02 Binary Fractionation
02 Binary Fractionation
Binary Fractionation
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Binary Fractionation
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BF-R00-01
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Binary Distillation
Mass Balance F = D+ B
X iF F = X iD D + X iB B
(i = 1 to N components)
Heat Balance hF F + QR = hD D + hB B + Qc
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Binary Distillation
Mass Balance V n + 1 = Ln + D
Yin + 1V n + 1 = X in Ln + X iD D
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Binary Distillation
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Binary Distillation
Mass Balance V n + 1 + Lo = V 1 + Ln
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Binary Distillation
ENVELOPE (4)
Rearranging the mass balance yields
V n + 1 = V 1 + Ln − Lo
Inserting this into the heat balance
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Binary Distillation
ASSUME
Sensible Heat Changes are Negligible
Heat Balance
hV V 1 + hV Ln − hV Lo + hL Lo = hV V 1 + hL Ln
Therefore Ln = Lo = Constant
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Binary Distillation
Constant Molal Overflow
Ln = Constant
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Binary Distillation
Constant Molal Overflow
VALIDITY?
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Binary Distillation
Equimolal Overflow
L = Constant
V = Constant
yin + 1 = ( L V )xin + ( D V )xiD
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Binary Distillation
BINARY Separations
xi x1, x2
x 2 = 1 - x1
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Binary Distillation
Equimolal Overflow
L' = Constant ≠ L
V ' = Constant ≠ V
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Binary Distillation
L
V
FV
F V' L
FL
L'
V'
BF-R00-02
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Binary Distillation
Feed Stage
V = L+ D
V ' = L' − B
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Binary Distillation
Since D + B = F
hV − hF
Then L' = L +
h − h F
V L
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Binary Distillation
hFV − hF
Define: q= V
hF − hFL
Then: L' = L + q F
n+ 1 q n 1
Also: y = x − xF At Feed Tray
(q − 1) (q − 1)
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Q Values
Condition Value of q
BP Liquid 1.0
DP Vapor 0
Sub Cooled Liquid >1.0
Superheated Vapor <0
Partly Vapor Mol Frac. Liquid
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Equilibrium K Value Definition
y
K=
x
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T-x Diagram
Dew Point Curve,
Saturated Vapor
T3
T1
Temperature
x3 x2 x1 y3 y2 y1
Mole Fraction (x or y)
Vapor or Liquid Phase
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Binary Distillation
EQUILIBRIUM
y = K 1x
(1 − y )= K 2 (1 − x )
1− K 2
x=
( K1 − K 2 )
y = K1 x
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Binary Distillation
EQUILIBRIUM
y = K 1x
(1 − y )= K 2 (1 − x ) Define
K K1
α=
=
y 1 x
K2
( 1− y) K (1 − x )
2
α x
y=
1 + (α − 1)x
y
x=
K1
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Equilibrium Curve or x-y Diagram
α x
y= Equilibrium Curves
1 + (α − 1)x
α =5
0.9
α = 2. 5
0.8 α = 1. 5
0.7 α =1
0.6
y, composition in 0.5
the vapor phase 45o line
0.4
0.3
0.2
0.1
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Binary System: Propane/Isobutane
n Specified
– Feed = 200 mol/h C3 + 200 mol/h iC4 at bubble
point
– Distillate = 196 mol/h
– Reflux = 400 mol/h at 100ºF
– Column pressure = 250 psia
– Number of trays = 24, feed on 13
n Problem
– Find xD and xB
464
– L = 1.16 R = 464 mol/h L F= = 1.16
400
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Binary System: Propane/Isobutane
xD = 0.927 0.917
xB = 0.090 0.098
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Internal vs. External Reflux
BF-R00-03
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Internal vs. External Reflux
hV 2 V2 + hR R = hV 1 V1 + hL1 L1
V1 = R + D
V2 = L1 + D
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Internal vs. External Reflux
ASSUME: hV 1 = hV 2
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Binary System: Propane/Benzene
n Specified
– Feed = 50 mol/h C3 + 50 mol/h Bz at bubble point
– Distillate = 50 mol/h
– xD = 0.99
– Column pressure = 215 psia
– Number of trays = 10, Feed on 6
n Problem
– Find reflux rate (temp = 100ºF)
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Binary System: Propane/Benzene
R = 5 Mol/hr R = 14 Mol/h !!
If 5 Mol/h, xD = 0.967
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Equilibrium
Pressure Constant
T y
x, y x
Ideal Vapor/Liquid Equilibria:
Systems that conform to Raoult's Law
(i.e. p* = P vx, ∴ α = Pv1 = constant)
P v2
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Equilibrium
Pressure Constant
T y
x, y x
Large Deviation from Ideality:
e.g. Minimum boiling azeotrope
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Water K Values
Y
K=
X
P o (1 − X HW )
Y=
π
and
X = X wh
(1 − X hw )P o
Kw =
X whπ
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Water Equilibrium Curve
α X
Y=
1 + (α − 1)X
As X goes to 0
Y=αX
and, therefore: ln(Y )= ln(α )+ ln( X )
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Summary of Equations
Equilibrium curve
n(1 − K 2 )
x = , y n = K 1 xn
(K 1 − K 2 )
or
n α xn
y = α = K1 K 2
1 + (α − 1)x n
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Summary of Equations
y n + 1 = ( L V )x n + ( D V )xD V = L+ D
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McCabe-Thiele
BF-R00-04
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Problem
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Problem
x F = 50 100 = 0.50
x F F = xD D + xB B
B=F− D
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Propane - Normal Butane
π= 200 psia
ºF K1 K2 α x1 y1
110 1.058 0.4098 2.58 0.911 0.963
120 1.151 0.4622 2.49 0.781 0.899
130 1.249 0.5180 2.41 0.659 0.824
140 1.350 0.5769 2.34 0.547 0.739
150 1.456 0.6389 2.28 0.442 0.643
160 1.566 0.7036 2.23 0.344 0.538
170 1.681 0.7710 2.18 0.252 0.423
180 1.801 0.8408 2.14 0.166 0.299
190 1.925 0.9130 2.11 0.086 0.165
200 2.051 0.9875 2.08 0.102 0.024
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Rectifying Section
y n + 1 = ( L V )x n + ( D V )x D , V = L+ D
Note: When xn = xD
L D
y n+ 1 = + xD = xD
L + D L + D
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Rectifying Section
L = 100 Mol/h
D = 50 Mol/h
L L
Slope = =
V L+ D
100
Slope = = 0.67
100 + 50
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Feed Q Line
n+ 1 q n 1 hVF − hF
y = x − xF q= V
(q − 1) (q − 1) hF − hFL
Note: When xn = xF
n+ 1 q 1
y = − xF = x F
q − 1 q − 1
can plot equation as a straight line with slope equal to
q/(q-1) that passes through the point (xF, xF)
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Feed Q Line
Therefore,
q =1
1
q Line Slope = =∞
1− 1
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McCabe Thiele
BF-R00-05
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McCabe Thiele
Effect of Feed Enthalpy
BF-R00-14
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McCabe Thiele
BF-R00-08
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McCabe Thiele
BF-R00-09
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McCabe-Thiele
Limiting Conditions
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McCabe Thiele
Minimum Trays
BF-R00-15
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McCabe Thiele
BF-R00-11
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McCabe Thiele
Minimum Reflux
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More Reflux or More Trays
Reflux
Rmin
Nmin Trays
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McCabe Thiele
BF-R00-12
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McCabe Thiele
BF-R00-13
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Minimum Trays
Fenske Equation
Log (rD rB )
nm =
Log α
XD
rD =
1− X D
XB
rB =
1− X B
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Feed Tray Location
Then
R
LOG (rD rF ) Assume ratio holds
nm
=
nm LOG (rD rB )
{ for any reflux ratio
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Minimum Reflux
Underwood Method
1 − xF α xF
1) + = 1 − q,1 < φ< α
1− φ α − φ
(1 − xD ) α xD
2) (L D )min = + − 1
(1 − φ) (α − φ)
Solve equation 1 for the proper root of the
quadratic for φ.
Solve equation 2 for (L/D)min using the φfrom
equation 1.
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Minimum Reflux
(1 − q )φ2 + (q + αq + α xF − α − xF )φ− qα = 0
A φ2 + B φ+ C = 0
− B ± B 2 − 4 AC
φ=
2A
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Minimum Reflux
Underwood Method
q =1
1 xD α (1 − xD )
(L D )m = −
α − 1 xF (1 − xF )
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Minimum Reflux
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Analytical Techniques
1.0
The Gillliland Relation
0.9 Trays and reflux as a function of their minimal
IEC, 1940, (p.1220)
0.8
N = Theoretical Plates (Design)
0.7 Nm = Min. Theor. Plates (L/D = ∞ )
R = L/D (Design)
Rm = L/D Min. (N = ∞ )
0.6
0.5
0.4
R - Rm
X= R+1
0.3 N - Nm
Y= N+1
0.2
0.1
0.0
0.0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1.0
X
BF-R01-16
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Analytical Techniques
R − Rm Rm + X
X= R=
R+ 1 1− X
N − Nm Nm + Y
Y= N=
N+ 1 1− Y
X + Y are parameters, not compositions
Determine:
Rm from Underwood Equation
Nm from Fenske Equation
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distributed for any purpose whatsoever except by written permission of UOP LLC and except as authorized under agreements with UOP LLC.
Example
XF = 0.5 rF = 1.0
XD = 0.927 rD = 12.7 D/F = 0.49
XB = 0.090 rB = 0.0989
α = 1.76 q = 1.0
UNDERWOOD
(L D )m = 1 X D − α (1 − X D )
α − 1 X F (1 − X F )
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Example
FENSKE
LOG (rD rB )
nm = = 8.59
LOGα
R
nm LOG (rD rF )
= = 0.523
nm LOG (rD rB )
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Example
GILLILAND
N − Nm
Y= = 0.616 → X = 0.055
N+ 1
( L D )m + X
L D= = 2.28 → R F = 1.12
1− X
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distributed for any purpose whatsoever except by written permission of UOP LLC and except as authorized under agreements with UOP LLC.
Example
N = 24 L/D = 2.28
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Smoker’s Equation
n Simplified form
ln (S )
N=
R+ q
ln α 1 −
( R + 1)( RxF + q)
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Equilibrium Stage
v n lin− 1
i
Stage n
vin+ 1 lin
V n+ 1 hvn+ 1 Ln hln
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Conventional Tray
Vn? Vn?
Ln-1
Ln
Vn+1
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Efficiency
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Typical Observed Tray Efficiency
(Simplistic Overall)
1.2 90
2.0 70
3.0 50
5.0 20
15.0 10
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Tray Efficiency
n Define Feed
n Define Product Specification
n Set Column Pressure
n Optimize Column Design
n Set Composition Control
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Define Feed
n Composition
n Flow Rate
n Temperature
n Pressure
n Enthalpy
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Define Product Specifications
n Receiver Temperature
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Set Column Pressure
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Set Column Pressure
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Optimize Column Design
n Feed Preheat
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Optimum Trays
Trays vs. Reboiler Duty
15
Reboiler Duty
10
0
0 10 20 30 40 50 60
Number of Theoretical Stages
BF-R01-19
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Best Feed Tray
38 Total Stages
15
10
0
0 10 20 30 40
Feed Stage BF-R01-19
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Feed Preheat Efficiency
60
50
40
30
20
10
0
0 10 20 30 40 50 60
Preheat Duty, MBtu/h
BF-R00-20
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