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Energy Balance on Open SystemOpen System is one in which there is Mass Flow
across its Boundaries
Types of Work
= Shaft Work + Flow Work
Shaft Work= Work Done by Process Fluid Moving Part within System
Flow Work = Work Done by Fluid at System Outlet – Work Done on Fluid at System Inlet
System(inlet Mass Flow Rate)
(inle
t Specific Internal Energy )
uin (inlet Velocity)
Zin (inlet elevation)
(Inlet Specific Volume)
Pin (Inlet Pressure)
(outlet Mass Flow Rate)
(outlet Specific Internal Energy)
uout (outlet Velocity)
Zout (outlet elevation)
(Outlet Specific Volume)
Pout(Outlet Pressure)
Illustration of Flow Work = PV Work
Dimensional Analysis
Flow Work is a State Function
Form of Energy Equation for Open System
Pipe
State Properties of Steam
(Table B.6)Prop. Of Saturated Steam
P T (Liq.Water)(Bars) (oC) M3/Kg M3/Kg KJoules/Kg KJoules/Kg
0.00611 0.01 0.001 206.2 Zero 2375.6
0.10 45.8 0.00101 14.67 191.8 2438.0
0.50 81.3 0.00103 3.24 340.5 2484.0
1.01325 100.0 0.001044 1.673 419.0 2506.5
Another State Function
Enthalpy = Internal Energy + Flow Work = A State Function
(Table B.6)Prop. Of Saturated Steam
P T(Bars) (oC) KJoules/Kg KJoules/Kg KJ/Kg KJ/Kg
0.00611 0.01 Zero 2375.6 +0.0 2501.6
0.10 45.8 191.8 2438.0 191.8 2584.8
0.50 81.3 340.5 2484.0 340.6 2646.0
1.01325 100.0 419.0 2506.5 419.1 2676.0
Heat of Vaporization
Internal Energy of Vaporization
Energy Balance for Open System with Multiple Feed & Product Streams
Energy Balance Equation
Simplification of First Law of Thermodynamics for Open System
Here All Terms are Rates of Energy &
Compare with First Law of ThermodynamicsFor Closed System
System
Here All Terms are Amounts of Energy &
Simplifications of Energy Balance for Open System
If Single Input & Single Output Stream
Simplifications:
If no Moving Parts in System
Shaft Work Rate = 0.0=
If System & Surroundings are at Same Temperature
Heat Transfer Rate = 0.0=
If Linear Velocities of All Streams are Equal
Neglect Kinetic Energy Term:
If all streams enter & leave process at the Same Height
Neglect Potential Energy Term:
If Specific Enthalpy is Same for All Streams& Because Mass is Conserved