19-2 Ideal Gases#

Prompts

  • State the ideal gas law in terms of moles (\(n\)) and in terms of number of molecules (\(N\)). How are \(R\) and \(k\) related?

  • Why is the gas called “ideal”? Under what conditions do real gases approximate ideal behavior?

  • On a \(p\)-\(V\) diagram, what is an isotherm? For an isothermal expansion, is the work \(W\) positive or negative?

  • For an isothermal process, what is \(\Delta E_{\text{int}}\)? How does \(Q\) relate to \(W\)?

  • A gas expands at constant pressure. Write the work done by the gas in terms of \(p\) and \(\Delta V\).

Lecture Notes#

Overview#

  • An ideal gas obeys \(pV = nRT\) (or \(pV = NkT\))—a simple relation between pressure, volume, and temperature.

  • Real gases approximate ideal behavior at low density (molecules far apart, negligible interactions).

  • The ideal gas law links macroscopic quantities (\(p\), \(V\), \(T\)) to the amount of gas (\(n\) or \(N\)).


The ideal gas law#

In terms of moles:

(171)#\[ pV = nRT \]
  • \(p\): absolute pressure; \(V\): volume; \(n\): number of moles; \(T\): temperature (kelvins).

  • \(R = 8.31\) J/(mol·K)—gas constant.

In terms of molecules:

(172)#\[ pV = NkT \]
  • \(N\): number of molecules; \(k = R/N_A = 1.38 \times 10^{-23}\) J/K—Boltzmann constant.

  • Relation: \(nR = Nk\).

Temperature in kelvins

The ideal gas law requires absolute temperature \(T\) in kelvins. Convert from Celsius: \(T = T_C + 273.15\).


Isotherms and work#

An isotherm is a curve of constant \(T\) on a \(p\)\(V\) diagram. For an ideal gas, \(p \propto 1/V\) along an isotherm.

Work done by the gas (general): \(W = \int_{V_i}^{V_f} p\,dV\)—area under the curve.

Process

Work

Isothermal

\(W = nRT\,\ln(V_f/V_i)\)

Constant volume

\(W = 0\)

Constant pressure

\(W = p\,\Delta V\)

Isothermal process: \(\Delta E_{\text{int}} = 0\) (internal energy of ideal gas depends only on \(T\)). By the first law, \(Q = W\).


Example: Highest temperature on a pV diagram#

Summary#

  • \(pV = nRT\) or \(pV = NkT\)—ideal gas law; \(k = R/N_A\).

  • Isotherm: \(p \propto 1/V\) at constant \(T\).

  • Isothermal: \(W = nRT\,\ln(V_f/V_i)\); \(\Delta E_{\text{int}} = 0\), \(Q = W\).

  • Constant pressure: \(W = p\,\Delta V\).