v a v g = 8 k B T π m = 8 R T π M 0 v_{avg} = \sqrt{\frac{8 k_B T}{\pi m}} = \sqrt{\frac{8 R T}{\pi M_0}} v a vg = πm 8 k B T = π M 0 8 RT The mean molecular speed in a Maxwell-Boltzmann distribution.
applies when Maxwellian velocity distribution.
speed average jee-advanced
ν = 1 τ = 2 n π d 2 ⟨ v ⟩ \nu = \frac{1}{\tau} = \sqrt{2} n \pi d^2 \langle v \rangle ν = τ 1 = 2 nπ d 2 ⟨ v ⟩ Rate at which a molecule undergoes collisions.
applies when Assuming Maxwellian speed distribution.
collision frequency kinetics
P 1 V 1 T 1 = P 2 V 2 T 2 \frac{P_1 V_1}{T_1} = \frac{P_2 V_2}{T_2} T 1 P 1 V 1 = T 2 P 2 V 2 Relates states of a fixed amount of gas undergoing a change.
applies when Constant number of moles.
ideal_gas state_change
Dalton's Law of Partial Pressures P t o t a l = P 1 + P 2 + ⋯ = ∑ μ i R T V P_{total} = P_1 + P_2 + \dots = \sum \frac{\mu_i R T}{V} P t o t a l = P 1 + P 2 + ⋯ = ∑ V μ i RT Total pressure of a mixture of non-reacting gases is the sum of their individual partial pressures.
applies when Non-reacting ideal gas mixture.
partial_pressure mixture
E D O F = 1 2 k B T E_{DOF} = \frac{1}{2} k_B T E D OF = 2 1 k B T Average energy associated with each quadratic term (degree of freedom) in thermal equilibrium.
applies when Classical limits, high enough temperature to activate modes.
equipartition degrees_of_freedom
Specific Heat Ratio (Gamma) γ = C p C v = 1 + 2 f \gamma = \frac{C_p}{C_v} = 1 + \frac{2}{f} γ = C v C p = 1 + f 2 Ratio of specific heats related to the degrees of freedom.
applies when Ideal gas with f active degrees of freedom.
specific_heat gamma adiabatic_index
Graham's Law of Diffusion r 1 r 2 = M 2 M 1 \frac{r_1}{r_2} = \sqrt{\frac{M_2}{M_1}} r 2 r 1 = M 1 M 2 Ratio of diffusion or effusion rates for two different gases.
applies when Gases at identical temperatures and pressures.
diffusion effusion graham jee-advanced
Ideal Gas Equation (Molar Form) Standard equation of state for an ideal gas relating pressure, volume, temperature, and moles.
applies when Ideal gas behavior (low pressure, high temperature limit).
ideal_gas thermodynamics state
Ideal Gas Equation (Number Density Form) Ideal gas equation expressed in terms of molecular number density.
applies when Ideal gas.
ideal_gas density boltzmann
Ideal Gas Equation (Mass Density Form) P = ρ R T M 0 P = \frac{\rho R T}{M_0} P = M 0 ρRT Ideal gas equation expressed in terms of mass density.
applies when Ideal gas.
ideal_gas mass_density
Total Internal Energy of Ideal Gas U = f 2 μ R T U = \frac{f}{2} \mu RT U = 2 f μ RT Total internal energy calculated from degrees of freedom.
applies when Ideal gas, f = total active degrees of freedom.
internal_energy degrees_of_freedom
Maxwell-Boltzmann Speed Distribution d N v = 4 π N ( m 2 π k B T ) 3 / 2 v 2 e − m v 2 2 k B T d v dN_v = 4\pi N \left( \frac{m}{2\pi k_B T} \right)^{3/2} v^2 e^{-\frac{mv^2}{2k_B T}} dv d N v = 4 π N ( 2 π k B T m ) 3/2 v 2 e − 2 k B T m v 2 d v Number of molecules with speeds between v and v + dv.
applies when Gas in thermal equilibrium.
distribution maxwell boltzmann jee-advanced
C p − C v = R C_p - C_v = R C p − C v = R Relationship between molar specific heat at constant pressure and constant volume.
applies when Ideal gas.
specific_heat mayer
l = 1 2 π n d 2 l = \frac{1}{\sqrt{2} \pi n d^2} l = 2 πn d 2 1 Average distance a molecule travels between two successive collisions.
applies when Assuming Maxwellian speed distribution.
mean_free_path collisions
Mean Free Path (P, T Dependence) l = k B T 2 π d 2 P l = \frac{k_B T}{\sqrt{2} \pi d^2 P} l = 2 π d 2 P k B T Mean free path expressed in terms of macroscopic pressure and temperature.
applies when Ideal gas.
mean_free_path pressure temperature jee-advanced
Average Translational Kinetic Energy ϵ t ‾ = 1 2 m v 2 ‾ = 3 2 k B T \overline{\epsilon_t} = \frac{1}{2} m \overline{v^2} = \frac{3}{2} k_B T ϵ t = 2 1 m v 2 = 2 3 k B T Average translational kinetic energy per molecule of a gas.
applies when Depends only on absolute temperature.
energy temperature microscopic
Specific Heat (Cv) of Mixture C v , m i x = μ 1 C v 1 + μ 2 C v 2 μ 1 + μ 2 C_{v, mix} = \frac{\mu_1 C_{v1} + \mu_2 C_{v2}}{\mu_1 + \mu_2} C v , mi x = μ 1 + μ 2 μ 1 C v 1 + μ 2 C v 2 Equivalent molar specific heat at constant volume for a gas mixture.
applies when Non-reacting ideal gas mixture.
mixture specific_heat jee-advanced
μ 1 + μ 2 γ m i x − 1 = μ 1 γ 1 − 1 + μ 2 γ 2 − 1 \frac{\mu_1 + \mu_2}{\gamma_{mix} - 1} = \frac{\mu_1}{\gamma_1 - 1} + \frac{\mu_2}{\gamma_2 - 1} γ mi x − 1 μ 1 + μ 2 = γ 1 − 1 μ 1 + γ 2 − 1 μ 2 Equivalent specific heat ratio (gamma) for a gas mixture.
applies when Non-reacting ideal gas mixture.
mixture gamma jee-advanced
Equivalent Molar Mass of Mixture M m i x = μ 1 M 1 + μ 2 M 2 μ 1 + μ 2 M_{mix} = \frac{\mu_1 M_1 + \mu_2 M_2}{\mu_1 + \mu_2} M mi x = μ 1 + μ 2 μ 1 M 1 + μ 2 M 2 Effective molar mass of a non-reacting gas mixture.
applies when Non-reacting gas mixture.
mixture molar_mass jee-advanced
μ = M M 0 = N N A \mu = \frac{M}{M_0} = \frac{N}{N_A} μ = M 0 M = N A N Calculation of moles from total mass or total number of molecules.
moles avogadro mass
Momentum Transfer to Wall Δ p = 2 m v x \Delta p = 2mv_x Δ p = 2 m v x Momentum imparted to a wall during a perfectly elastic molecular collision in 1D.
applies when Perfectly elastic collision with a stationary wall.
momentum collision derivation
Rebound Speed (Moving Wall) v r e b o u n d = u + 2 V v_{rebound} = u + 2V v re b o u n d = u + 2 V Speed of a gas molecule after an elastic collision with a massive wall (like a piston) moving towards it.
applies when Elastic collision; V is wall speed, u is initial molecular speed.
collision piston kinematics
v m p = 2 k B T m = 2 R T M 0 v_{mp} = \sqrt{\frac{2 k_B T}{m}} = \sqrt{\frac{2 R T}{M_0}} v m p = m 2 k B T = M 0 2 RT The speed possessed by the largest fraction of molecules in a gas.
applies when Maxwellian velocity distribution.
speed most_probable jee-advanced
P V = 2 3 E PV = \frac{2}{3} E P V = 3 2 E Relationship between the pressure of an ideal gas and its total translational kinetic energy.
applies when Ideal gas.
pressure energy translational
Kinetic Pressure Equation P = 1 3 n m v 2 ‾ P = \frac{1}{3} n m \overline{v^2} P = 3 1 nm v 2 Macroscopic pressure derived from microscopic kinetic theory.
applies when Isotropic gas in thermal equilibrium.
pressure kinetic_theory microscopic
Root Mean Square (RMS) Speed v r m s = 3 k B T m = 3 R T M 0 v_{rms} = \sqrt{\frac{3 k_B T}{m}} = \sqrt{\frac{3 R T}{M_0}} v r m s = m 3 k B T = M 0 3 RT The square root of the mean squared speed of gas molecules.
applies when Thermal equilibrium.
speed rms temperature
Specific Heat Capacity of Solids Dulong-Petit law prediction for molar specific heat of solids.
applies when High temperatures where quantum effects are negligible.
solid specific_heat dulong_petit
ϵ v = 1 2 m ( d y d t ) 2 + 1 2 k y 2 \epsilon_v = \frac{1}{2} m \left(\frac{dy}{dt}\right)^2 + \frac{1}{2} k y^2 ϵ v = 2 1 m ( d t d y ) 2 + 2 1 k y 2 Energy of a 1D vibrational mode consisting of both kinetic and potential energy components.
applies when High temperatures where vibrational modes are active.
vibration energy diatomic
Molecular Volume Fraction f = N 4 3 π r 3 V t o t a l f = \frac{N \frac{4}{3} \pi r^3}{V_{total}} f = V t o t a l N 3 4 π r 3 Ratio of the actual volume of the molecules to the total volume of the gas.
applies when Hard sphere model approximation.
volume molecules fraction