Section XI – Second Law Applied to Open SystemsPage 1
SECTION XI – SECOND LAW APPLIED TO OPEN SYSTEM
6-54 Steam enters an adiabatic turbine at 5 MPa and 400C and leaves at a pressure of 200 kPa. Determine the maximum amount of work that can be delivered by this turbine.
Answer: 678.4 kJ/kg
Assumptions
Flow is steady,
i.e.
Flow is uniform at
the inlet and exit of turbine
ep and ekh
Given: Turbine is adiabatic
Conservation of energy applied to the turbine:
TI = 400C > Tsat = 263.99C corresponding to PI = 5 MPa steam is superheated at the inlet hi = 3195.7 kJ/kg, si = 6.6439 kJ/kg K
For maximum power output, flow through turbine must be isentropic (i.e. no loses since turbine is adiabatic) si = se = 6.6459 kJ/kg K
sef < se < seg steam is a saturated liquid-vapour mixture at the exit
Exit quality:
Exit enthalpy:
6.61Steam expands in a turbine steadily at a rate of 25,000 kg/h, entering at 8 MPa and 450C and leaving at 50 kPa as saturated vapor. If the power generated by the turbine is 4 MW, determine the rate of entropy generation for this process. Assume the surrounding medium is at 25C. Answer: 8.38 kW/K
Assumptions:
Flow is uniform at exit and inlet of turbine
epekh
Given:
Flow is steady
Conservation of energy applied to the turbine:
Inlet conditions: PI = 8 MPa, TI = 450C
TI = 450C > Tsat = 295.06C corresponding to PI = 8 MPa steam is superheated at the inlet.
hi = 3272.0 kJ/kg, si = 6.5551 kJ/kg K
Exit conditons: Pe = 50 KPa, saturated vapour
Second Law: dStot 0
6.65A 0.1 m3 rigid tank initially contains refrigerant-12 at 1 MPa and 100 percent quality. The tank is connected by a valve to a supply line that carries refrigerant-12 at 1.4 MPa and 30C. The valve is now opened, allowing the refrigerant to enter the tank, and it is closed when it is observed that the tank contains only saturated liquid at 1.2 MPa. Determine (a) the mass of the refrigerant that entered the tank, (b) the amount of heat transfer with the surroundings at 50C, and (c) the entropy generated during this process.
Answers: (a) 115.67 kg, (b) 1564 kJ, (c) 0.0907 kJ/K.
Assumptions:
Pressure drop through valve is
negligible
Flow is uniform at the inlet
R-12 is at uniform state in tank
ep and ek < h at the inlet
Given:
Tank is rigid d = 0 W12 = 0
Conservation of mass
(a)
u1 = u1g = 186.32 kJ/kg, u2 = u2f = 83.22 kJ/kg
s1 = s1g = 0.6820 kJ/kg K, s2 = s2f = 0.3015 kJ/kg K
P1 = 1.4 MPa, TI = 30C < Tsat = 56.09C corresponding to PI = 4 MPa R-12 is subcooled (or compressed) at the inlet.
Difference between hi(i) and hi(ii) is less than 1% hi(i) will be used here
Conservation of energy:
(b)
(d=0)
Second Law:
(c)
5.66Fifty kilojoules of heat is transferred from a thermal-energy reservoir at 500 K to the environment at 15C. Calculate the change in entropy of the reservoir and the change in entropy of the environment. Show that the total entropy change satisfies the second law. If the amount of heat transfer remains unchanged, but the reservoir temperature is lower, what effect does this have on the total entropy change? Explain.
Entropy change of thermal-energy reservoir
Entropy change of the environment
Total change of entropy: (S)tot = (S)R + (S)E
second law not violated
As TR TE, (S)tot 0 process reversible