Week 5 Lecture 7 Flashcards
Rate of entropy change =
Rate of entropy transfer + rate of entropy production
At steady state the rate of entropy change is ____
0
At steady state, the equation for rate of entropy is:
0 = rate of entropy transfer + rate of entropy production
The rate of entropy transfer =
Σ(Qk/Tk) + Σmisi - Σmjsj
(Qk/Tk) represents the heat transfer occuring at temperature Tk
i and j refer to the inlet and outlet streams
Rate of entropy production
S gen
Rate of entropy transfer + Rate of entropy production equation
Σ(Qk/Tk) + Σmisi - Σmjsj + S gen = 0
Entropy is not a ________ quantity
conserved
If the process is irreversible, there maybe an ________
internal generation
If the process is ________, there maybe an internal generation
irreversible
Type of diagram used for Rankine cycle
T-S diagram
T is for temperature
S is for entropy
enthalpy-entropy chart
h-s diagram
enthalpy-entropy chart
p-h diagram
pressure enthalpy diagram
constant entropy
isentropic
isentropic conditions are shown by a ____ line on T-S and H-S diagrams
straight vertical
example of a reversible heat engine
carnot cycle
The two vertical steps on a carnot engine are ____ processes
adiabatic
The two horizontal steps on a carnot engine are ____ processes
isothermal
Carnot engine adiabatic compression equation for work
W = nCv(Th-Tc)
Carnot engine adiabatic expansion equation for work
W = nCv(Tc-Th)
Carnot engine isothermal expansion equation for work
W = nRT ln(P2/P3)
Carnot engine isothermal compression equation for work
W = nRT ln(P1/P4)
Net work of carnot cycle =
net work = W12 + W23 + W34 + W41
as W12 and W34 cancel, net work reduces to
net work = W23 + W41
Type of diagram carnot cycle is shown on
P-V
Result of carnot engine analysis shows that
- No engine can be more efficient than the Carnot engine
- Net work extracted is the area inside the cycle
Thermal or cycle efficiency, for a reversible process =
η = 1 - Tc/Th
Reason why no engine can be more efficient than Carnot engine
irreversibility
COP refrigeration
COP = Tc/ (Th - Tc)
COP heat pump
COP = Th/ (Th - Tc)
For a reversible heat engine:
W = Qh/Th (Th - Tc)
Qh/Th = Qc/Tc
Used to produce most forms of electricity
Vapour power cycle
Rankine cycle components order
Pump
Boiler
Turbine
Condenser
Please Break The Chair
In Rankine cycle, has input of work
Pump
In Rankine cycle, has output of work
turbine
Process over the pump in rankine cycle
reversible adiabatic compression (isentropic)
Process over the turbine in rankine cycle
reversible adiabatic expansion (isentropic)
Rankine cycle heat input/output
Heat input > condenser heat output
Rankine cycle power input/output
Steam turbine power output»_space; pump power input
Type of diagram Rankine cycle usually depicted on
T-S diagram
High moisture content in the turbine leads to
Poor efficiency
Step in Rankine cycle where Qh is added to the system
boiler
Step in Rankine cycle where Qc exits the system
condenser