Lecture 16 thermal processes.
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Transcript of Lecture 16 thermal processes.
![Page 1: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/1.jpg)
Lecture 16Thermodynamic processes
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Types of processes
Reversible• must be slow (quasistatic: system has time to go to equilibrium after each change) • system is in equilibrium at all points along the process• corresponds to a line in pV diagram• can be run in reverse
eg: He balloon shrink in liquid N and expands.
Irreversible• often fast (but not always)• is not a line in pV diagram (you can only mark initial and final states)• cannot run in reverse
eg. explosion
DEMO: Reversible and
irreversible processes
![Page 3: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/3.jpg)
Basic thermodynamic processes
W p V
0W
0 f or ideal gasesU
0Q
• Isobaric: Constant p
• Isochoric: Constant V
• Isothermal: Constant T
• Adiabatic: No heat exchange
• An infinite number of other processes without any special name!
![Page 4: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/4.jpg)
An ideal monoatomic gas is trapped in a cylindrical container whose cap is a piston of negligible mass that can slide up and down the cylinder. The gas is initially at room temperature (298K) and occupies a volume of 1.0 m3. The piston is in its equilibrium position.
(1)A mild heat source is then applied at the base of the container, and the gas is then slowly warmed up to 350K while the piston moves up to allow the gas to expand. Once the new temperature is reached, the volume of the gas is 2.0 m3.
(2) The piston is locked in the new position and the gas is allowed to cool down to room temperature.
(3) Finally, when room temperature is reached, the piston is pushed back manually but very slowly, so that the gas is allowed to remain in thermal equilibrium with the air in the room at all times. At the end, the piston is back in its initial position.
Example: Ideal gas cycle
Isobaric expansion
Isochoric cooling
Isothermal compression
![Page 5: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/5.jpg)
p
V
1
2
1.0 m3 2.0 m3
3
278 K
350 K
A B
CpC
1 atm
![Page 6: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/6.jpg)
p
V
1
2
1.0 m3
2.0 m3
3
278 K
350 K
A B
CpC
1 atmWork for each process:
5 3 51 A B A 1.01 10 Pa 1.0 m 1.0 10 JW p V V
2 0W
A
C3
V
VW pdV
AA
C
lnV
nRTV
I deal gas: nRT
pV
A
C
AV
V
nRTdV
V
5 3 411.01 10 Pa 1.0 m ln 7.0 10 J
2
AA A
C
lnV
pVV
A A
A
f rom state A: pV
n nRT
4cycle 1 2 3 3.1 10 JW W W W
![Page 7: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/7.jpg)
p
V
1
2
1.0 m3
2.0 m3
3
278 K
350 K
A B
CpC
1 atmChange in internal energy for each process:
1 B A
3 32 2
U nRT nRT
A A
A
f rom state A: pV
n nRT
B AA A
A
32
T TpV
T
43.9 10 J
2 C B
3 32 2
U nRT nRT 1U C Asince T T
3 0 (isothermal)U
cycle 0U
![Page 8: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/8.jpg)
p
V
1
2
1.0 m3
2.0 m3
3
278 K
350 K
A B
CpC
1 atmHeat for each process:
1 1 1Q U W 51.4 10 J
2 2 2Q U W 43.9 10 J
3 3 3Q U W 47.0 10 J
4cycle 1 2 3 3.1 10 JQ Q Q Q cycle good!W
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Heat capacities
Take any process with a change in temperature, find heat Q. Their relation is the definition of heat capacity!
Process at constant volume:
VdQ nC dT
p
V
Process at constant pressure:
PdQ nC dT
p
V
Process X!p
V
XdQ nC dT
![Page 10: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/10.jpg)
Heat capacities (ideal gas)
Process at constant volume:
VdU dQ nC dT
Process at constant pressure:
dW pdV
0W
dU dQ dW
PnC dT pdV
PnC dT nRdT
pV nRT
pdV nRdT
V PnC dT nC dT nRdT
But: For the same change in temperature, the change in internal energy must be the same!
P VC C R
Also, good news: we can use for any process!
VdU nC dT
![Page 11: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/11.jpg)
Ratio of heat capacities
P
V
C
C
Ideal gas:
Monoatomic5
52 1.673 32
P
V
RC
CR
Diatomic7
72 1.45 52
P
V
RC
CR
3 J12.47
2 mol K5 J
20.78 2 mol K
V
P V
C R
C C R R
J5 / 2 20.78
mol K7 J
29.09 2 mol K
V
P V
C R
C C R R
![Page 12: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/12.jpg)
It works!
![Page 13: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/13.jpg)
ACT: Different heating processes
Two containers have each 1 mole of monoatomic ideal gas inside. Heat is transferred into both, causing a 50°C rise in temperature. For container A, this happens at constant volume. For container B, this happens at constant pressure. Which of the following is correct?
A. More heat is transferred into sample A
B. More heat is transferred into sample B
C. Both samples absorb the same heat.
A
B
v
P
Q nC T
Q nC T
P v vC C R C A BQ Q
B A
J1 mole 8.31 50 K 415 J
mol Kp vQ Q n C C T nR T
How much more?
![Page 14: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/14.jpg)
Compression Stroke of Engines
If piston and cylinder are thermally insulated, no heat is transferred during compression, Q = 0 (adiabatic process)
In this stroke of an engine• Gas is compressed it does negative work• Internal energy increases• Temperature increases
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Adiabatic Gas Expansion
Piston is insulated so that, as gas expands, Q = 0
U Q W W with W > 0 (expansion), so ΔU < 0
ΔT < 0Temperature
decrease
![Page 16: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/16.jpg)
Adiabatic curve for ideal gases: T and V
I f 0, Q dU dW
VnC dT pdV
V
nRTnC dT dV
V
0V
dT R dVT C V
ln 1 ln constantT V
1 constantTV For expansion, T decreases
For compression, T increases1 0
1P V
V V
C CRC C
1 0dT dVT V
DEMO: Adiabatic
compression
![Page 17: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/17.jpg)
Adiabatic curve for ideal gases: p and V
1 constantTV
1 constantpV
VnR
constantpV
![Page 18: Lecture 16 thermal processes.](https://reader036.fdocuments.us/reader036/viewer/2022081505/5563ba3ad8b42a79028b54a8/html5/thumbnails/18.jpg)
Work in adiabatic processes
I f 0, Q W U
VW nC T
V
pVnC
nR
VW nC T
1
pV
1
pVW