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Physics · Ch 9 — Kinetic Theory of Gases

Some Elementary Deductions from Kinetic Theory of Gases

9.2.4

Some Elementary Deductions from Kinetic Theory of Gases

Boyle's law. From equation (9.12), PV=23UPV=\tfrac23 U. The internal energy of an ideal gas also equals NN times the average kinetic energy ϵ\epsilon of a single molecule, U=NϵU=N\epsilon. At a fixed temperature, ϵ\epsilon stays constant (since ϵ=32kT\epsilon=\tfrac32 kT depends only on TT), so

PV=23Nϵ=constant(at fixed T).PV = \frac23 N\epsilon = \text{constant} \quad (\text{at fixed } T).

This is exactly Boyle's law: at constant temperature, the pressure of a fixed amount of gas is inversely proportional to its volume.

Charles' law. From the same relation, PV=23UPV=\tfrac23 U, now hold the pressure fixed instead. Then VV is directly proportional to the internal energy UU (equivalently, to the average kinetic energy of the gas), and since U∝TU\propto T, it follows that

V∝T⇒VT=constant(at fixed P).V \propto T \quad\Rightarrow\quad \frac{V}{T} = \text{constant} \quad (\text{at fixed } P).

This is exactly Charles' law: at constant pressure, the volume of a fixed amount of gas is directly proportional to its absolute temperature.

Avogadro's law. Consider two different gases at the same temperature and pressure, with N1N_1 and N2N_2 molecules respectively (masses m1,m2m_1,m_2, mean square speeds v12‾,v22‾\overline{v_1^2},\overline{v_2^2}). Applying equation (9.6) to each gas separately,

P=13N1Vm1v12‾=13N2Vm2v22‾.(9.15)P = \frac13\frac{N_1}{V}m_1\overline{v_1^2} = \frac13\frac{N_2}{V}m_2\overline{v_2^2}. \qquad (9.15)

Since both gases are at the same temperature, they have the same average kinetic energy per molecule (equation 9.9 does not depend on the type of molecule):

12m1v12‾=12m2v22‾.(9.16)\frac12 m_1\overline{v_1^2} = \frac12 m_2\overline{v_2^2}. \qquad (9.16) …