \sqrt{\frac{3kT}{m}} = \sqrt{\frac{3RT}{M}}
  • v{rms} > v{ave} > v_{mp}

Molecular Collisions

  • Collision cross-section area: σ<em>AB=πd</em>AB2\sigma<em>{AB} = \pi d</em>{AB}^2
  • Single-particle collision frequency: z<em>AB=η</em>Bσ<em>ABv</em>relz<em>{AB} = \eta</em>B \sigma<em>{AB} v</em>{rel}
  • Total collision frequency: Z<em>AB=η</em>Az<em>AB=η</em>Aη<em>Bσ</em>ABvrelZ<em>{AB} = \eta</em>A z<em>{AB} = \eta</em>A \eta<em>B \sigma</em>{AB} v_{rel}

Collision Frequency

  • v<em>rel=(v</em>A,ave)2+(vB,ave)2v<em>{rel} = \sqrt{(v</em>{A,ave})^2 + (v_{B,ave})^2}
  • If A = B: z<em>AA=2η</em>Aσ<em>AAv</em>A,avez<em>{AA} = \sqrt{2} \eta</em>A \sigma<em>{AA} v</em>{A,ave}; Z<em>AA=122η</em>A2σ<em>AAv</em>A,aveZ<em>{AA} = \frac{1}{2} \sqrt{2} \eta</em>A^2 \sigma<em>{AA} v</em>{A,ave}

Mean Free Path

  • λ=vavez=12ησ\lambda = \frac{v_{ave}}{z} = \frac{1}{\sqrt{2} \eta \sigma}

Molecular Diffusion/Effusion

  • Diffusion: Molecules move from high to low concentration.
  • Effusion: Escape of molecules through a tiny hole.

Graham's Law

  • \frac{r1}{r2} = \sqrt{\frac{M2}{M1}}