Week 5 Lecture 7 Flashcards

1
Q
A
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2
Q

Rate of entropy change =

A

Rate of entropy transfer + rate of entropy production

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3
Q

At steady state the rate of entropy change is ____

A

0

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4
Q

At steady state, the equation for rate of entropy is:

A

0 = rate of entropy transfer + rate of entropy production

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5
Q

The rate of entropy transfer =

A

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

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6
Q

Rate of entropy production

A

S gen

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7
Q

Rate of entropy transfer + Rate of entropy production equation

A

Σ(Qk/Tk) + Σmisi - Σmjsj + S gen = 0

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8
Q

Entropy is not a ________ quantity

A

conserved

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9
Q

If the process is irreversible, there maybe an ________

A

internal generation

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10
Q

If the process is ________, there maybe an internal generation

A

irreversible

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11
Q

Type of diagram used for Rankine cycle

A

T-S diagram

T is for temperature
S is for entropy

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12
Q

enthalpy-entropy chart

A

h-s diagram

enthalpy-entropy chart

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13
Q

p-h diagram

A

pressure enthalpy diagram

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14
Q

constant entropy

A

isentropic

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15
Q

isentropic conditions are shown by a ____ line on T-S and H-S diagrams

A

straight vertical

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16
Q

example of a reversible heat engine

A

carnot cycle

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17
Q

The two vertical steps on a carnot engine are ____ processes

A

adiabatic

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18
Q

The two horizontal steps on a carnot engine are ____ processes

A

isothermal

19
Q

Carnot engine adiabatic compression equation for work

A

W = nCv(Th-Tc)

20
Q

Carnot engine adiabatic expansion equation for work

A

W = nCv(Tc-Th)

21
Q

Carnot engine isothermal expansion equation for work

A

W = nRT ln(P2/P3)

22
Q

Carnot engine isothermal compression equation for work

A

W = nRT ln(P1/P4)

23
Q

Net work of carnot cycle =

A

net work = W12 + W23 + W34 + W41
as W12 and W34 cancel, net work reduces to
net work = W23 + W41

24
Q

Type of diagram carnot cycle is shown on

25
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
26
Thermal or cycle efficiency, for a reversible process =
η = 1 - Tc/Th
27
Reason why no engine can be more efficient than Carnot engine
irreversibility
28
COP refrigeration
COP = Tc/ (Th - Tc)
29
COP heat pump
COP = Th/ (Th - Tc)
30
For a reversible heat engine:
W = Qh/Th (Th - Tc) Qh/Th = Qc/Tc
31
Used to produce most forms of electricity
Vapour power cycle
32
33
34
Rankine cycle components order
Pump Boiler Turbine Condenser ## Footnote Please Break The Chair
35
In Rankine cycle, has input of work
Pump
36
In Rankine cycle, has output of work
turbine
37
Process over the pump in rankine cycle
reversible adiabatic compression (isentropic)
38
Process over the turbine in rankine cycle
reversible adiabatic expansion (isentropic)
39
Rankine cycle heat input/output
Heat input > condenser heat output
40
Rankine cycle power input/output
Steam turbine power output >> pump power input
41
Type of diagram Rankine cycle usually depicted on
T-S diagram
42
High moisture content in the turbine leads to
Poor efficiency
43
Step in Rankine cycle where Qh is added to the system
boiler
44
Step in Rankine cycle where Qc exits the system
condenser