Gas Laws, Ideal Gas Equation & Real Gas Deviations
1. The Fundamental Gas Laws
1. Boyle's Law (Isothermal Law)
At constant temperature (T = constant), the pressure P of a given mass of gas is inversely proportional to its volume V:
A plot of P versus V at constant T gives a rectangular hyperbola called an isotherm.
2. Charles's Law (Isobaric Law)
At constant pressure (P = constant), the volume V of a given mass of gas is directly proportional to its absolute temperature T (in Kelvin):
A plot of V versus T at constant P gives a straight line passing through the absolute zero (−273.15 °C), called an isobar.
3. Gay-Lussac's Law (Isochoric Law)
At constant volume (V = constant), the pressure P of a given mass of gas is directly proportional to its absolute temperature T:
A plot of P versus T at constant V gives a straight line called an isochore.
4. Avogadro's Hypothesis
Equal volumes of all gases under identical conditions of temperature and pressure contain an equal number of molecules:
At STP (Standard Temperature 273.15 K and Pressure 1 atm = 1.013 × 105 Pa), 1 mole of any ideal gas occupies 22.4 litres.
2. The Ideal Gas Equation of State
Combining Boyle's, Charles's, and Avogadro's laws yields the universal Ideal Gas Equation:
where:
- μ (or n): Number of moles = Total mass M / Molar mass M0 = Total molecules N / Avogadro's number NA.
- R: Universal Gas Constant = 8.314 J · mol−1 · K−1 ≈ 2.0 cal · mol−1 · K−1 ≈ 0.0821 L · atm · mol−1 · K−1.
- kB: Boltzmann Constant = R / NA = 1.38 × 10−23 J · K−1.
- NA: Avogadro's constant = 6.022 × 1023 molecules · mol−1.
3. Ideal Gas Equation in Terms of Density
Since μ = M / M0 and density ρ = M / V:
At constant temperature, density of a gas is directly proportional to its pressure (ρ ∝ P).
4. Real Gases vs. Ideal Gas: Condition for Ideal Behaviour
Real gases (like H2, He, N2, O2) obey the ideal gas equation only approximately. A real gas behaves closest to an ideal gas under:
• At low pressure, the volume of gas is large, making molecular volume negligible compared to the total container volume.
• At high temperature, high kinetic energy overcomes weak intermolecular attractive forces.
5. Dalton's Law of Partial Pressures
For a mixture of non-reacting ideal gases enclosed in a common volume V at temperature T, the total pressure P exerted is the sum of their individual partial pressures:
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