daltons law of partial pressure: total pressure of a mixture of gases is the sum of the partial pressure of each gas
postulate of kinetic molecular theory: volume of individual gas particles are negligible (so small they don't matter)
postulate of kinetic molecular theory: particles of gas are in constant motion so collision of gas particles with walls of container causes pressure
postulate of kinetic molecular theory: particles of gasses don't attract or repel each other
postulate of kinetic molecular theory: average kinetic energy of a gas is directly proportional to the temperature (only in Kelvin)
rootmeansquared velocity is a special average of the velocities of gas; it keeps opposite velocities from canceling out
the M in the root mean squared velocity equation is the mass in kilograms of a mole of the gas (molar mass)
bigger molar mass = slower velocity and smaller molar mass = faster velocity
effusion is the movement of gas molecules from one container to another through a tiny hole
grahams law shows the ratio of the rate of effusion between two gasses of different molar masses
diffusion is the mixing of gases
diffusion is much more theoretically complicated because many gases may be present and collide with the gas that is diffusing
biggest deviations from ideal behavior are low temperature and high pressure
PV/nRT = 1 for ideal gases
the "b" van der waals correction corrects for volume of molecules
the "a" van der waals correction corrects for attraction of molecules (pressure)
larger a & b values = bigger deviations from ideal behavior
a gas with a smaller b value will take up the most volume
SI unit for energy: Joule (J)
Pext = external pressure
when volume expands energy is leaving the system so work is negative
conceptually you can tell P-V work has happened when there's been a change in the amount of gas caused by a chemical reaction
visually you can tell P-V work has happened when the piston moves up in a diagram
change in internal energy of a system (U) is zero for an isolated system
system can exchange internal energy with its surroundings through heat (q) or work (w)
change in internal energy (ΔU) = heat (q) + work (w)
when a system releases heat into its surroundings heat (q) and work (w) are negative
the amount of heat (q) needed to change the temperature of a substance depends on how much temperature changes, quantity of substance, and the nature of the substance
SI unit for heat is Joule (J)
1 calorie (cal) is the quantity needed to change the temperature of 1 gram of water by 1 degrees Celsius
1 calorie = 4.184 J
any property that has unique value for a specific state is a function of state
functions of state do not depend on how that state was established (path independent)
heat and work are functions that depend on the path taken when a system undergoes a change
heat capacity (C) = q/ΔT
molar heat capacity = nCΔT
specific heat capacity = mCΔT (m = mass)
q is positive if heat is gained and negative if heat is lost
heat gained by the system is lost by the surroundings
experimental determination of specific heat: heat transferred from substance 1 to substance 2 will be equal in magnitude and have opposite signs