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110 Terms

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System definition
whatever part of the universe we choose to study
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Surroundings definiton
the parts of the universe we didnt choose to study
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Closed definition
no particle exchange between the system and the surrounding
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Adiathermal definition
no heat exchange allowed
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Adiabatic definition
adiathermal and reversible
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Isothermal
constant temperature
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Isobaric
constant pressure
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Isovolumic
constant volume
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Phase
a region within the system that is homogeneous with well defined boundaries
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Equilibrium
a state without change
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Function of state definition
any physical quantity that has a well defined value for each equilibrium state
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Extensive definition
quantities that are proportional to system size
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Intensive definition
quantities that are independent of system size
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Zero-th law of thermodynamics
Two systems in thermal equilibrium with a third are also in thermal equilibrium with each other
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redundancy definition
more functions of state than independent variables
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reciprocity theorem
(dx/dy)z(dy/dz)x(dz/dx)y \= -1
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why do functions of state always have exact differentials
because they are single valued
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First law of thermodynamics
Energy is conserved if heat is taken into account
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First law of thermodynamics equation
deltaE \= deltaQ + deltaW
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Heat capacity equation
C \= dQ/dT
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Isothermal expansion equation
delta Q \= RT ln(V2/V1)
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Adiabatic expansion equation
TV^(gamma - 1) \= const
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Second law of thermodynamics
entropy always increases
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Heat engine
a device that converts thermal energy into mechanical energy
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A to B in carnot cycle
isothermal expansion
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B to C in carrnot cycle
adiabatic expansion
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C to D in carnot cycle
isothermal compression
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D to A in carnot cycle
adiabatic compression
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How do you find the total work done of a carnot cycle
The area of the p-v graph
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what is W in thermodyamics
work done on the system
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what is W in heat engines
work done by the system
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what is Qh in heat engines
heat absorbed by the system
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what is Ql in heat engines
heat released by the system
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A to B carnot cycle equation
Qh \= RTh ln(VB/VA)
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B to C carnot cycle equation
Th/Tl \= (VC/VB) ^ gamma - 1
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C to D carnot cycle equation
Ql \= RTl ln(VC/VD)
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D to A carnot cycle equation
Tl/Th \= (VA/VD)^ gamma - 1
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What is the efficiency for a heat engine?
the work done divided by the heat
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What is the efficiency for a refrigerator?
the heat divided by the work done
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Carnots theorem
No real engine operating between two energy reservoirs can be more efficient than a Carnot engine
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Thermodynamic temperature scale equation
theta 2 \= theta 1 Q1/Q2
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entropy equation
dS \= dQ/T
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Work done equation
W \= - integral pdV
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What is the heat released by a system when the energy does not depend on the volume?
the work done
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where is entropy defined up to?
an arbitrary additive constant
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Define entropy in classical thermodynamic terms
dS \= dQrev/T, the entropy is defined up to an arbitrary additive constant, S(B) - S(A) \= integral from A to B dQrev/T
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State the law of increase in entropy, sometimes known as the third statement of the second law of thermodynamics
The entropy of an isolated system tends to a maximum
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What is the second statement of the second law
heat goes from hot to cold
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What is the heat capacity of diatomic air?
Cp \= 7/2 R
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Do ideal gases depend on volume?
no
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What are some examples of extensive functions of state
Internal energy, volume, magnetisation
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What are some examples of intensive functions of state?
Temperature, pressure, magnetic field
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Why are microscopic quantities not functions of state?
Because they vary even when in equillibrium
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Why is work done of heat transferred not a function of state?
becuase they depend on the process and not just the states involved
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How was the first thermometer invented
by trapping air inside a cylinder which was sealed at the top and dipped in liquid in the bottom. As the trapped air cooled or heated liquid was pushed in or sucked out of the cylinder and the temperature could be found
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Examples of thermometers based on thermal expansion
bi-metalic strips, thermo-couples, liquid crystal
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using the ideal gas law how do we define temperature?
a system has a temperature T if it can maintain thermal equilibrium with an ideal gas at that temperatre
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What is the ideal gas equation for one mole (hint- pV\=nRT)
(dV/dT)p \= R/p
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what is the adiabatic index
the ratio of the heat capacities: gamma \= Cp/Cv
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what is the E for an ideal gas per mole
E \= 3RT/2
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what is the heat capacity for an ideal gas with constant volume?
Cv \= 3R/2
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What is the heat capacity for an ideal gas with constant pressure
Cp \= 5R/2
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what is the adiabatic index (gamma) for an ideal gas?
5/3
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For a real diatomic gas that is dilute enough to be ideal what is E
E \= 5RT/2 per mole
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For a real diatomic gas what is the heat capacity at a constant volume?
Cv \= 5R/2
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For a real diatomic gas what is the heat capacity at a constant pressure?
Cp \= 7R/2
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For a real diatomic gas what is the adiabatic index?
1.4
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In general for gas with more complex molecules what happens to the values of E and gamma
there are more available energy modes which lead to higher values of E and lower values of gamma
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for isothermal expansion what is dE?
dE \= 0 since we have constant internal energy
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For isothermal expansion is the work done by the gas on the surroundings or by the surroundings on the gas?
by the gas on the surroundings
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what is dQ for adiabatic expansion
dQ \= 0 since no heat is exchanged
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What is the equation for the adiabatic index (gamma)
gamma \= 1 + R/Cv
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Why are adiabatic lines always steeper than isotherms in p-V plots?
because the adiabatic index (gamma) is greater than 1
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What is a reversible processs
A process carried out so slowly that the system goes through an infinite sequence of equilibrium states (which are infinitely close together)
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What must there not be for a process to be reversible?
friction, turbulence or acceleration
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What does quasistatic mean
if we reverse the process exactly, we would recover the initial state
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What are irreversible processes defined by
an asymmetry in time
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What is kelvins statement
No process is possible whose sole result is the complete conversion of heat into work
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What is Clausius' statement
No process is possible whose sole result is the transfer of heat from a colder body to a hotter body
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What does the idea of a sole result require?
the system and surrounding to be returned o their initial state except for the heat and work mentioned
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What does a heat engine require?
a working substance which is used cyclically
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What is the difference between an adiabatic process and an isothermal process
adiabatic is a thermodynamic change where no heat is supplied, isothermal is a thermodynamic change where the temperature does not change
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For a carnot cycle in reverse is the work done by the system on the surroundings or by the surroundings on the system?
the surroundings does work on the system
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What is a carnot cycle in reverse?
a system that extracts heat from a lower temperature and delivers in to a higher temperature, like a fridge
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what is the equation for efficiency of a carnot engine
fancy n \= (Th-Tl)/Th
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what is the equation for efficiency of a carnot refridgerator
fancy n \= Tl/(Th-Tl)
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What kind of heat engine does a thermodynamic temperature scale require
one that is reversible
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Clausius' inequality equation
closed integral dQ/T
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What is T in clausius' inequality?
the temperature of the external heat reservoir from which the heat dQ is supplied
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In clausius' inequality what does a negative indicate?
heat leaving the system
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equation for entropy change between phases
(S2 - S1) \= L/T where L is the latent heat
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What is the energy for equation in differential form
dE \= TdS - pdV
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What is the equation for enthalpy in differential form
dH \= TdS + Vdp
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What is the equation in differential form for Helmholtz free energy
dF \= -SdT - pdV
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What is the equation in differential form for Gibbs free energy
dG \= -SdT + Vdp
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What is gibbs free energy minimised for G(T, p)
systems with fixed pressure and temperature
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What is enthalpy minimised for? H(S,p)
systems with fixed pressure and heat
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What is energy minimised for E(S,V)?
systems with fixed volumes and heat
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What is helmholtz free energy minimised for F(T, V)
systems with fixed temperature and volume
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Applications of the thermodynamic potential energy (E(S,V)
isolated systems, mechanical equilibrium