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Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
First law of thermodynamics
Polytropic process
Isentropic process
Isothermal process
Isobaric process
Isochoric process
Energy (E)
Heat (Q)
𝐻2 − 𝐻1
𝐻𝑔 − 𝐻𝑓
= 𝐻𝑓𝑔
m*C*ΔT
m*Cv*ΔT
m*Cp*ΔT
ሶ
𝑚 * H.V
Work (W)
T * 𝜔
1
2
𝑘(x2
2
− 𝑥1
2
)
ሶ
𝑊 = 𝑉 ∗ 𝐼
Internal
Energy (U)
Kinetic Energy
(KE)
1
2
𝑚𝑉2
Potential
Energy (PE)
M*g*z
Moving Flow
Work
P*V
▪Polytropic process
▪Isentropic process
▪Isothermal process
▪Isobaric process
▪Isochoric process
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
▪Polytropic process
▪Isentropic process
▪Isothermal process
▪Isobaric process
▪Isochoric process
Expansion and compression work is often called moving boundary work
𝒅𝑾=𝑷×𝒅𝑽
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
P=f(V)
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
𝑷𝑉𝑛=𝑪,where n and C are constants. Polytropic process 𝑷1V1
𝑛
= 𝑷2V2
𝑛
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
(n=𝜸)
𝑷𝑉𝑛=𝑪
Polytropic process
Isentropic process
Adiabatic (Q=0) and Reversible (S=C)
𝜸 is the specific heat ratio = 𝑪𝒑/𝑪𝒗
Isothermal process
(n=𝟏)
Isobaric process
(n=0)
Isochoric process
(n=∞)
P
v
𝑃𝑉 = 𝑚ℝ𝑇
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
Air expanded according to 𝑷𝑉1.33=𝑪 from 5 bar, 227℃ to 1 bar, and then heated at constant
pressure to original temperature.
Determine total work done and amount of heat transferred
Solution
𝑷𝑉𝑛=𝑪
P
v
1
2 3
𝑤𝑡𝑜𝑡𝑎𝑙 = 𝑤1:2 + 𝑤2:3
𝑃𝑉 = 𝑚ℝ𝑇
0.287
1 kg
𝑉2 = ? ?
𝑉1 = 0.284 𝑚3
𝑉3 = 1.421 𝑚3
𝑇2 = 335 𝐾 = 62 ℃ 𝑉2 = 0.952 𝑚3
=
−505 ∗0.952+101 ∗0.284
1−1.33
+ 101 1.421 − 0.952 = +1417.3 𝑘𝐽 𝑎
+47.4 KJ
+1369.9 KJ
𝑞𝑝𝑜𝑙=
ϒ−𝑛
ϒ−1
* 𝑤𝑝𝑜𝑙 +239.5 KJ
𝑞𝑖𝑠𝑜𝑏𝑎𝑟𝑖𝑐= 𝑐𝑝 ∗ (𝑑𝑇 ) +165.825 KJ

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13.pdf

  • 1. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com First law of thermodynamics Polytropic process Isentropic process Isothermal process Isobaric process Isochoric process
  • 2. Energy (E) Heat (Q) 𝐻2 − 𝐻1 𝐻𝑔 − 𝐻𝑓 = 𝐻𝑓𝑔 m*C*ΔT m*Cv*ΔT m*Cp*ΔT ሶ 𝑚 * H.V Work (W) T * 𝜔 1 2 𝑘(x2 2 − 𝑥1 2 ) ሶ 𝑊 = 𝑉 ∗ 𝐼 Internal Energy (U) Kinetic Energy (KE) 1 2 𝑚𝑉2 Potential Energy (PE) M*g*z Moving Flow Work P*V ▪Polytropic process ▪Isentropic process ▪Isothermal process ▪Isobaric process ▪Isochoric process Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
  • 3. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com ▪Polytropic process ▪Isentropic process ▪Isothermal process ▪Isobaric process ▪Isochoric process Expansion and compression work is often called moving boundary work 𝒅𝑾=𝑷×𝒅𝑽
  • 4. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com P=f(V)
  • 5. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com 𝑷𝑉𝑛=𝑪,where n and C are constants. Polytropic process 𝑷1V1 𝑛 = 𝑷2V2 𝑛
  • 6. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com (n=𝜸) 𝑷𝑉𝑛=𝑪 Polytropic process Isentropic process Adiabatic (Q=0) and Reversible (S=C) 𝜸 is the specific heat ratio = 𝑪𝒑/𝑪𝒗 Isothermal process (n=𝟏) Isobaric process (n=0) Isochoric process (n=∞) P v 𝑃𝑉 = 𝑚ℝ𝑇
  • 7. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com Air expanded according to 𝑷𝑉1.33=𝑪 from 5 bar, 227℃ to 1 bar, and then heated at constant pressure to original temperature. Determine total work done and amount of heat transferred Solution 𝑷𝑉𝑛=𝑪 P v 1 2 3 𝑤𝑡𝑜𝑡𝑎𝑙 = 𝑤1:2 + 𝑤2:3 𝑃𝑉 = 𝑚ℝ𝑇 0.287 1 kg 𝑉2 = ? ? 𝑉1 = 0.284 𝑚3 𝑉3 = 1.421 𝑚3 𝑇2 = 335 𝐾 = 62 ℃ 𝑉2 = 0.952 𝑚3 = −505 ∗0.952+101 ∗0.284 1−1.33 + 101 1.421 − 0.952 = +1417.3 𝑘𝐽 𝑎 +47.4 KJ +1369.9 KJ 𝑞𝑝𝑜𝑙= ϒ−𝑛 ϒ−1 * 𝑤𝑝𝑜𝑙 +239.5 KJ 𝑞𝑖𝑠𝑜𝑏𝑎𝑟𝑖𝑐= 𝑐𝑝 ∗ (𝑑𝑇 ) +165.825 KJ