The “state” of a system is characterised by a set of variables such as P, V, T, n, etc., which are state variables (or state functions) and can be classified as either intensive or extensive.
If temperatures are different, energy (heat) flows from high temperature to low temperature.
All chemical reactions are accompanied by an energy change.
The law of conservation of energy is often represented as ∆ U = q + w, where ∆ U is the change in internal energy, q is system heat, w is work, and U is internal energy.
Temperature is a measure of a particle’s average kinetic energy, an indication of heat content, and objects at the same temperature do not exchange heat energy.
The difference between the change in internal energy and the enthalpy is the amount of work that needs to be done to make room for the products of the reaction.
Hess' Law states that ∆ H ° for an overall process is the sum of the ∆ H ° 's for the individual steps of the process.
Bond Dissociation Enthalpy values are for GASES ONLY and all reactants & products must be in the gaseous state to use BDE values alone.
Ionic bonds result from a complete transfer of an electron.
Expansion work is negative since energy leaves the system as the system does work on the surroundings.
Compression: work is done on the system by the surroundings.
Pressure-Volume (or P-V) work is the most common type of work encountered in chemical systems.
Work is the energy exchange that results when a force moves an object through a distance.
Molar Heat Capacity (C m or C) is the amount of heat needed to raise 1 mole through 1C ° or 1 K unit, or the heat capacity per mole, units: J∙K –1.
Specific Heat (C S or c) is the amount of energy to raise 1 gram through 1C ° or 1 K unit, or the heat capacity per gram of substance, units: J∙g –1.
If heat is given off, the rxn is Exothermic (∆ H is negative).
If heat is absorbed, the rxn is Endothermic (∆ H is positive).
Hess's Law states that thermochemical equations can be added (or subtracted) to yield other thermochemical equations.
The name for the reverse process of Enthalpy of Vaporization is Deposition.
Lattice enthalpies are larger for short ion separations and/or larger ionic charges.
The lattice energy of ionic compounds is determined by the electrostatic interactions between ions.
Reactions at Constant Pressure, i.e., open to the atmosphere, allow the volume to change, hence, ∆ V can be ≠ 0.
A state function for a system is independent of how that value was achieved and only depends on the difference between the final and initial state, not on the path it takes to get there.
Reactions at Constant Volume, i.e., a sealed container, result in zero work and zero change in internal energy, hence, ∆ U = 0.
When an ideal gas expands at constant temperature, ∆ U is zero.
Both enthalpy (H) and internal energy (U) are state functions.
If work done, such as pushing back the atmosphere, is considered, ∆ U = -P ext ∆ V.
Entropy is a thermodynamic function that indicates whether or not a reaction will occur spontaneously.
Spontaneous reactions always proceed so as to move towards a state of equilibrium, i.e., Q → K.
The direction of spontaneity is determined by the sign of ∆G.
Positional distribution of species in space is referred to as mixing of two gases or the expansion of a gas into a vacuum.
For any substance, entropy rises with temperature due to more atomic/molecular motions and therefore more ways the system can contain energy.
Thermal distribution of energy among species, or distribution of species over energy levels, is referred to as heat flow from hot to cold objects.
A spontaneous process is one that occurs without any external influence.
An instantaneous process is one that occurs almost instantly, that is very rapid.
A spontaneous process may be fast or slow, so it is not generally true that a spontaneous process is also instantaneous.
Expansion of a gas into a vacuum is not only spontaneous but also instantaneous.
The entropies of the four gases are likely to be different because their molecular structures are different.
If the reaction is spontaneous, ∆ G is negative.
The number of moles of gases is the same on both sides of the equation, however, so the entropy change is likely to be small if the temperature is constant.