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Introduction to
Chemical Engineering
Thermodynamics

Chapter 7
KFUPM Housam Binous CHE 303

1
Throttling Process
Fluid flows through a restriction results in a pressure drop
No change in kinetic or potential energy
No shaft work produced and no heat transfer

∆H=0
For an ideal gas: no change in T occurs
For real gases: T reduction results from a throttling process

KFUPM Housam Binous CHE 303

2
KFUPM Housam Binous CHE 303

3
KFUPM Housam Binous CHE 303

4
Turbines (Expanders)
Expansion of a gas in a nozzle to produce a high-velocity stream
This kinetic energy is converted into shaft work when the stream
impinges on blades attached to a rotating shaft
Overall result is conversion of internal energy of a high-pressure
stream into shaft work
Steam : device is called a turbine
High-pressure gas (e.g., ethylene) device called expander
KFUPM Housam Binous CHE 303

5
KFUPM Housam Binous CHE 303

6
Neglect potential energy, heat transfer is negligible, inlet and
outlet are sized so that fluid velocities are roughly equal

T1, P1 and P2 are known but ignore T2, Ws and H2
Reversible isentropic turbine (constant entropy)

S2=S1.

Thus, one can determine H2 and then Ws.

KFUPM Housam Binous CHE 303

7
KFUPM Housam Binous CHE 303

8
Compressors
Rotating blades (not too high discharge pressure) or
cylinders with reciprocating pistons (for high pressures)
Kinetic and potential energy changes negligible.
Adiabatic compression

KFUPM Housam Binous CHE 303

9
KFUPM Housam Binous CHE 303

10
KFUPM Housam Binous CHE 303

11
Pumps

Need to determine enthalpy of compressed subcooled liquids

KFUPM Housam Binous CHE 303

12
Other useful relations:

Both equations are usually integrated assuming that:
CP, β and V are constant

KFUPM Housam Binous CHE 303

13

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Ch7

  • 2. Throttling Process Fluid flows through a restriction results in a pressure drop No change in kinetic or potential energy No shaft work produced and no heat transfer ∆H=0 For an ideal gas: no change in T occurs For real gases: T reduction results from a throttling process KFUPM Housam Binous CHE 303 2
  • 5. Turbines (Expanders) Expansion of a gas in a nozzle to produce a high-velocity stream This kinetic energy is converted into shaft work when the stream impinges on blades attached to a rotating shaft Overall result is conversion of internal energy of a high-pressure stream into shaft work Steam : device is called a turbine High-pressure gas (e.g., ethylene) device called expander KFUPM Housam Binous CHE 303 5
  • 7. Neglect potential energy, heat transfer is negligible, inlet and outlet are sized so that fluid velocities are roughly equal T1, P1 and P2 are known but ignore T2, Ws and H2 Reversible isentropic turbine (constant entropy) S2=S1. Thus, one can determine H2 and then Ws. KFUPM Housam Binous CHE 303 7
  • 9. Compressors Rotating blades (not too high discharge pressure) or cylinders with reciprocating pistons (for high pressures) Kinetic and potential energy changes negligible. Adiabatic compression KFUPM Housam Binous CHE 303 9
  • 10. KFUPM Housam Binous CHE 303 10
  • 11. KFUPM Housam Binous CHE 303 11
  • 12. Pumps Need to determine enthalpy of compressed subcooled liquids KFUPM Housam Binous CHE 303 12
  • 13. Other useful relations: Both equations are usually integrated assuming that: CP, β and V are constant KFUPM Housam Binous CHE 303 13