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Chapter 12 Properties Of Gases
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Pressure Measure of the number of collisions between gas particles and a unit area of the wall of the container Pressure = force / unit area
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Force/area English system: pounds/in2 (psi) Metric system:
Newton/m2 (pascal)
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Torricelli Barometer h = 760 mm Hg 1 atmosphere pressure
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1 atm = 760 torr (mm Hg) = kPa = bar =14.70 psi
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Patm Manometer h Pgas
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Patm Manometer h Pgas
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Volume Total space of a container that gases occupy due to the free random motion of the gas molecules
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Relationship between Volume & Pressure of Gases
P-V
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V P (at constant T)
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Slope = k V 1/P (at constant T)
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In mathematical terms:
y = mx + b Boyle’s Law
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Relationship between Volume & Temperature of Gases
V-T
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In mathematical terms:
y = mx + b V = mT + b Charles’ Law
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Where T must be in Kelvin (K) temperature
K = 0C + 273
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Relationship between Pressure & Temperature of Gases
P-T
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In mathematical terms:
y = mx + b P = mT + b Gay-Lussac’s Law
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Relationship between Volume & Moles
of Gases V-n
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In mathematical terms:
y = mx + b V = mn + b Avogadro’s Law
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Avogadro’s Hypothesis
At constant temperature and pressure, equal volumes of gases contain equal number of particles
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Combined Gas Law
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Ideal & Real Gasses
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Kinetic Molecular Theory
1. Gases consist of small particles that are far apart in comparison to their own size. These particles are considered to be tiny points occupying a negligible volume compared to that of their container.
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Kinetic Molecular Theory
2. Molecules are in rapid and random straight-line motion. This motion can be described by well-defined and established laws of motion.
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Kinetic Molecular Theory
3. The collisions of molecules with the walls of a container or with other molecules are perfectly elastic. That is, no loss of energy occurs.
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Kinetic Molecular Theory
4. There are no attractive forces between molecules or between molecules and the walls with which they collide.
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Kinetic Molecular Theory
5. At any particular instant, the molecules in a given sample of gas do not all possess the same amount of energy.
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Ideal Gas Equation
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Note that is similar to the Combined Gas Law derived earlier.
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Variations on Ideal Gas Equation
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Variations on Ideal Gas Equation
Bromine Variations on Ideal Gas Equation
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Real Gas Behavior
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Ideal Gas Equation P V = n R T
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N2 2.0 CH4 H2 PV nRT 1.0 Ideal gas CO2 P (atm)
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“correct” for volume of molecules
(V - b)
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attractive forces between molecules
also “correct” for attractive forces between molecules
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van der Waals’ Equation
for 1 mole
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van der Waals’ Equation
for n moles
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from CRC Handbook a* b* He Ne *when P(atm) & V(L)
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from CRC Handbook a* b* NH H2O *when P(atm) & V(L)
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from CRC Handbook a* b* CCl C5H *when P(atm) & V(L)
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Cl2 gas has a = 6.49, b = For 8.0 mol Cl2 in a 4.0 L tank at 27oC. P (ideal) = nRT/V = 49.3 atm P (van der Waals) = 29.5 atm
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T & P conditions where a real gas approximates an ideal gas?
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N2 gas PV nRT 203 K 293 K 1.8 1.4 673 K Ideal 1.0 gas 0.6
P (atm)
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T & P conditions where a real gas approximates an ideal gas? high temperature low pressure
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Gaseous Molecular Movement
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pressure exerted by each component in a mixture of gases
Partial Pressure pressure exerted by each component in a mixture of gases
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this assumes that NO interactions occurs between the molecules of gas
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must conclude 1. each gas acts as if it is in container alone
2. each gas collides with the container wall as an “event”
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where n = # components Or Dalton’s Law PT = P1 + P2 + P
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Pi V = ni R T or
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thus:
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or
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therefore: nT = ni and PT sum of mols of gas
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Mole Fraction
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Since: and
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Then
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and Pi = Xi PT
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diffusion is the gradual mixing of molecules of different gases.
effusion is the movement of molecules through a small hole into an empty container.
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rate of average effusion speed
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But ... where
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thus then RMS speed
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substituting:
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simplifying Graham’s Law NH3-HCl
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if “d” is constant
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if “t” is constant
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GAS LAW STOICHIOMETRY
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