Gases
Properties of Gases
- Gases assume the shape and volume of their container.
- Gases are compressible.
- Gases have variable densities much smaller than liquids and solids.
- Gases form homogeneous mixtures in any proportion.
- Pressure is force per unit area: pressure=areaforce
- SI unit of force is the newton (N): 1 N=1 kg⋅s2m
- SI unit of pressure is the pascal (Pa): 1 Pa=1m2N
Units of Pressure
- Standard Atmosphere (atm): 1 atm=101,325 Pa
- mmHg: 1 mmHg=133.322 Pa
- torr: 1 torr=133.322 Pa
- bar: 1 bar=1×105 Pa
- 1 atm=101,325 Pa=760 mm Hg=760 torr=1.01325 bar=14.7 psi
Gas Laws
- Gay-Lussac's Law: T</em>1P<em>1=T</em>2P<em>2 (constant volume)
- Boyle's Law: P<em>1V</em>1=P<em>2V</em>2 (constant temperature)
- Charles's Law: T</em>1V<em>1=T</em>2V<em>2 (constant pressure)
- Avogadro's Law: n</em>1V<em>1=n</em>2V<em>2 (constant temperature and pressure)
- Combined Gas Law: n<em>1T</em>1P<em>1V</em>1=n<em>2T</em>2P<em>2V</em>2
Ideal Gas Equation
- PV=nRT
- R (gas constant) values: 0.08206 L⋅atm/mol⋅K, 8.314 J/mol⋅K, 0.08314 L⋅bar/mol⋅K, 1.987 cal/mol⋅K
- STP Conditions: 1 atm and 0 °C (273.15 K)
Applications of Ideal Gas Equation
- Density: d=R⋅TP⋅MM
Gas Mixtures: Dalton’s Law of Partial Pressures
- P<em>total=ΣP</em>i
Mole Fractions
- χ<em>i=n<em>totaln</em>i and χ</em>i=P</em>totalP<em>i
Reactions with Gaseous Reactants and Products
- Use stoichiometry and the ideal gas equation to find required volumes.
Collecting Gas Over Water
- P<em>total=P</em>collected gas+P<em>H</em>2O
Kinetic Molecular Theory
- Gas particles are separated by large distances and have negligible volume.
- Gas molecules are in constant, random motion with elastic collisions.
- Gas molecules do not exert attractive or repulsive forces on each other.
- Average kinetic energy is proportional to absolute temperature: Ek∝T
Molecular Speed
- Root-mean-square speed: urms=M3RT
Diffusion and Effusion
- Graham's Law: Rate∝M1
Real Gases: Deviations from Ideal Behavior
- High pressure and low temperatures cause deviations.
- Van der Waals Equation: (P+V2an2)(V−nb)=nRT