THERMO7 Flashcards

1
Q

2nd Law of Thermodynamics

Calussius

A

-no process is possible whose sole result is the transfer of heat from a colder body to a hotter body

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2
Q

2nd Law of Thermodynamics

Kelvin

A

-no process is possible whose solo result is the complete conversion of heat into work

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3
Q

Coefficient of Performance

Equation

A

useful product / necessary input

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4
Q

In a complete cycle on a PV diagram…

A

… ΔEint = 0
… net work done = are enclosed
… clockwise, Won is -ve and Qin is +ve
… anticlockwise, Won is +ve and Qin is -ve

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5
Q

2nd Law of Thermodynamics

Refrigerator Statement

A

-it is impossible for a refrigerator working in a cycle to produce only the effect of extracting heat from a cold object and reject the same amount of heat to a hot object

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6
Q

Refrigerators / Air Conditioning

A
Qh = W + Qc
COP = Qc / W
Qh = heat removed to hot reservoir
Qc = heat added from cold reservoir
W = work put in
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7
Q

Heat Pump

A
Qh = W + Qc
COP = Qc / W
Qh = heat removed
Qc = heat added
W = work put in
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8
Q

Heat Engines

A
Qh = W + Qc
COP = W / Qh = (Qh-Qc)/Qh = 1 - Qc/Qh
Qh = heat added from hot reservoir
Qc = heat removed to cold reservoir
W = work output from engine
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9
Q

2nd Law of Thermodynamics

Heat-Engine Statement

A

-it is impossible for a heat engine working in a cycle to produce only the effect of extracting heat from a single reservoir and performing an equivalent amount of work

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10
Q

Theoretical Maximum Efficiency

A

ε = 1 - Tc/Th

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11
Q

Entropy

Definition

A
  • a measure of the disorder of a system
  • hot -> cold
  • order -> disorder
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12
Q

Entropy

Statistical Mechanics Approach

A

-disorder isn’t more favourable than order, it is just that there are many more ways / arrangements of a system that are disordered rather than ordered
-as time passes the entropy of the universe increases
S = k log

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13
Q

Entropy

Classical Thermodynamics Approach

A

-for a reversible process, dS = dQ/T
-entropy is a state variable so ΔS depends only on the initial and final states, not the path
ΔS = ∫ dS = ∫ dQ/T

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14
Q

Adiabatic Expansion and Entropy

A

dS = dQ/T
-but for an adiabatic process, dQ = 0 so dS =0
ΔS = ∫ dS so there is no change in entropy
-there is an increase in disorder from the gas occupying a greater volume as there are more possible disordered arrangements of the system
-but this is exactly balanced out by the decrease in disorder due to the reduced molecular speeds at a lower temperature

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15
Q

Free Expansion and Entropy

A

-insulated container so, Q = 0
-the gas is expanding into a vacuum so, W = 0
-from the 1st law, ΔEint = Q + W = 0
-so, ΔT = 0
-the free expansion is isothermal so Qin = -nRTln(Vi/Vf)
dS = dQ/T
ΔS = Q/T = -nR
ln(Vi/Vf)

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16
Q

Tc and Th

A
Tc = temperature of the system
Th = temperature of the surroundings
17
Q

Entropy of the Universe

A
-universe = system + surroundings
Tc < Th
ΔSsys = Q/Tc and ΔSsur = - Q/Th
ΔSuni = Q/Tc + (- Q/Th) = Q/Tc - Q/Th
-as Tc < Th this means that ΔS≥0
-so ΔS can never be negative so the entropy of a universe always tends to a maximum
18
Q

Carnot Cycle

Definition

A
  • a theoretical thermodynamic cycle with maximum efficieny

- reversible

19
Q

Carnot Cycle

Processes

A
-cycle between four points on a PV diagram
1 to 2: isothermal
2 to 3: adiabatic
3 to 4: isothermal 
4 to 1: adibatic
20
Q

Carnot Cycle

Equations and Explainations

A

1 to 2: Qh is absorbed so entropy increases by ΔS=Qh/Th
2 to 3: Qin = 0 so ΔS = 0
3 to 4: Qc is expelled so entropy decreases by ΔS=Qc/Tc
4 to 1: Qin = 0 so ΔS = 0

21
Q

Carnot Cycle

Entropy and Reversibility

A
  • to be reversible net ΔS = 0 in either direction

- because is ΔS was greater than zero, it would be negative in the opposite direction and ΔS≥0 would be violated

22
Q

Carnot Cycle

Maximum Theoretical Efficiency

A

ε = W / Qin = 1 - Qc/Qh
-but for carnot cycle, Qc=TcΔS and Qh=ThΔS
ε = 1 - TcΔS/ThΔS = 1 - Tc/Th