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 6, Problem 6.21P
Interpretation Introduction

Interpretation:

The enthalpy and entropy of a liquid-vapor equilibrium mixture at a temperature of 350F0 should be deduced.

Concept Introduction:

  • For a two-phase liquid-vapor equilibrium mixture the specific volume (V), enthalpy (H) and entropy (S) are given as:
  •   H = Hf + x(Hg-Hf)-----(1)S = Sf + x(Sg-Sf)--------(2)where, Hg and Hf are the specific enthalpies in the vapor and liquid phases respectivelySg and Sf are the specific entropies in the vapor and liquid phases respectivelyx = steam quality = mass of vapormass of vapor + mass of liquid ----(3)

Enthalpy, H = 788.7 kJ/kg

Entropy, S = 2.196 kJ/kg-K

Given:

Total mass, M = 3.0 lbm

Equilibrium temperature = 350F0

Explanation:

Based on the steam tables at temperature = 350F0 we have:

Specific volume of liquid, vf = 0.01799 ft3/lbm

Specific volume of vapor, vg = 3.3426 ft3/lbm

Specific enthalpy of liquid, Hf = 321.73 Btu/lbm

Specific enthalpy of vapor, Hg = 1192.7 Btu/lbm

Specific entropy of liquid, Sf = 0.50322 Btu/lbm-R

Specific entropy of liquid, Sg = 5.7450 Btu/lbm-R

Calculation:

Step 1:

Calculate the steam quality x using equation (3)

It is given that in the volumes of the vapor is 50 times the volume of liquid. The total volume, Vt is:-

   V t  = V liq  + V vap

   V t  = m liq ×v f  + m vap ×v g  ------(4)

   where, m liq  and m vap  are mass of the liquid and vapor phases

   v f  and v g  are the specific volumes of the liquid and vapor

   Since,  V vap  = 50 V liq

   we can write, V t  = 51V liq  -----(5)

   by extension, V t  = 51(m liq ×v f ) ------(6)

   Substituting for V t  in equation (4) we get:

   51(m liq ×v f ) = m liq ×v f  + m vap ×v g

   50(m liq ×v f ) = m vap ×v g

   m vap ×v g m liq ×v f  = 50

   m vap m liq  = 50× v f v g  

   Substituting the values for v f  and v g ,

   m vap m liq  = 50× 0.01799 3.3426  =0.269 -------(7)

   Now, the total mass m = 3.0 lbm , i.e.

   m vap + m liq =3

   Based on equation 3, we can then write,

   3x = m vap   and 3(1-x) = m liq

   Substituting for m liq  and m vap  in eq(7) we get:

   x 1-x  = 0.269

   x = 0.212

Step 2:

Calculate H and S based on equations 1 and 2

  H = Hf + x (Hg-Hf)    = 321.73 + 0.212(1192.7-321.73) = 506.38 Btu/lbm

  S = Sf + x (Sg-Sf)   = 0.50322 + 0.212(1.5789-0.50322) = 0.731 Btu/lbm-R

Thus the total enthalpy and entropy values are:

Enthalpy, H = 506.38 Btu/lbm

Entropy, S = 0.731 Btu/lbm-R

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Chapter 6 Solutions

Introduction to Chemical Engineering Thermodynamics

Ch. 6 - Prob. 6.11PCh. 6 - Prob. 6.12PCh. 6 - Prob. 6.13PCh. 6 - Prob. 6.14PCh. 6 - Prob. 6.15PCh. 6 - Prob. 6.16PCh. 6 - Prob. 6.17PCh. 6 - Prob. 6.18PCh. 6 - Prob. 6.19PCh. 6 - Prob. 6.20PCh. 6 - Prob. 6.21PCh. 6 - Prob. 6.22PCh. 6 - Prob. 6.23PCh. 6 - Prob. 6.24PCh. 6 - Prob. 6.25PCh. 6 - Prob. 6.26PCh. 6 - Prob. 6.27PCh. 6 - What is the mole fraction of water vapor in air...Ch. 6 - Prob. 6.29PCh. 6 - Prob. 6.30PCh. 6 - Prob. 6.31PCh. 6 - Prob. 6.32PCh. 6 - Prob. 6.33PCh. 6 - Prob. 6.34PCh. 6 - Prob. 6.35PCh. 6 - Prob. 6.36PCh. 6 - Prob. 6.37PCh. 6 - Prob. 6.38PCh. 6 - Prob. 6.39PCh. 6 - Prob. 6.40PCh. 6 - Prob. 6.41PCh. 6 - Prob. 6.42PCh. 6 - Prob. 6.43PCh. 6 - Prob. 6.44PCh. 6 - Prob. 6.45PCh. 6 - Prob. 6.46PCh. 6 - Prob. 6.47PCh. 6 - Prob. 6.48PCh. 6 - Prob. 6.49PCh. 6 - Prob. 6.50PCh. 6 - Prob. 6.51PCh. 6 - Prob. 6.52PCh. 6 - Prob. 6.53PCh. 6 - Prob. 6.54PCh. 6 - Prob. 6.55PCh. 6 - Prob. 6.56PCh. 6 - Prob. 6.57PCh. 6 - Prob. 6.58PCh. 6 - Prob. 6.59PCh. 6 - Prob. 6.60PCh. 6 - Prob. 6.61PCh. 6 - Prob. 6.62PCh. 6 - Prob. 6.63PCh. 6 - Prob. 6.64PCh. 6 - Prob. 6.65PCh. 6 - Prob. 6.66PCh. 6 - Prob. 6.67PCh. 6 - Prob. 6.68PCh. 6 - Prob. 6.69PCh. 6 - Prob. 6.71PCh. 6 - Prob. 6.72PCh. 6 - Prob. 6.73PCh. 6 - Prob. 6.74PCh. 6 - Prob. 6.75PCh. 6 - Prob. 6.76PCh. 6 - Prob. 6.77PCh. 6 - Prob. 6.78PCh. 6 - Prob. 6.79PCh. 6 - Prob. 6.80PCh. 6 - Prob. 6.81PCh. 6 - The temperature dependence of the second virial...Ch. 6 - Prob. 6.83PCh. 6 - Prob. 6.84PCh. 6 - Prob. 6.85PCh. 6 - Prob. 6.86PCh. 6 - Prob. 6.87PCh. 6 - Prob. 6.88PCh. 6 - Prob. 6.89PCh. 6 - Prob. 6.90PCh. 6 - Prob. 6.91PCh. 6 - Prob. 6.92PCh. 6 - Prob. 6.93PCh. 6 - Prob. 6.94PCh. 6 - Prob. 6.95PCh. 6 - Prob. 6.96PCh. 6 - Prob. 6.97PCh. 6 - Prob. 6.98PCh. 6 - Prob. 6.99PCh. 6 - Prob. 6.100P
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