Dr. Mohammed H. Ahmed College of Petroleum and Mining Engineering University of Mosul • Engineering Thermodynamics: Work and Heat Transfer Book by G. F. C. Rogers and Y. R. Mayhew • Applied Heat for Engineers Thermodynamics • Applied Thermodynamics for Engineering Technologists (5th Edition) T.D. Eastop , A. Mcconkey Octave Sneeden, Samuel Vallance Kerr Lecture 7,8 π12 = 0 π12 = −βπ’12 Ex.13/ A closed vessel having a volume of 0.4 m3 contains 2.0 kg of a liquid water and water vapor mixture in equilibrium at a pressure of 6 bar (0.6 MPa). Calculate: a) The volume and mass of the liquid. π3 b) The volume and mass of the vapor. (Take π£π = 0.001101 ππ , π£π π3 = 0.3156 ππ ) 4. Adiabatic process An adiabatic process occurs without transfer of heat or mass of substances between a thermodynamic system and its surroundings. (Isolated) πΈππ = π Apply the N.F.E.E πΈππ = πΎππ + βπππ ∴ πΎππ = −βπππ For this process that is a property has constant through reversible adiabatic process which called “Entropy (s)” π π·π π = π −ππͺπ π»π − π»π Take differentials, π·π π = −ππͺπ π π» And we have; ππ = ππ π βΉ π·= And we have; πͺπ = ππΉπ» π½ πΉ πΈ−π ππ£ π ππ π =π ππ‘ π (πΎ − 1) ππ£ 1 ππ‘ =− π (πΎ − 1) π 2 1 ππ£ 1 =− π (πΎ − 1) 2 1 ππ‘ π 1 2 ln π 1 = − [ln π] 1 (πΎ − 1) 2 π2 π2 −(πΎ − 1)ln = ln π1 π1 π2 ln π1 π2 π1 −(πΎ−1) −(πΎ−1) π2 = ln π1 π2 = π1 ∴ π1 π1 (πΎ−1) = π2 π2 (πΎ−1) or π1 π2 = π2 π1 (πΎ−1) (i.e) ππ (πΎ−1) = ππππ π‘πππ‘ π1 π1 π1 as; π1 π2 = π2 π2 π2 (πΎ−1) = βΉ π2 π1 = π2 π2 π1 π1 π2 π2 π1 π1 π1 π1 . π1 (πΎ−1) = π2 π2 . π2 (πΎ−1) ∴ π1 π1 (i.e) (πΎ) = π2 π2 ππ£ (πΎ) = ππππ π‘πππ‘ π1 π2 = π2 π1 πΎ (πΎ) From the equation of adiabatic process; ∴ πΎππ = −βπππ = −ππΆπ£ π2 − π1 , let say per 1 kg = πΆπ£ π1 − π2 And, πΆπ£ = π πΎ−1 π12 π π1 − π2 = πΎ−1 π12 π1 π£1 − π2 π£2 = πΎ−1 We have, ππ£ = π π, And for reversible process, π£2 π12 = ππ£ (πΎ) = ππππ π‘πππ‘ πππ£ π£1 Then, π12 = π£2 πΆ.ππ£ π£1 π£ πΎ = πΆ. π12 = πΆ. π£2 ππ£ π£1 π£ πΎ −πΎ+1 π£2 π£ −πΎ + 1 π£2 −πΎ+1 − π£1 −πΎ+1 = πΆ. = πΆ. 1−πΎ π£1 π£1 −πΎ+1 − π£2 −πΎ+1 πΎ−1 And ππ£ (πΎ) = ππππ π‘πππ‘ ∴ π12 = π1 π£1 πΎ π£11−πΎ − π2 π£2 πΎ π£21−πΎ πΎ−1 ∴ π12 = = π1 π£1 − π2 π£2 πΎ−1 π1 π£1 − π2 π£2 πΎ−1 Ex.14/0.285 m3 of air at a pressure of 2.7 bar is expanded to volume of 0.708 m3. find the work during expansion for each of the following process: - Constant pressure - Isothermal - adiabatic Thank you for your attention Next lecture: Application for open system