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Appendix N Homework The Fth Edition Was Moreover General Revision
APPENDIX— EVOLUTION OF A TEXTBOOK Introduction to Chemical Engineering Thermodynamics HENDRICK C. VAN NESS Rensselaer Polytechnic Institute •Troy, NY Rarely does a textbook remain in print for anything ap- proaching 55 years. Introduction to Chemical Engineering Thermodynamics is the only […]
Chapter 1 Homework The Obvious Advantage Coal That Cheap Used
1.7 Pabs ρg⋅h⋅Patm += ρ13.535 gm cm3 ⋅:= g 9.832 m s2 ⋅:= h 56.38cm:= Patm 101.78kPa:= Pabs ρg⋅h⋅Patm +:= Pabs 176.808kPa=Ans. 1.8 ρ13.535 gm cm3 ⋅:= g 32.243 ft s2 ⋅:= h 25.62in:= Patm 29.86in_Hg:= Pabs ρg⋅h⋅Patm +:= Pabs […]
Chapter 1 Homework User defined units for Smith, Van Ness
MCPH T0 T,A,B,C,D,()AH 2T0 T,B,()+H3T0 T,C,()+H4T0 T,D,()+ () ≡ Enthalpy H4T0 T,D,() D τT0 T,() T0 K ⎛ ⎜ ⎝ ⎞ ⎠ 2 ⋅ ≡ H3T0 T,C,() C 3 T0 K ⎛ ⎜ ⎝ ⎞ ⎠ 2 ⋅τT0 T,() 2τT0 […]
Chapter 10 Homework Each part of this problem is exactly like
y10.33:= T 100 degC⋅:= Guess: x10.33:= P 100 kPa⋅:= Given x1Psat1T()⋅1x 1 − () Psat2T()⋅+ P= (c) Given: x10.33:= P 120 kPa⋅:= Guess: y10.5:= T 100 degC⋅:= Given x1Psat1T()⋅1x 1 − () Psat2T()⋅+ P= x1Psat1T()⋅y1P⋅= y1 T ⎛ ⎜ ⎝ […]
Chapter 10 Homework Proprietary Material only Teachers And Educators For Course
b)For water as solvent: Ms18.015 gm mol := 10.36 Acetone: Psat1T() e 14.3145 2756.22 T degC 228.060+ − kPa⋅:= Acetonitrile Psat2T() e 14.8950 3413.10 T degC 250.523+ − kPa⋅:= a) Find BUBL P and DEW P values T 50degC:= x10.5:= […]
Chapter 11 Homework By definition of the excess properties
To find the maximum, set dVE/dx1 = 0 and solve for x1. Then use x1 to find VEmax. (b) Vbar2 () Ex1 () 2ab−2b c−()⋅x1 ⋅+ 3c⋅x1 () 2 ⋅+ ⎡ ⎣ ⎤ ⎦ ⋅= Vbar1 () Ex2 () 2a2b⋅x1 […]
Chapter 11 Homework The last term is the entropy change of UNmixing
nAr 2.5 mol⋅:= TAr 130 273.15+()K⋅:= PAr 20 bar⋅:= TN2 348.15 K=TAr 403.15 K=i12..:= ntotal nN2 nAr +:= x1 nN2 ntotal := x2 nAr ntotal := x10.615=x20.385= Find T after mixing by energy balance: TTN2 TAr + 2 := (guess) […]
Chapter 12 Homework 1 second, during which the following are mixed
∆H11.509 kJ mol =∆H1104.8 kJ kg ⋅21.01 kJ kg ⋅− ⎛ ⎜ ⎝ ⎞ ⎠18.015⋅gm mol ⋅:= H2O @ 5 C —–> H2O @ 25 C (1) LiCl(3 H2O) —–> LiCl + 3 H2O (2) LiCl + 4 H2O —–> […]
Chapter 12 Homework can be found in Section Bof this manual
∆H298 411153−285830−425609−92307−()−[]J⋅:= ∆H298 1.791−105 ×J= NaOH(s) + HCl(g) —> NaCl(s) + H2O(l) (1) NaOH(inf H2O) —> NaOH(s) + inf H2O (2) HCl(9 H2O) —> HCl(g) + 9 H2O(l) (3) NaCl(s) + inf H2O —> NaCl(inf H2O) (4) —————————————————————————————- NaOH(inf H2O) […]
Chapter 12 Homework Heat M1 moles of water from 10 C to 25 C2
Λ21 T() V1 V2 exp a21− RT⋅ ⎛ ⎜ ⎝ ⎞ ⎠ ⋅:=Λ12 T() V2 V1 exp a12− RT⋅ ⎛ ⎜ ⎝ ⎞ ⎠ ⋅:= a21 1351.90 cal mol ⋅:=a12 775.48 cal mol ⋅:= V2 18.07 cm3 mol ⋅:=V1 75.14 […]
Chapter 12 Homework Minimize the sum of the squared errors using the
P-x,y Diagram from Margules Equation fit to GE/RT data. 0 0.2 0.4 0.6 0.8 36 38 P-x data P-y data P-x calculated P-y calculated Pi kPa x1iy1i ,X1j ,y1calcj , (d) Consistency Test: δGERTiGeRT x1ix2i , () GERTi −:= δlnγ1γ2iln […]
Chapter 12 Homework Parameters for the Wilson equation
Calculate EXPERIMENTAL values of activity coefficients and excess Gibbs energy. Psat219.953 kPa⋅:=Psat184.562 kPa⋅:= Vapor Pressures from equilibrium data: y21y 1 − () → ⎯ ⎯ ⎯ :=x21x 1 − () → ⎯ ⎯ ⎯ := Calculate x2 and y2: i1n..:=n10=n […]
Chapter 12 Homework Plot Pxy diagram with fit and data γ1x1x2
γ1x1x2,() exp x2 Λ12 x1 x2 Λ12 ⋅+ Λ21 x2 x1 Λ21 ⋅+ − ⎛ ⎜ ⎝ ⎞ ⎠ ⋅ ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ x1 x2 Λ12 ⋅+ () := γ2x1x2,() exp x1−Λ12 x1 x2 Λ12 ⋅+ x2 […]
Chapter 13 Homework Basis is 1 mol species 1 + x mol steam
0.2 0.3 0.4 0.5 0.6 2.086 2.084 Gε () 105 2.082 ε ε0.3 0.31,0.6..:= εe0.45308=εeFind εe () := εe Gεe () d d 0J mol ⋅=Given εe0.5:= Guess: Gε () 1ε− 2 ⎛ ⎜ ⎝ ⎞ ⎠395790−()⋅J mol ⋅ε 2192420−200240−()⋅J […]
Chapter 13 Homework If the pure CO2 is assumed an ideal gas at 1(atm)
For CH3OH(3): Tc3 512.6kelvin:= Pc3 80.97bar:= ω30.564:= By Eq. (11.67) and data from Tables E.15 & E.16. φ30.6206 0.9763ω3 ⋅:= φ30.612= For H2(2), the reduced temperature is so large that it may be assumed ideal: φ = 1. Therefore: i13..:= […]
Chapter 13 Homework where the CO2 mole fraction approaches zero
K20.5798=K2exp ∆G− RT⋅ ⎛ ⎜ ⎝ ⎞ ⎠ :=∆G 5.892 103 ×J mol = ∆G∆H298 T T0 ∆H298 ∆G298 − () ⋅− R IDCPH T0T,∆A,∆B,∆C,∆D, () ⋅+ … R−T⋅IDCPS T0T,∆A,∆B,∆C,∆D, () ⋅+ … := ∆D 1.164−105 ⋅:=∆C 0.0:=∆B 0.540−10 3− […]
Chapter 14 Homework Apply mole balances around the process as well as an
Find the conditions for VLLE: Guess: Pstar P1sat:= y1star 0.5:= Given Pstar x1βγ1×1β () ⋅P1sat⋅1×1α− () γ2×1α () ⋅P2sat⋅+= y1star Pstar⋅x1αγ1×1α () ⋅P1sat⋅= Pstar y1star ⎛ ⎜ ⎝ ⎞ ⎠Find Pstar y1star,():= Pstar 160.699=y1star 0.405= Calculate VLE in two-phase region. […]
Chapter 14 Homework The most satisfactory procedure for reduction of this set
δ12 2B 12 ⋅B11 −B22 −:= B12 52 cm3 mol ⋅:=B22 1523−cm3 mol ⋅:=B11 963−cm3 mol ⋅:= BUBL P calculations with virial coefficients:(b) y1x1 () 0.808=Pbubl x1 () 85.701 kPa=x10.75:= y1x1 () 0.731=Pbubl x1 () 80.357 kPa=x10.50:= y1x1 () 0.562=Pbubl […]
Chapter 14 Homework To solve for another temperature, simply change
0 0.5 1 0 0.05 A21 x1⋅A12 1×1−()⋅+ ⎡ ⎣ ⎤ ⎦ x1⋅1×1−()⋅ 0.1 GERTi x1ix1, x1 0 0.01,1..:=RMS 9.187 10 4− ×= RMS 1 n i GERTiA21 x1i ⋅A12 x2i ⋅+ () x1i ⋅x2i ⋅− ⎡ ⎣ ⎤ ⎦ […]
Chapter 15 Homework Compression to a pressure at which condensation in coils occurs
QdotC 600 500 400 300 200 ⎛ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ ⎞ ⎟ ⎟ ⎟ ⎠ −BTU sec ⋅:=tC 40 30 20 10 0 ⎛ ⎜ ⎜ ⎜ ⎜ ⎜ ⎝ ⎞ ⎟ ⎟ ⎟ ⎠ := The […]
Chapter 15 Homework The only irreversibility is the transfer of heat from
Chapter 15 – Section A – Mathcad Solutions 15.1 Initial state: Liquid water at 70 degF. H138.05 BTU lbm ⋅:= S10.0745 BTU lbmrankine⋅ ⋅:= (Table F.3) Final state: Ice at 32 degF. H20.02−143.3−() BTU lbm ⋅:= S20.0 143.3 491.67 − […]
Chapter 16 Homework If you are a student using this Manual, you are using it without permission
b) For Krypton: M mol NA := Sig R ln 2π⋅ M⋅k⋅T⋅ h2 ⎛ ⎜ ⎝ ⎞ ⎠ 3 2Ve 5 2 ⋅ NA ⋅ ⎡ ⎢ ⎢ ⎢ ⎣ ⎤ ⎥ ⎥ ⎥ ⎦ ⋅:= Sig 164.08 J mol […]
Chapter 2 Homework Symbol V is used for total volume in this problem
(d) For the restoration process, the change in internal energy is equal but of opposite sign to that of the initial process. Thus Q∆Utotal −:= Q 1.715−kJ=Ans.Ans. (e) In all cases the total internal energy change of the universe is […]
Chapter 3 Homework A value is required for PV/T
a bit of algebra leads to 3.5 κabP⋅+=a 3.9 10 6− ⋅atm 1− ⋅:= b 0.1−10 9− ⋅atm 2− ⋅:= P11 atm⋅:= P23000 atm⋅:= V1ft 3 ⋅:= (assume const.) Combine Eqs. (1.3) and (3.3) for const. T: Work V P1 […]
Chapter 3 Homework The intersection of these two relations can be found by one means
Table 3.1 αTrω, () 1 0.480 1.574ω+ 0.176ω2 − () 1T r 2 − ⎛ ⎜ ⎝ ⎞ ⎠ ⋅+ ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ := qT r () Ψα Trω, () ⋅ ΩTr ⋅ := Eq. (3.54) βTrPr […]
Chapter 3 Homework Limited distribution permitted Below is a plot of
Pr1 P1 Pc := Tr2 T2 Tc := Pr2 P2 Pc := Tr1 0.62=Pr1 0.03=Tr2 0.88=Pr2 3.561= From Fig. (3.16): ρr1 2.69:= ρr2 2.27:= 3.54 For ethanol: Tc513.9 K⋅:= T 453.15 K⋅:= Tr T Tc := Tr0.882= Pc61.48 bar⋅:= P […]
Chapter 4 Homework Our procedure is therefore to take 5 points
PROPRIETARY MATERIAL only to teachers and educators for course preparation. If you are a student using this Manual, you are using it without permission. . © 2005 The McGraw-Hill Companies, Inc. All rights reserved. Limited distribution permitted Ans. 4.2 (a) […]
Chapter 4 Homework The calculations are repeated and the answers are in
nCO2∆H1148a ⋅nO2∆H1148b ⋅+ 0= The combined heats of reaction must be zero: ∆H1148b 2.249−105 ×J mol = ∆H1148b ∆H298b R MCPH 298.15K 1148.15K,∆A,∆B,∆C,∆D, () ⋅1148.15K 298.15K−()⋅+ …:= ∆D 1.899 105 ×=∆C0:=∆B 9.34−10 4− ×=∆A 0.429−= ∆D i niDi ⋅ () […]
Chapter 4 Homework The Energy Balance Isthen Written H773 H298
n39.781=n32.6 79 21 ⋅:= n22.6=n22 1.3⋅:= n11:= Moles methane Moles oxygen Moles nitrogen Entering: FURNACE: Basis is 1 mole of methane burned with 30% excess air. CH4 + 2O2 = CO2 + 2H2O(g) 4.29 This value is for the constant-V […]
Chapter 5 Homework Since ηactual>ηmax, the process is impossible
5.34 E 110 volt⋅:= i 9.7 amp⋅:= Tσ300 K⋅:= Wdotmech 1.25−hp⋅:= Wdotelect iE⋅:= Wdotelect 1.067 103 ×W= At steady state: Qdot Wdotelect +Wdotmech + t Ut d d =0= Qdot TσSdotG + t St d d =0= Qdot Wdotelect −Wdotmech […]
Chapter 5 Homework The Following Equations are Used Derive And Expression
5.4 (a) TC303.15 K⋅:= TH623.15 K⋅:= ηCarnot 1TC TH −:= η 0.55 ηCarnot ⋅:= η 0.282=Ans. Chapter 5 – Section A – Mathcad Solutions 5.2 Let the symbols Q and Work represent rates in kJ/s. Then by Eq. (5.8) ηWork […]
Chapter 6 Homework For the wet vapor the entropy is given by
(c) Tc647.1 K⋅:= Pc220.55 bar⋅:= ω 0.345:= Tr1 T1 Tc := Pr1 P1 Pc := Tr2 T2 Tc := Pr2 P2 Pc := Tr1 1.11752=Pr1 0.13602=Tr2 0.63846=Pr2 0.01066= The generalized virial-coefficient correlation is suitable here ∆H∆Hig RT c ⋅HRB Tr2 […]
Chapter 6 Homework neglecting kinetic and potential energies and setting the
The process is the same as that of Example 6.8, except that the stream flows out rather than in. The energy balance is the same, except for a sign: m1257.832 kg=V17.757 10 3− ×m3 kg = m1 Vtank V1 :=V1Vliq […]
Chapter 6 Homework Property changes by equations for an ideal gas
A 1.637:= B22.706 10 3− ⋅ K := C6.915−10 6− ⋅ K2 := Solve energy balance for final T. See Eq. (4.7). τ1:= (guess) Given HRRAT⋅τ1− () ⋅B 2T2 ⋅τ 21− () ⋅+ ⎡ ⎢ ⎣ ⎤ ⎥ ⎦ C […]
Chapter 6 Homework The pressure is the vapor pressure given by the
6.8 Isobutane: Tc408.1 K⋅:= Zc0.282:= CP2.78 J gm K⋅ ⋅:= P14000 kPa⋅:= P22000 kPa⋅:= molwt 58.123 gm mol ⋅:= Vc262.7 cm3 mol ⋅:= Eq. (3.63) for volume of a saturated liquid may be used for the volume of a compressed […]
Chapter 7 Homework Interpolations in Table F.2 at several pressures and
Interpolation in Table F.2 at P = 525 kPa and S = 7.1595 kJ/(kg*K) yields: H22855.2 kJ kg ⋅:= V2531.21 cm3 gm ⋅:= mdot 0.75 kg sec ⋅:= With the heat, work, and potential-energy terms set equal to zero and […]
Chapter 7 Homework liquid and sat. vapor at the turbine exhaust
These are sufficiently close, and we conclude that: xS0.925=xH0.924= The trial values given produce: xS 6.7093 Sl− Sv Sl− :=xH Hv 801.7−.75 Hl⋅− .75 Hv Hl−()⋅ := The two equations for x are: Sv 7.1293:=Sl 1.5276:= Hv 2706.0:=Hl 503.7:= If […]
Chapter 7 Homework Table B2at Cestimate The Heat Vaporization Tsat
(guess) τ1.1:= The actual final temperature is now found from Eq. (6.91) combined with E q (4.7), written: The actual enthalpy change from Eq. (7.17): ∆H’ 1158.8 J mol = ∆H’ ∆Hig RT c ⋅HRB TrPr ,ω, () HRB Tr0 […]
Chapter 8 Homework For Saturated Vapor 30715 Was Found Problem
t8t95+:=t9 190 t7 − 2t7 +:=t7tsat ∆T67 K +:= CP 272.0 230.2− 10 kJ kg K⋅ ⋅:=β 1 Vliq 1.023 1.012− 20 ⎛ ⎜ ⎝ ⎞ ⎠ ⋅cm3 gm K⋅ ⋅:= We apply Eq. (7.25) for the calculation of the […]
Chapter 8 Homework The following vectors contain values for Parts
For isentropic expansion, S’3S2 := x’3 S’3Sliq − ∆Slv := x’30.855= Chapter 8 – Section A – Mathcad Solutions 8.1 With reference to Fig. 8.1, SI units, At point 2: Table F.2, H23531.5:= S26.9636:= At point 4: Table F.1, H4209.3:= […]
Chapter 9 Homework For isentropic compression, from Point 2 to Point 3
(b) Steps 3–2 and 1–4 (Fi g . 8.2) are isentropic, for which S3=S2 and S1=S4 . Thus by Eq. 6.82): x3 S2 Sliq− Svap Sliq− := x3 0.971=x4 S1 Sliq− Svap Sliq− := x4 0.302= (c) Heat addition, Step […]