Gas Law Notes Basic gas law problems First identify the type of problem by asking: is the problem single state or is there a change occurring? o If single state then use PV=nRT o If a change is occurring then derive PV=nRT problems Identify each variable by its units o (P) can be in atm or kPa o (V) must be in L o (n) is in moles o (R) is determined by the pressure in the problem o (T) must be in Kelvin Derived problems Identify the variables that are changing Underline them within PV=nRT Put all variables on the same side Set them equal to one another Additional things to remember o T must be in Kelvin ALWAYS o Units on other variables just need to match Dalton’s Law of Partial Pressures The total pressure in the system is equal to the sum of all partial pressures PTotal = Px + Py + Pz +… Vapor pressure represents the partial pressure of water PVap = PH2O PV = nRT This will allow you to convert between the pressure and moles of different things: P and n for the entire gas P and n for any one of the gasses in the mixture Setup for Partial Pressures (layout your variables like this) PT = Px = PY = nT = nX = nY = T V Work down pressure or mole columns using PT = Px + Py … and nT = nx + ny … If you have temp or volume use PV=nRT to to work across the row o Plugging in PT with V or T will give you nT or vice versa Same for any PP and individual gas o If you’re looking for T or V, make sure you use the same P and n Ex: Px and nx or PT and nT Do not mix: PT and nX is not allowed Kinetic molecular theory (The logic behind gas laws) There are two approaches to solving these problems: 1. Picture it: a. Think of a container of gas as you within a phone booth filled with bouncy balls b. The impact of the bouncy balls on you is what causes pressure c. Consider the changes being made to the container or the bouncy balls and the effect they will have d. Remember that heating up the gas increases the speed of the bouncy balls 2. The algebraic approach using PV=nRT: a. Variables on the same side of the equation, such as P and V, are inversely proportional i. If P increases then V must decrease by the same magnitude for that side to remain equal to the constant nRT on the other b. Variables on opposite sides, such as P and T are directly proportional i. If T doubles then P must as well in order to keep both sides equal