Introduction to Chemical Engineering Thermodynamics
Introduction to Chemical Engineering Thermodynamics
8th Edition
ISBN: 9781259696527
Author: J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
Publisher: McGraw-Hill Education
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Chapter 7, Problem 7.32P
Interpretation Introduction

Interpretation

For the given conditions i.e. adiabatic ideal gas, the discharge stream temperature and power required of the compressor is to be found out for any one of the set of operating conditions ( in this case (a)).

Concept Introduction:

Assume ideal gas for given conditions, ΔS=0

  ΔSR=T0TCPRdTTln(PP0)

  T0TCPRdTT=A.lnτ+[BT0+(CT02+Dτ2T02)(τ+1τ)](τ1)

ΔH=T1T2CPdT

T0TCPRdT=A.T0(τ1)+B2T02(τ21)+C3T03(τ31)+DT0(τ1τ)

Consider operating conditions (a)

W=(m.ΔH)

τ=TT0

ΔH=ΔHη

Where,

ΔS = Change in Entropy

Cp = Molar heat capacity

R = Universal Gas Constant

T0= Initial given temperature = 25oC = 298.15K

P0 = Initial given Pressure = 101.33 kPa

P2 = Final Given Pressure = 375 kPa

n = Given Molar flow rate = 100 mol / s

η = Given efficiency = 0.75

A, B, C, D = Constants for heat capacity of air

A = 3.355

B = 0.575 x 10-3 K-1

C = 0

D = -0.016 x 105K2ΔH = Actual Change in Enthalpy

ΔH = Ideal Change in Enthalpy

W = Power required of the compressor

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