the sum of the kinetic energy and the potential energy
open system
a system that can exchange thermal energy, work and matter with its surroundings
closed system
a system that can exchange thermal energy or work with its surroundings, but not matter
isolated system
a system that cannot exchange energy, work or matter with its surroundings
isobaric process
a process occurring at the gas with constant pressure
isovolumetric process
a process occuring at the gas with constant volume
isothermal process
a process occuring at the gas with constant temperature
adiabatic process
no thermal energy transfer between the gas and its surroundings in this process
Entropy
a thermodynamic quantity that relates to the degree of disorder of the particles in a system
microstate
a specific molecular configuration
macrostate
a larger-scale, measurable outcome, resulting from the outcome of each of the smaller microstates
spontaneously
one that occurs on its own, without any energy input from the outside
heat engine
a device which converts heat into useful mechanical energy
the clausius statement
It is impossible to construct a device which works on a cycle and produces no effect other than heattransfer from a coolbody to a hot body
the kelvin statement
it is impossible to devise a heat engine that takes heat from the hot reservoir ( Q H ) and converts all the energy into useful external work without losing heat to the cold reservoir ( Q C )
high entropy = high disorder
the first law of thermodynamics
The thermal energy entering a closed system is equal to the sum of the change in internal energy of the system and the work done by the system.
the second law of thermodynamics
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when Q is positive, thermal energy is supplied to the gas
when Q is negatice, thermal energy is removed from the gas
when the △U is positive, there is an increase in internal energy (kinetic energy increased, temperature increased)
when the △U is negative, there is an decrease in internal energy (kinetic energy decreased, temperature decreased)
when W is positive, work is being done by the gas (expansion)
when W is negative, work is being done on the gas (compression)
for isothermal process, △U = zero
no change in temp = no change in KE
for adiabatic process, Q is always zero
adiabatic expansion results in cooling
adiabatic compression results in heating
there is nochange in entropy in a carnot cycle
a carnot cycle is an reversible heat engine
Second Law of Thermodynamics
The total entropy of an isolated system always increases over time
Entropy (S)
A measure of disorder or randomness in a system
Enthalpy (H)
A measure of the total energy of a system, including internal energy and the energy associated with the pressure and volume of a system
Heat (Q)
Energy transferred from one body to another due to a temperature difference
Work (W)
Energy transferred from one body to another due to a force applied over a distance
Carnot Efficiency
The maximum possible efficiency of a heat engine, given by η = 1 - (Tc/Th)
Thermal Efficiency
The ratio of the work output to the heat input, given by η = W/Q
adiabatic process happens quickly = there isn't sufficient time for heat to be exchanged between the surroundings and the gas
when the process is irreversible, entropy is increasing throughout the process