INTRO.TO CHEM.ENGR.THERMO.-EBOOK>I<
INTRO.TO CHEM.ENGR.THERMO.-EBOOK>I<
8th Edition
ISBN: 9781260940961
Author: SMITH
Publisher: INTER MCG
Question
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Chapter 3, Problem 3.32P

(a)

Interpretation Introduction

Interpretation:

The values of Q, W, ΔU and ΔH should be deduced for 1 mole of an ideal gas at 30C0 and 1 bar which is first heated at constant volume and isothermally compressed to a final state at 130C0 and 10 bar.

Concept Introduction:

  • Isothermal process proceeds with no change in temperature i.e. ΔT = 0
  • Isobaric process proceeds with no change in pressure i.e. ΔP = 0
  • Isochoric process proceeds with no change in volume i.e. ΔV = 0
  • Isobaric process with no exchange of heat i.e. Q = 0
  • Based on the first law of thermodynamics
  • ΔU = Q + W ------(1)where:ΔU = change in internal energyQ = heat involvedW = work done

  • For an isochoric process
  • ΔU = CvΔT ------(2)where:ΔT = change in temperatureCv = specific heat capacity at constant volume

  • For an isobaric process:
  • ΔH = CpΔT ------(3)where:ΔH = change in temperatureCp = specific heat capacity at constant pressure

  • The ratio of specific heats is given as:γ = CpCv ---------(4)

(b)

Interpretation Introduction

Interpretation:

The values of Q, W, ΔU and ΔH should be deduced for 1 mole of an ideal gas at 30C0 and 1 bar which is first heated at constant pressure and isothermally compressed to a final state at 130C0 and 10 bar.

Concept Introduction:

  • Isothermal process proceeds with no change in temperature i.e. ΔT = 0
  • Isobaric process proceeds with no change in pressure i.e. ΔP = 0
  • Isochoric process proceeds with no change in volume i.e. ΔV = 0
  • Isobaric process with no exchange of heat i.e. Q = 0

(c)

Interpretation Introduction

Interpretation:

The values of Q, W, ΔU and ΔH should be deduced for 1 mole of an ideal gas at 30C0 and 1 bar which is first isothermally compressed and then heated at constant pressure to a final state at 130C0 and 10 bar.

Concept Introduction:

  • Isothermal process proceeds with no change in temperature i.e. ΔT = 0
  • Isobaric process proceeds with no change in pressure i.e. ΔP = 0
  • Isochoric process proceeds with no change in volume i.e. ΔV = 0
  • Isobaric process with no exchange of heat i.e. Q = 0

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Chapter 3 Solutions

INTRO.TO CHEM.ENGR.THERMO.-EBOOK>I<

Ch. 3 - Prob. 3.11PCh. 3 - Prob. 3.12PCh. 3 - Prob. 3.13PCh. 3 - Prob. 3.14PCh. 3 - Prob. 3.15PCh. 3 - Prob. 3.16PCh. 3 - Prob. 3.17PCh. 3 - Prob. 3.18PCh. 3 - Prob. 3.19PCh. 3 - Prob. 3.20PCh. 3 - Prob. 3.21PCh. 3 - Prob. 3.22PCh. 3 - Prob. 3.23PCh. 3 - Prob. 3.24PCh. 3 - Prob. 3.25PCh. 3 - Prob. 3.26PCh. 3 - Prob. 3.27PCh. 3 - Prob. 3.28PCh. 3 - Prob. 3.29PCh. 3 - Prob. 3.30PCh. 3 - Prob. 3.31PCh. 3 - Prob. 3.32PCh. 3 - Prob. 3.33PCh. 3 - Prob. 3.34PCh. 3 - Prob. 3.35PCh. 3 - Prob. 3.36PCh. 3 - Prob. 3.37PCh. 3 - Prob. 3.38PCh. 3 - Prob. 3.39PCh. 3 - Prob. 3.40PCh. 3 - Prob. 3.41PCh. 3 - Prob. 3.42PCh. 3 - Prob. 3.43PCh. 3 - Prob. 3.44PCh. 3 - Prob. 3.45PCh. 3 - Prob. 3.46PCh. 3 - Prob. 3.47PCh. 3 - Prob. 3.48PCh. 3 - Prob. 3.49PCh. 3 - Prob. 3.50PCh. 3 - Prob. 3.51PCh. 3 - Prob. 3.52PCh. 3 - Prob. 3.53PCh. 3 - Prob. 3.54PCh. 3 - Prob. 3.55PCh. 3 - Prob. 3.56PCh. 3 - Prob. 3.57PCh. 3 - Prob. 3.58PCh. 3 - Prob. 3.59PCh. 3 - Prob. 3.60PCh. 3 - Prob. 3.61PCh. 3 - Prob. 3.62PCh. 3 - Prob. 3.63PCh. 3 - Prob. 3.64PCh. 3 - Prob. 3.65PCh. 3 - Prob. 3.66PCh. 3 - Prob. 3.67PCh. 3 - Prob. 3.68PCh. 3 - Prob. 3.69PCh. 3 - Prob. 3.70PCh. 3 - Prob. 3.71PCh. 3 - Prob. 3.72PCh. 3 - Prob. 3.73PCh. 3 - Prob. 3.74PCh. 3 - Prob. 3.75PCh. 3 - Prob. 3.76PCh. 3 - Prob. 3.77PCh. 3 - Prob. 3.78PCh. 3 - Prob. 3.79PCh. 3 - Prob. 3.80PCh. 3 - Prob. 3.81PCh. 3 - Prob. 3.82PCh. 3 - Prob. 3.83PCh. 3 - Prob. 3.84PCh. 3 - Prob. 3.85PCh. 3 - Prob. 3.86PCh. 3 - Prob. 3.87PCh. 3 - Prob. 3.88PCh. 3 - Prob. 3.89PCh. 3 - Prob. 3.90PCh. 3 - Prob. 3.91PCh. 3 - Prob. 3.92PCh. 3 - Prob. 3.93PCh. 3 - Prob. 3.94PCh. 3 - Prob. 3.95P
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