the internal energy of an isolated system is constant
experimentally, changes in internal energy or enthalpy may be measured by techniques known collectively as ‘calorimetry’
thermochemistry
the study of heat transactions during chemical reactions
‘adiabatic’ processes occur without transfer of energy as heat
work
the process of achieving motion against an opposing force
energy
capacity to do work
exothermic
a process that releases energy as heat
endothermic
process in which energy is acquired as heat
heat
the process of transferring energy as a result of a temperature difference
work (molecular terms)
transfer of energy that makes use of organized motion of atoms in the surroundings and heat is the transfer of energy that makes use of their disorderly motion
internal energy
total energy of a system; state function
internal energy increases as the temperature is raised
equipartition theorem
used to estimate the contribution to the internal energy of each classically behaving mode of motion
free expansion (expansion against zero pressure) does no work
reversible change
change that can be reversed by an infinitesimal change in a variable
reversible expansion
external pressure is matched at every stage to the pressure of the system
the energy transferred as heat at constant volume is equal to the change in internal energy of the system
calorimetry
measurement of heat transactions
a change in enthalpy is equal to the energy transferred as
heat at constant pressure
heat capacity at constant pressure
equal to the slope of enthalpy with temperature
energy transferred as heatat constant pressure is equal to the change in enthalpy of a system
enthalpy changes can be measured in a constant-pressure calorimeter
thermochemical data
provide a way of assessing heat output of chem rxns, including thos involved with the combustion of fuels and the consumption of food
standard enthalpy of transition
energy transferred as heat at constant pressure in the transition under standard conditions
standard state
pure form of a substance at specified temperature at 1 bar
thermochemical equation
chemical equation and its associated change in enthalpy
hess's law
strandard rxn enthalpy is the sum of values for individual rxns into which overall rxn may be divided
standard enthalpies of formation
defined in terms of reference states of elements
reference state
most stable state at specified temperature and 1 bar
standard rxn enthalpy
difference of the standard enthalpies of formation of products and reactants
kirchhoff''s law
express temperature dependence of a rxn enthalpy
state function
internal energy; enthalpy
dU is an exact differential but dw and dq are not
change in internal energy
expressed in terms of changes in temperature and volume
internal pressure
variation of internal energy with volume at constant temperature
joule's experiment
showed that internal pressure of gas is zero
joule-thomson effect
change in temperature of gas during isenthalpic expansion
CHANGE in internal energy with PRESSURE and TEMPERATURE is expressed in terms of the INTERNAL PRESSURE and the HEAT CAPACITY and leads to a general expression for the relation between heat capacities
adiabatic processes complement isothermal processes, and are used in the discussion of the second law of thermodynamics