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Kinetic Molecular Theory Assumptions
Assumes gas molecules:
Have tiny volumes compared with their containerās volume
Move randomly and constantly
Collide elastically with the walls of a container and other gas molecules
Have no intermolecular interactions
Average kinetic energy is proportional to temperature
Kinetic Energy for Gases
At a given temperature, all gases have the same average kinetic energy - but, they donāt have the same speed!
urms trends
urms = ā((3RT)/M)
As temperature increases, the most probable speed (urms) increases and the distribution of speeds gets wider (because T is in the numerator) - as mass increases, urms decreases (because M is in the denominator)
Effusion
Gas escaping from its container through a tiny hole into a region of lower concentration - heavier gases effuse more slowly
Diffusion
Spreading of gas through other gases - heavier gases diffuse more slowly
Grahamās Law
Rate of diffusion and effusion is inversely proportional to density and inversely proportional to āM
(RateA)/(RateB) = ā((MB)/(MA))
Pressure
The amount of force applied to an area - can be measured with a barometer
P = force/area
Parameters Affecting Gases
Pressure (P) in atm, Pa, or mmHg
Volume (V) in L or m3
Temperature (T) in K
# of Moles (n)
Boyleās Law
V goes down as P goes up - decreasing the volume increases the number of collisions per area, so pressure increases - P is proportional to 1/V, so P1V1 = P2V2
Charlesās Law
V decreases as T increases - V is proportional to T, so V1/T1 = V2/T2
Avogadroās Law
V increases as n increases - V is proportional to n, so V1/n1 = V2/n2
Amontonās Law
P increases as T increases - P is proportional to T, so P1/T1 = P2/T2
Ideal Gas Law
PV = nRT
Combines all four laws (Boyle, Charles, Avogadro, Amonton) - āidealā because weāre assuming KMT assumptions are valid
STP
Standard temperature and pressure for gases
Standard temp is 273.15 K
Standard pressure is 1 bar
1 mol of gas at STP = 22.7 L in molar volume
Molar Mass Law
M = m/n (grams/mole), so you combine it with the ideal gas law to make M = (mRT/PV)
Density Equation
d = PM/RT
Density of gases increases when the molar mass of the gas increases
Buoyancy
Depends on differences in gas density which arise from:
Molar Masses (smaller M = lower d)
Temperature (higher T = lower d)
So, hot air balloons can float!
Daltonās Law of Partial Pressures
Total Pressure = the sum of pressures each gas would exert if it were alone in the same volume (āpartialā pressures) - TP depends on the number of moles of gas present, not their identities
Ptotal = (ntotalRT)/V
Mole Fraction
Ratio between moles of one component and the total moles present
X1 = n1/ntotal so⦠P1 = X1Ptotal
Van der Waals Force
Any interaction between neutral atoms/molecules, including hydrogen bonds, dipole-dipole interactions, and london dispersion forces - NOT chemical bonds, just electrostatic interactions
London Dispersion Forces
An intermolecular force between atoms/molecules caused by the presence of temporary dipoles - temporary dipoles are based on the polarizability of the atom/molecule - present between all atoms/molecules
Polarizability
The tendency of an electron cloud to distort - the bigger the atom, the larger the polarizability - larger polarizability = larger london dispersion forces
Dipole-Dipole Interactions
An attraction between regions of polar molecules that have partial charges of opposite sign
Hydrogen Bonds
A strong dipole-dipole interaction which occurs between a hydrogen bonded to an N, O, or F atom and another N, O, or F atom
Ion-Dipole Interactions
An attractive force between an ion and a molecule that has a permanent dipole
Four Types of Intermolecular Forces (weakest ā strongest)
London Dispersion Forces
Dipole-Dipole Interactions
Hydrogen Bonds
Ion-Dipole Interactions
Real Life Gases (violations of ideal gas law)
Particle volume is not negligible at high pressure (violates KMT) - intermolecular attractions are significant at low temperatures (violates KMT) - so, ideal gas behavior must be corrected when at high pressure and/or low temperature (Van der Waals Equation)
Van der Waals Equation
Law for real gases when attractive forces and/or volume of particles are not negligible - a and b are specific to each gas - (n2a)/V2 corrects for attraction forces and (nb) corrects for the volume of particles
(P+(n2a)/V2)(V-nb) = nRT

Boiling Point of Gases
Boiling point increases with polarizability as the number of electrons and the electron-cloud radius increases - more surface area = greater LDFs