Part of THERM-01 — Thermodynamics & Kinetic Theory of Gases

Formula Reference: All Thermodynamics and Kinetic Theory Equations

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First Law and Processes

Q=ΔU+WIsothermal: W=nRTln(V2/V1),ΔU=0Q = \Delta U + W \qquad \text{Isothermal: } W = nRT\ln(V_2/V_1), \quad \Delta U = 0

Adiabatic: Q=0,  PVγ=const,  W=P1V1P2V2γ1\text{Adiabatic: } Q=0,\; PV^\gamma=\text{const},\; W = \frac{P_1V_1 - P_2V_2}{\gamma-1}

Isochoric: W=0,  Q=ΔU=nCvΔT\text{Isochoric: } W=0,\; Q=\Delta U = nC_v\Delta T

Isobaric: W=PΔV=nRΔT,  Q=nCpΔT\text{Isobaric: } W = P\Delta V = nR\Delta T,\; Q = nC_p\Delta T

Specific Heats and γ

CpCv=R[ML2T2K1mol1]C_p - C_v = R \quad [ML^2T^{-2}K^{-1}mol^{-1}]

Cv=f2R,Cp=f+22R,γ=f+2fC_v = \frac{f}{2}R,\quad C_p = \frac{f+2}{2}R,\quad \gamma = \frac{f+2}{f}

Carnot and COP

η=1T2T1=WQ1[dimensionless, T in K]\eta = 1 - \frac{T_2}{T_1} = \frac{W}{Q_1} \quad [\text{dimensionless, T in K}]

COPref=Q2W=T2T1T2\text{COP}_{ref} = \frac{Q_2}{W} = \frac{T_2}{T_1 - T_2}

Kinetic Theory

P=13ρvrms2[ML1T2]P = \frac{1}{3}\rho v_{rms}^2 \quad [ML^{-1}T^{-2}]

vrms=3RTM,vavg=8RTπM,vmp=2RTM[LT1]v_{rms} = \sqrt{\frac{3RT}{M}},\quad v_{avg} = \sqrt{\frac{8RT}{\pi M}},\quad v_{mp} = \sqrt{\frac{2RT}{M}} \quad [LT^{-1}]

Internal Energy and KE

U=f2nRT[ML2T2]U = \frac{f}{2}nRT \quad [ML^2T^{-2}]

KEtrans/molecule=32kBT,kB=1.38×1023 J/KKE_{trans/molecule} = \frac{3}{2}k_BT,\quad k_B = 1.38\times10^{-23}\ \text{J/K}

Ideal Gas

PV=nRT=NkBT,R=8.314 J mol1K1PV = nRT = Nk_BT,\quad R = 8.314\ \text{J mol}^{-1}\text{K}^{-1}

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