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Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
Reversibility , Irreversibility, Entropy in pure substance , Entropy change.
PT.02
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
P
v
1
2
ර
𝛿𝑄
𝑇
=
𝛿𝑄𝐻
𝑇
⃒A -
𝛿𝑄𝐿
𝑇
⃒B
A
B
C
ර
𝛿𝑄
𝑇
=
𝛿𝑄𝐻
𝑇
⃒C -
𝛿𝑄𝐿
𝑇
⃒B
ර
𝛿𝑄
𝑇
≤ 0
0
𝛿𝑄𝐻
𝑇
⃒C
𝛿𝑄𝐻
𝑇
⃒A
Independent of the path
𝛿𝑄𝐻
𝑇
Pressure ( P ) Temperature ( T ) Enthalpy ( H )
Entropy ( S )
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
Entropy ( S ) All things trend toward disorder.
Entropy is simply a measure of disorder
Independent of the path
𝛿𝑄𝐻
𝑇 Entropy ( S )
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
Entropy ( S )
ර
𝛿𝑄
𝑇
≤ 0
Reversible Irreversible
𝑑𝑆 =
𝛿𝑄
𝑇
𝑑𝑆 >
𝛿𝑄
𝑇
ර
𝛿𝑄
𝑇
ර
𝛿𝑄
𝑇
0 0
P
v
1
2
A
B
Reversible
ර
𝛿𝑄
𝑇
= ‫׬‬
1
2 𝛿𝑄𝐻
𝑇
⃒A + ‫׬‬
1
2 𝛿𝑄𝐻
𝑇
⃒B = 0
𝛿𝑄𝐻
𝑇
⃒C
𝛿𝑄𝐻
𝑇
⃒A
ර
𝛿𝑄
𝑇
= ‫׬‬
1
2 𝛿𝑄𝐻
𝑇
⃒c + ‫׬‬
1
2 𝛿𝑄𝐻
𝑇
⃒B < 0
𝛿𝑄
𝑇
⃒irreversible < 𝑑𝑆
c
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
𝛿𝑄
𝑇
⃒irreversible < 𝑑𝑆
𝑆2 − 𝑆1 = ‫׬‬1
2 𝛿𝑄𝐻
𝑇
+𝛿𝑆𝑔𝑒𝑛
𝛿 𝑆𝑆𝑈𝑅𝑅𝑂𝑈𝑁𝐷𝐼𝑁𝐺
Temperature ( T0 )
Q
𝑊
𝑆𝑆𝑈𝑅 =
−𝑄
T0
𝛿𝑆𝑆𝑌𝑆𝑇𝐸𝑀
𝐿𝑖𝑞𝑢𝑖𝑑 & 𝑆𝑜𝑙𝑖𝑑
𝐺𝑎𝑠
𝛿𝑆 = 𝑚 𝐶𝑣 ln(
𝑇2
𝑇1
)
𝛿𝑆 = 𝑚 𝐶𝑣 ln(
𝑇2
𝑇1
) + m R ln(
𝑣2
𝑣1
)
𝑷𝟐
𝑷𝟏
=
𝝆𝟐
𝝆𝟏
𝜰
=
𝒗𝟏
𝒗𝟐
𝜰
=
𝑻𝟐
𝑻𝟏
𝜰
𝜰 −𝟏
Isentropic relations
Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com
Comment with your questions

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10.pdf

  • 1. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com Reversibility , Irreversibility, Entropy in pure substance , Entropy change. PT.02
  • 2. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com P v 1 2 ර 𝛿𝑄 𝑇 = 𝛿𝑄𝐻 𝑇 ⃒A - 𝛿𝑄𝐿 𝑇 ⃒B A B C ර 𝛿𝑄 𝑇 = 𝛿𝑄𝐻 𝑇 ⃒C - 𝛿𝑄𝐿 𝑇 ⃒B ර 𝛿𝑄 𝑇 ≤ 0 0 𝛿𝑄𝐻 𝑇 ⃒C 𝛿𝑄𝐻 𝑇 ⃒A Independent of the path 𝛿𝑄𝐻 𝑇 Pressure ( P ) Temperature ( T ) Enthalpy ( H ) Entropy ( S )
  • 3. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com Entropy ( S ) All things trend toward disorder. Entropy is simply a measure of disorder Independent of the path 𝛿𝑄𝐻 𝑇 Entropy ( S )
  • 4. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com Entropy ( S ) ර 𝛿𝑄 𝑇 ≤ 0 Reversible Irreversible 𝑑𝑆 = 𝛿𝑄 𝑇 𝑑𝑆 > 𝛿𝑄 𝑇 ර 𝛿𝑄 𝑇 ර 𝛿𝑄 𝑇 0 0 P v 1 2 A B Reversible ර 𝛿𝑄 𝑇 = ‫׬‬ 1 2 𝛿𝑄𝐻 𝑇 ⃒A + ‫׬‬ 1 2 𝛿𝑄𝐻 𝑇 ⃒B = 0 𝛿𝑄𝐻 𝑇 ⃒C 𝛿𝑄𝐻 𝑇 ⃒A ර 𝛿𝑄 𝑇 = ‫׬‬ 1 2 𝛿𝑄𝐻 𝑇 ⃒c + ‫׬‬ 1 2 𝛿𝑄𝐻 𝑇 ⃒B < 0 𝛿𝑄 𝑇 ⃒irreversible < 𝑑𝑆 c
  • 5. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com 𝛿𝑄 𝑇 ⃒irreversible < 𝑑𝑆 𝑆2 − 𝑆1 = ‫׬‬1 2 𝛿𝑄𝐻 𝑇 +𝛿𝑆𝑔𝑒𝑛 𝛿 𝑆𝑆𝑈𝑅𝑅𝑂𝑈𝑁𝐷𝐼𝑁𝐺 Temperature ( T0 ) Q 𝑊 𝑆𝑆𝑈𝑅 = −𝑄 T0 𝛿𝑆𝑆𝑌𝑆𝑇𝐸𝑀 𝐿𝑖𝑞𝑢𝑖𝑑 & 𝑆𝑜𝑙𝑖𝑑 𝐺𝑎𝑠 𝛿𝑆 = 𝑚 𝐶𝑣 ln( 𝑇2 𝑇1 ) 𝛿𝑆 = 𝑚 𝐶𝑣 ln( 𝑇2 𝑇1 ) + m R ln( 𝑣2 𝑣1 ) 𝑷𝟐 𝑷𝟏 = 𝝆𝟐 𝝆𝟏 𝜰 = 𝒗𝟏 𝒗𝟐 𝜰 = 𝑻𝟐 𝑻𝟏 𝜰 𝜰 −𝟏 Isentropic relations
  • 6. Ahmed Medhat - Thermodynamics 1 - ahmedhatfa@hotmail.com Comment with your questions