5C-5 : | Open Feedwater Heater | 6 pts | ||||||
An open feedwater heater in a steam power plant operates at steady-state with liquid entering at T1 = 40oC and P1 = 7 bar. Water vapor at T2 = 200oC and P2 = 7 bar enters in a second feed stream. The effluent is saturated liquid water at P3 = 7 bar. If heat exchange with the surroundings and changes in potential and kinetic energies are negligible, determine the ratio of the mass flow rates of the two feed streams, mdot1 / mdot,2. | ||||||||
Read : | The feedwater heater is just a fancy mixer. When we write the MIMO form of the 1st Law at steady-state, there are three unknowns: the three mass flow rates. The states of all three streams are fixed, so we can determine the specific enthalpy of each of them. Mass conservation tells us that m3 = m1 + m2. We can use this to eliminate m3 from the 1st Law. Then we can solve the 1st Law for m1 / m2 ! |
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Given : | T1 | 40 | oC | Find : | ||||
P1 | 700 | kPa | mdot1 / mdot,2 = | ??? | ||||
T2 | 200 | oC | ||||||
P2 | 700 | kPa | ||||||
P3 | 700 | kPa | ||||||
Q | 0 | kW | ||||||
Diagram: | ||||||||
Assumptions: | ||||||||
1 - | The feedwater heater operates at steady-state. | |||||||
2 - | Changes in potential and kinetic energies are negligible. | |||||||
3 - | Heat transfer is negligible. | |||||||
4 - | No shaft work crosses the system boundary in this process. | |||||||
Equations / Data / Solve : | ||||||||
An open feedwater heater is essentially a mixer in which superheated vapor is used to raise the temperature of a subcooled liquid. We can begin our analysis with the steady-state form of the 1st Law. | ||||||||
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Eqn 1 | ||||||||
The assumptions in the list above allow us to simplify the 1st Law considerably: | ||||||||
Eqn 2 | ||||||||
Conservation of mass on the feedwater heater operating at steady-state tells us that : | ||||||||
Eqn 3 | ||||||||
We can solve Eqn 3 for mdot,3 and use the result to eliminate mdot,3 from Eqn 2. The result is: | ||||||||
Eqn 4 | ||||||||
The easiest way to determine mdot,1 / mdot,2 is to divide Eqn 4 by mdot,2. | ||||||||
Eqn 5 | ||||||||
Now, we can solve Eqn 5 for mdot,1 / mdot,2 : | ||||||||
Eqn 6 | ||||||||
Now, all we need to do is to determine the specific enthalpy of all three streams and plug these values into Eqn 6 to complete the problem. | ||||||||
First we must determine the phase(s) present in each stream. | ||||||||
Tsat(700kPa)= | 164.95 | oC | ||||||
Therefore: | Stream 1 is a subcooled liquid because T1 < Tsat | |||||||
Stream 2 is a superheated vapor because T2 > Tsat | ||||||||
T3 = Tsat because it is a saturated liquid. | ||||||||
Data from the Steam Tables of the NIST Webbook (using the default reference state) : | ||||||||
H1 | 168.15 | kJ/kg | H2 | 2845.3 | kJ/kg | |||
H3 | 697 | kJ/kg | ||||||
Now, plug these values into Eqn 6 to obtain : | mdot1 / mdot,2 = | 4.062 | ||||||
Verify : | None of the assumptions made in this problem solution can be verified. | |||||||
Answers : | mdot1 / mdot,2 = | 4.06 |