Vapor product ny(mol) YB(mol C,H/mol) Liquid feed I mol (basis) T(°C) P(mm Hg) ZB(mol C,H,/mol) (1– 2g)(mol C,Hg/mol) 130°C Liquid product (mol) xg(mol C,H/mol) Heat The pressure in the unit may be adjusted to any desired value, and the heat input may similarly be adjusted to vary the temperature at which the separation is conducted. The vapor and liquid product streams both emerge at the temperature T(°C) and pressure P(mm Hg) maintained in the vessel. Assume that the vapor pressures of benzene and toluene are given by the Antoine equation, Table B.4 or APEX; that Raoult's law–Equation 6.4-1¬applies; and that the enthalpies of benzene and toluene liquid and vapor are linear functions of temperature. Specific enthalpies at two tempera- tures are given here for each substance in each phase. C,H6(1) (T = 0°C, Ĥ =0 kJ/mol) C6H6(v) (T = 80°C, Ĥ = 41.61 kJ/mol) (T = 120°C, Ĥ = 45.79 kJ/mol) C,Hg(1) (T = 0°C, Ĥ =0 kJ/mol) C;Hg(v) (T = 89°C, Ĥ = 49.18 kJ/mol) (T = 111°C, Ĥ = 52.05 kJ/mol) (T = 80°C, H = 10.85 kJ/mol) (T = 111°C, Ĥ = 18.58 kJ/mol) (a) Suppose the feed is equimolar in benzene and toluene (zB = 0.500). Take a basis of 1 mol of feed and do the degree-of-freedom analysis on the unit to show that if T and P are specified, you can calculate the molar compositions of each phase (xâ and yp), the moles of the liquid and vapor products (nį and ny), and the required heat input (Q). Don't do any numerical calculations in this part. (b) Do the calculations of Part (a) for T = 90°C and P = 652 mm Hg. (Suggestion: First derive an equation for xg that can be solved by trial and error from known values of T and P.) (c) For zB = 0.5 and T = 90°C, there is a range of feasible operating pressures for the evaporator, Pmin P< Pmax- If the evaporator pressure P fell outside this range, no separation of benzene and toluerte would be achieved. Why not? What would emerge from the unit if P < Pmin ? What would emerge if P > Pmax? [Hint: Look at your solution to Part (b) and think about how it would change if you lowered P.] y and Energy Balances (d) Set up a spreadsheet to perform the calculation of Part (b) and then use it to determine Pmax and Pmin. The spreadsheet should appear as follows (some solutions are shown): Problem 7.55-Flash vaporization of benzene and toluene

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7.55. A liquid mixture of benzene and toluene is to be separated in a continuous single-stage equilibrium
flash tank.
Vapor product
ny(mol)
YB(mol C,H/mol)
Liquid feed
I mol (basis)
T(°C)
P(mm Hg)
ZB (mol C,H/mol)
(1 – zg)(mol C,Hg/mol)
130°C
Liquid product
n (mol)
Xg(mol CgH/mol)
Heat
The pressure in the unit may be adjusted to any desired value, and the heat input may similarly be
adjusted to vary the temperature at which the separation is conducted. The vapor and liquid product
streams both emerge at the temperature T(°C) and pressure P(mm Hg) maintained in the vessel.
Assume that the vapor pressures of benzene and toluene are given by the Antoine equation,
Table B.4 or APEX; that Raoult's law–Equation 6.4-1¬applies; and that the enthalpies of benzene
and toluene liquid and vapor are linear functions of temperature. Specific enthalpies at two tempera-
tures are given here for each substance in each phase.
C,H6(1) (T = 0°C, Ĥ = 0 kJ/mol)
C,H6(v) (T = 80°C, Ĥ = 41.61 kJ/mol) (T = 120°C, Ĥ = 45.79 kJ/mol)
(T = 80°C, Ħ = 10.85 kJ/mol)
C,Hg(1)
(T = 0°C, Ĥ = 0 kJ/mol)
(T = 111°C, Ĥ = 18.58 kJ/mol)
C;Hg(v) (T = 89°C, Ĥ = 49.18 kJ/mol) (T = 111°C, Ĥ = 52.05 kJ/mol)
(a) Suppose the feed is equimolar in benzene and toluene (ZB = 0.500). Take a basis of 1 mol of feed
and do the degree-of-freedom analysis on the unit to show that if T and P are specified, you can
calculate the molar compositions of each phase (xB and yß), the moles of the liquid and vapor
products (nį and ny), and the required heat input (Q). Don’t do any numerical calculations in this
part.
(b) Do the calculations of Part (a) for T = 90°C and P = 652 mm Hg. (Suggestion: First derive an
equation for xB that can be solved by trial and error from known values of T and P.)
(c) For zB = 0.5 and T = 90°C, there is a range of feasible operating pressures for the evaporator,
P< Pmax- If the evaporator pressure P fell outside this range, no separation of benzene and
Pmin
toluerte would be achieved. Why not? What would emerge from the unit if P < Pmin? What would
emerge if P > Pmax? [Hint: Look at your solution to Part (b) and think about how it would change
if you lowered P.]
APTER 7 Energy and Energy Balances
(d) Set up a spreadsheet to perform the calculation of Part (b) and then use it to determine Pmax and
Pmin- The spreadsheet should appear as follows (some solutions are shown):
Problem 7.55-Flash vaporization of benzene and toluene
Transcribed Image Text:7.55. A liquid mixture of benzene and toluene is to be separated in a continuous single-stage equilibrium flash tank. Vapor product ny(mol) YB(mol C,H/mol) Liquid feed I mol (basis) T(°C) P(mm Hg) ZB (mol C,H/mol) (1 – zg)(mol C,Hg/mol) 130°C Liquid product n (mol) Xg(mol CgH/mol) Heat The pressure in the unit may be adjusted to any desired value, and the heat input may similarly be adjusted to vary the temperature at which the separation is conducted. The vapor and liquid product streams both emerge at the temperature T(°C) and pressure P(mm Hg) maintained in the vessel. Assume that the vapor pressures of benzene and toluene are given by the Antoine equation, Table B.4 or APEX; that Raoult's law–Equation 6.4-1¬applies; and that the enthalpies of benzene and toluene liquid and vapor are linear functions of temperature. Specific enthalpies at two tempera- tures are given here for each substance in each phase. C,H6(1) (T = 0°C, Ĥ = 0 kJ/mol) C,H6(v) (T = 80°C, Ĥ = 41.61 kJ/mol) (T = 120°C, Ĥ = 45.79 kJ/mol) (T = 80°C, Ħ = 10.85 kJ/mol) C,Hg(1) (T = 0°C, Ĥ = 0 kJ/mol) (T = 111°C, Ĥ = 18.58 kJ/mol) C;Hg(v) (T = 89°C, Ĥ = 49.18 kJ/mol) (T = 111°C, Ĥ = 52.05 kJ/mol) (a) Suppose the feed is equimolar in benzene and toluene (ZB = 0.500). Take a basis of 1 mol of feed and do the degree-of-freedom analysis on the unit to show that if T and P are specified, you can calculate the molar compositions of each phase (xB and yß), the moles of the liquid and vapor products (nį and ny), and the required heat input (Q). Don’t do any numerical calculations in this part. (b) Do the calculations of Part (a) for T = 90°C and P = 652 mm Hg. (Suggestion: First derive an equation for xB that can be solved by trial and error from known values of T and P.) (c) For zB = 0.5 and T = 90°C, there is a range of feasible operating pressures for the evaporator, P< Pmax- If the evaporator pressure P fell outside this range, no separation of benzene and Pmin toluerte would be achieved. Why not? What would emerge from the unit if P < Pmin? What would emerge if P > Pmax? [Hint: Look at your solution to Part (b) and think about how it would change if you lowered P.] APTER 7 Energy and Energy Balances (d) Set up a spreadsheet to perform the calculation of Part (b) and then use it to determine Pmax and Pmin- The spreadsheet should appear as follows (some solutions are shown): Problem 7.55-Flash vaporization of benzene and toluene
sucais vour emerge at uie temperature 1TC) and pIessure r(1IIIII ng) mamameu II Uie vesseI,
Assume that the vapor pressures of benzene and toluene are given by the Antoine equation,
Table B.4 or APEX; that Raoult's law-Equation 6.4-1-applies; and that the enthalpies of benzene
and toluene liquid and vapor are linear functions of temperature. Specific enthalpies at two tempera-
tures are given here for each substance in each phase.
C6H6(1) (T = 0°C, H = 0 kJ/mol)
C6H6(v) (T = 80°C, Ĥ = 41.61 kJ/mol) (T = 120°C, Ĥ = 45.79 kJ/mol)
(T = 80°C, H = 10.85 kJ/mol)
C,Hg(1)
(T = 0°C, Ĥ = 0 kJ/mol)
(T = 111°C, ÂĤ = 18.58 kJ/mol)
C,H3(v) (T = 89°C, Ĥ = 49.18 kJ/mol) (T = 111°C, Ĥ = 52.05 kJ/mol)
(a) Suppose the feed is equimolar in benzene and toluene (zB = 0.500). Take a basis of 1 mol of feed
and do the degree-of-freedom analysis on the unit to show that if T and P are specified, you can
calculate the molar compositions of each phase (xB and yg), the moles of the liquid and vapor
products (nį and ny), and the required heat input (Q). Don't do any numerical calculations in this
part.
(b) Do the calculations of Part (a) for T = 90°C and P = 652 mm Hg. (Suggestion: First derive an
equation for XB that can be solved by trial and error from known values of T and P.)
(c) For zB = 0.5 and T = 90°C, there is a range of feasible operating pressures for the evaporator,
Pmin < P< Pmax- If the evaporator pressure P fell outside this range, no separation of benzene and
toluene would be achieved. Why not? What would emerge from the unit if P < Pmin? What would
emerge if P > Pmax? [Hint: Look at your solution to Part (b) and think about how it would change
if you lowered P.]
7 Energy and Energy Balances
(d) Set up a spreadsheet to perform the calculation of Part (b) and then use it to determine Pmax and
Pmin. The spreadsheet should appear as follows (some solutions are shown):
Problem 7.55–Flash vaporization of benzene and toluene
zB
pB pT*
xB yB
nL
nV
0.500 90.0 652 1021
0.5543
8.144
0.500 90.0 | 714
-6,093
0.500 90.0
Additional columns may be used to store other calculated variables (e.g., specific enthalpies).
Briefly explain why Q is positive when P = 652 mm Hg and negative when P = 714 mm Hg.
(e) In successive rows, repeat the calculation for the same zg and T at several pressures between Pmin
and Pmax. Generate a plot (using the spreadsheet program itself, if possible) of ny versus P. At
approximately what pressure is half of the feed stream vaporized?
Transcribed Image Text:sucais vour emerge at uie temperature 1TC) and pIessure r(1IIIII ng) mamameu II Uie vesseI, Assume that the vapor pressures of benzene and toluene are given by the Antoine equation, Table B.4 or APEX; that Raoult's law-Equation 6.4-1-applies; and that the enthalpies of benzene and toluene liquid and vapor are linear functions of temperature. Specific enthalpies at two tempera- tures are given here for each substance in each phase. C6H6(1) (T = 0°C, H = 0 kJ/mol) C6H6(v) (T = 80°C, Ĥ = 41.61 kJ/mol) (T = 120°C, Ĥ = 45.79 kJ/mol) (T = 80°C, H = 10.85 kJ/mol) C,Hg(1) (T = 0°C, Ĥ = 0 kJ/mol) (T = 111°C, ÂĤ = 18.58 kJ/mol) C,H3(v) (T = 89°C, Ĥ = 49.18 kJ/mol) (T = 111°C, Ĥ = 52.05 kJ/mol) (a) Suppose the feed is equimolar in benzene and toluene (zB = 0.500). Take a basis of 1 mol of feed and do the degree-of-freedom analysis on the unit to show that if T and P are specified, you can calculate the molar compositions of each phase (xB and yg), the moles of the liquid and vapor products (nį and ny), and the required heat input (Q). Don't do any numerical calculations in this part. (b) Do the calculations of Part (a) for T = 90°C and P = 652 mm Hg. (Suggestion: First derive an equation for XB that can be solved by trial and error from known values of T and P.) (c) For zB = 0.5 and T = 90°C, there is a range of feasible operating pressures for the evaporator, Pmin < P< Pmax- If the evaporator pressure P fell outside this range, no separation of benzene and toluene would be achieved. Why not? What would emerge from the unit if P < Pmin? What would emerge if P > Pmax? [Hint: Look at your solution to Part (b) and think about how it would change if you lowered P.] 7 Energy and Energy Balances (d) Set up a spreadsheet to perform the calculation of Part (b) and then use it to determine Pmax and Pmin. The spreadsheet should appear as follows (some solutions are shown): Problem 7.55–Flash vaporization of benzene and toluene zB pB pT* xB yB nL nV 0.500 90.0 652 1021 0.5543 8.144 0.500 90.0 | 714 -6,093 0.500 90.0 Additional columns may be used to store other calculated variables (e.g., specific enthalpies). Briefly explain why Q is positive when P = 652 mm Hg and negative when P = 714 mm Hg. (e) In successive rows, repeat the calculation for the same zg and T at several pressures between Pmin and Pmax. Generate a plot (using the spreadsheet program itself, if possible) of ny versus P. At approximately what pressure is half of the feed stream vaporized?
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