Thermodynamics Flashcards
Heat
(q) amount of thermal energy in transit between a system and its surroundings due to a temperature difference
Thermal energy
energy that arises from kinetic energy of particles
Second Law of Thermodynamics
energy and matter naturally tend to disperse uniformly
Clausius Theorem
heat does not spontaneously pass from a colder object to a hotter body
thermal equilibrium
energy and temperature of both objects are equal and temperature change of both objects is 0 so no net flow of thermal energy
endothermic
system experiences an increase in thermal energy
exothermic
system experiences a decrease in thermal energy
Entropy
(S: J/K) amount of energy in a system that is unavailable to do work. Also a measure of the number of ways a system can be arranged under constraints such as temperature and pressure. extensive property
S_universe =
S_surroundings + S_system
Change in Entropy of Surroundings
Change S_universe = Change S_surroundings + Change S_system where for a reversible process: change in S= q_rev/T
spontaneous reaction
increases the entropy of the universe
non-spontaneous
decrease the entropy of the universe
change in entropy of the universe is greater than 0
spontaneous reaction; favored process
change in entropy of the universe is less than 0
nonspontaneous reaction; disfavored
change in entropy of the universe is equal to 0
at equilibrium; neither favored or disfavored
Heat capacity
(C: J/K) objects that are heated or cooled without a change in phase experience a change in temperature–physical and extensive property of matter
q=CΔT
molar heat capacity
(C_m: J/mol K) amount of heat required to change one mole of a substance one Kelvin
q=nC_mΔT
Specific Heat Capacity
(c: J/gK) amount of heat required to change one mole of a substance one Kelvin
q=mcΔT
heat capacity changes with
phase that the object or substance is given in
Molar Heat Capacity–> Specific Heat Capacity
c(X) = C(X) M(X)^-1
Specific Heat Capacity–> Molar Heat Capacity
C(X)=c(X) M(X)
Work
(w) form of energy transfer
Internal Energy
(U) energy of a system necessary too bring the system from its standard (internal) state to its present internal state of interest
- accounts for the kinetic and potential energy microscopically. That is, it accounts for the kinetic energy of molecules (motion, vibrations, and rotations) as well as potential energy arising from chemical bonds and intermolecular forces.
Change in internal energy
ΔU=q+w