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isothermal process
constant temp
internal energy and enthalpy = 0
Q = -W
Isobaric process
constant pressure
Q=H
Isochoric
constant volume
Q=U
W=0
Adiabatic Process
no Q
W = U
irreversable processes
produces work-multiply by efficiency
requires work- divide by efficiency
compressibility factor (Z)
measure of the deviation of the real-gas molar value from its ideal-gas value
ideal-gas state- V=V(ig), Z=1
moderate temps Z < 1
elevated temps Z > 1
Van Der Waals equation
sensible heat effect
heat transfer with no phase transitions, chemical reactions, or composition
temperature of the system changes
latent heats
amount of heat absorbed or released during a phase change
constant temp and pressure
types: fusion, vaporization
Standard State
if in standard state, known as standard heat of reaction
state of a substance at specified pressure, composition, and physical condition, e.g., gas, liquid, or solid
based on pressure of 1 bar(105 Pa)
can be calculated if the standard heats of formation at the same temp are known
formation reaction
a reaction that produces a single compound from its constituent elements
based on 1 mol of compound formed
heat of combustion
chemical reaction where substance reacts with oxygen and releases heat
usually forms carbon dioxide and water
Entropy
intrinsic property
reflects how energy is dispersed and spread out in a system
transferred along with heat
if you add heat, entropy increases (more randomness)
removing heat (to make work as in steam engines), not all of the heat is used for the work
in thermo: measure of a system’s thermal energy per unit temperature that is unavailable for doing useful work
“Tax paid whenever you try to convert heat into motion”
high entropy: energy spread
low entropy: concentrated, bundled up energy
over time systems move towards a state of maximum entropy because entropy can only increase (remain in constant reversible process)
ex: melting of ice, spreading perfume, hot object cooling
heat flows from hot to cold
heat engines
rely on high temperature source of heat and discard heat to the environment
ex: internal combustion engine and steam power plant
second law imposes restrictions on how much of the heat intake can be converted to work
since engines operate in cycles, U=0, W= - (QH+ QC)
energy that flows from the higher temp reservoir, must flow out as work or as heat transfer to the low temp reservoir
thermal efficiency of a heat engine
ratio of the work produced to the hear supplied to the engine
Carnot engine
heat engine that operates in a completely reversible manner