1-OPERASI-MULTISTAGE1
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Transcript of 1-OPERASI-MULTISTAGE1
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IDEAL STAGEFeed
F, xF
Distillate
D, xD
Bottom Product
B, xB
SINGLE-STAGE (FLASH) DISTILLATION
UNECONOMICAL
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3
2
4
1
5
F, xF
V1
V2
V3
V5
V4
V6L5
L4
L3
L2
L1
L0
Countercurrent multistage contact
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Simple counter-current flow cannot give as
complete a separation as required
N = More concentrated L0
uneconomical x0is fixed by other
consideration
Where does L0
come from?
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Multistage cascade
with reflux at bothends for distillation
V1
-qC
m
p
LC
D
F
Enriching
section
Strippingsection
F-1
F+1
N
1
B
C
S qS
L0
Condenser
Reboiler
NL
1NV
SL
F
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ZERO REFLUX
No liquid returned to stage 1
No condensation of V2to
supply liquid leaving stage 1
The vapor leaving stage 1
would be the same quantity andcomposition of the vapor
leaving stage 2.
The vapor leaving stage 2
would be the same quantity and
composition of the vaporleaving stage 3.
Etc.
V1
-qCLC
D
F F
1
C
2
V2
V3
3
Multistage cascade with no
liquid reflux
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F
N-2
N-1
N
F
B
SqS
NL
1NV 0L
S
1NL
2NL
If the vapor reflux were eliminated:
No vapor returned to stage N
No vaporization of to
supply vapor leaving stage N
The liquid leaving stage N
would be the same quantity andcomposition of the liquid
leaving stage N-1.
The liquid leaving stage N-1
would be the same quantity and
composition of the liquidleaving stage N-2.
Etc.
1NL
Multistage cascade with no
vapor reflux
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A fractionating column by its inherent nature has two limits of
operation based upon reflux ratio:
Minimum reflux
Total reflux
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MINIMUM REFLUX
D
B
F
L0 There is insufficient liquid returned
to the column
There is only an infinitesimal
change in vapor and liquid
compositions through the plates.
Infinite number of plates would be
needed.
Actual operation of a column
below or at minimum reflux isimpossible.
Schematic representation of
minimum reflux operation
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TOTAL REFLUX
All condensate is returned to
the column
It requires the least number of
stages.
Practically no overhead
product and no bottomproduct can be made and no
feed is introduced.
It is possible to operate
experimentally a fractionating
column at total reflux when thesystem inventory is large and
only very small samples of
distillate and bottoms are
removed.
D = 0
B = 0
F = 0
Schematic representation of total
reflux operation
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MINIMUM REFLUX VS TOTAL REFLUX
Large reflux ratio
Small reflux ratio
More coolant
More heating medium
Greater operating cost
Greater number of
plates
Greater investment
cost
$/unitpro
duct
Number of stages
Nmin
Total cost
Operating cost
Equipment cost
Optimum design
at minimum cost
Schematic relationship between reflux
ratio and number of stages
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Over-all:
Component i:
(1)
(2)
(3)
(4)
(5)
V1= L0+ D
D01 ii0i1 xDxLyV
D01 iii xxy
11
0
V
D
1V
L
1
D
V
D
L 10
MATERIAL BALANCE AROUND TOTAL CONDENSER
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D0D100D0D111 hLhVhLQLQVHV
DD0
DD1
1
0
Qhh
QhH
V
L
01
1DD0
hH
HQh
D
L
(10)
(11)
V1H1+ (V1L0) QD= L0h0+ (V1L0) hD
DD11DD00 QhHVQhhL
Introducing eq. (1) into eq. (8) to eliminate V1yields:
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MATERIAL BALANCE IN ENRICHING SECTION
V1, y1, H1
L1, x1, h1 L0
x0h0
D
xDhD
qD
Vm+1
ym+1
Hm+1
Lmxm
hm
F
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Over-all:
Component i:
(12)
(13)
(14)
Vm+1= Lm+ D
Dm1m iimi1m xDxLyV
Dm1m im1mimi1m xLVxLyV
Dm
D1m
ii
ii
1m
m
xx
xy
V
L
Introducing eq. (12) into eq. (13) to eliminate Dresults in
D1mDm ii1miim xyVxxL
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(15)m1m
1mD
ii
iim
xy
yx
D
L
Introducing eq. (12) into eq. (13) to eliminate Vm+1
results in:
Dm1m iimim xDxLyDL
1mDm1m iiiim yxDxyL
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ENTHALPY BALANCE IN ENRICHING SECTION
(16)DmmD1m1m hDhLQDHV
Dm1mmmDm1m1m1m hLVhLQLVHV
Introducing eq. (12) into eq. (16) to eliminate Dresults in
DmD1mmmDmD1m1m1m hLhVhLQLQVHV
DD1m1mDDmm QhHVQhhL
DDm
DD1m
1m
m
Qhh
QhH
V
L
(17)
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m1m
D1mDm
hH
QHh
D
L
(18)
Introducing eq. (12) into eq. (16) to eliminate Vm+1
results in:
DmmD1mm hDhLQDHDL
DmmD1m1mm DhhLDQDHHL
D1mDm1mm QHhDhHL
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Partial condenser
MATERIAL AND ENTHALPY BALANCES
AROUND PARTIAL CONDENSER
V1, y1, H1
L1, x1, h1
L0
x0
h0
D
yD
HDqD
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Over-all:
Component i:
(19)
(20)
(21)
V1= L0+ D
D01 ii0i1 yDxLyV
0
D
D01
i
i
Diiix
yK;xxy
D01 i01i0i1
yLVxLyV
(22)D0
D01
D0
D1
ii
iii
ii
ii
1
0
K1x
Kxy
yx
yy
V
L
D1D0 ii1ii0 yyVyxL
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(23)
D01 ii0i0 yDxLyDL
01
1D0
01
1D
ii
iii
ii
ii0
xy
yKx
xy
yy
D
L
1D01 iiii0
yyDxyL
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V1H1+ (V1L0) QD= L0h0+ (V1L0) HD
DD11DD00 QHHVQHhL
DD0
DD1
1
0
QHh
QHH
V
L
(27)
Replacing D in equation (26) with (V1L0):
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01
1DD0
hH
HQH
D
L
(28)
(L0+ D) H1+ D QD= L0h0+ D HD
1DD010 HQHDhHL
Replacing V1in equation (26) by (L0+ D):
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MATERIAL BALANCE IN ENRICHING SECTION
WITH PARTIAL CONDENSER
V1, y1, H1
L1, x1, h1
L0
x0h0
D
yD
hD
qD
Vm+1
ym+1
Hm+1
Lm
xm
hm
F
m
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Over-all:
Component i:
(29)
(30)
(31)
Vm+1= Lm+ D
Dm1m iimi1m
yDxLyV
Dm1m im1mimi1m yLVxLyV
Dm
D1m
ii
ii
1m
m
yx
yy
V
L
D is eliminated from equation (30) by substituting D with
(Vm+1Lm):
D1mDm ii1miim yyVyxL
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(32)m1m
1mD
ii
iim
xy
yy
D
L
Dm1m iimim yDxLyDL
Vm+1is eliminated from equation (30) by substituting
Vm+1with Lm+ D
1mDm1m iiiim yyDxyL
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ENTHALPY BALANCE IN ENRICHING SECTION
V1, y1, H1
L1, x1, h1L0
x0
h0
D
xD
hD
qD
Vm+1
ym+1
Hm+1
Lm
xmhm
F
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(33)
(34)
DmmD1m1m HDhLQDHV
Dm1mmmDm1m1m1m HLVhLQLVHV
D is eliminated from equation (33) by substituting D with
Vm+1Lm
DDm
DD1m
1m
m
QHh
QHH
V
L
DD1m1mDDmm QHHVQHhL
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Vm+1is eliminated from equation (33) by substituting
Vm+1with Lm+ D
DmmD1mm HDhLQDHDL
m1m
D1mDm
hH
QHH
D
L
D1mDm1mm QHHDhHL
(35)
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MATERIAL BALANCE IN STRIPPING SECTION
qBB
xB
hB
yp+1Hp+1xphp
F
1pV pL
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Over-all: BVL 1pp
Component i: B1pp ii1pip xByVxL
B1pp i1ppi1pip xVLyVxL
Bp
B1p
ii
ii
1p
p
xx
xy
V
L
(36)
(37)
(38)
Replacing B in equation (37) with 1pp VL
B1pBp ii1piip xyVxxL
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ENTHALPY BALANCE:
B1p1pBpp
hBHVqhL qB= B QB
B1p1pBpp hBHVQBhL
B1pp1p1pB1pppp hVLHVQVLhL
BB1p1pBBpp QhHVhQhL
BBp
BB1p
1p
p
hQh
QhH
V
L
(39)(40)
(41)
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MATERIAL & ENTHALPY BALANCES ABOUT REBOILER
qB
BxB
hB
yN+1
HN+1
yN
HN
1NV NL
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Over-all: BVL 1NN
Component i: B1NN ii1NiN xByVxL
B1NN i1NNi1NiN xVLyVxL
BN
B1N
ii
ii
1N
N
xx
xy
V
L
(42)
(43)
(44)
Replacing B in equation (43) with1NN VL
B1pBp ii1piip xyVxxL
MATERIAL BALANCE AROUND THE FEED PLATE
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MATERIAL BALANCE AROUND THE FEED PLATE
F = FV+ FL
LV FFF HHh
LV FFF xyx
1pV Hp+1
yp+1
pL
hp
xp
Vm+1
Hm+1ym+1
Lm
hmxm
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Over-all:
1mpm1pLV VLLVFF
Component i:
1mpm1pLV i1mipimi1pF,iLF,iV yVxLxLyVxFyF
1m1pV VVF
pmL LLF
(45)
(48)
(46)
(47)
1mp
m1pLV
i1mimL
imiV1mF,iLF,iV
yVxLF
xLyFVxFyF
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(49)
V1pLp1p1mpm F,iiVF,iiLii1miim yyFxxFyyVxxL
pm
V1p
pm
Lp
pm
1p1m
ii1m
F,iiV
ii1m
F,iiL
ii
ii
1m
m
xxV
yyF
xxV
xxF
xx
yy
V
L
If the feed is a saturated liquid, the last term in eq. (49)
drops out.
If the feed is a saturated vapor, the middle term on the
right side of eq. (49) drops out.
ENTHALPY BALANCE AROUND THE FEED PLATE
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ENTHALPY BALANCE AROUND THE FEED PLATE
pp1m1mmm1p1pFLFV hLHVhLHVhFHF LV
pmL1m1mmm1pV1mFLFV hLFHVhLHFVhFHF LV
VL F1pVFpL1p1m1mpmm HHFhhFHHVhhL
pm
F1p
1m
V
pm
Fp
1m
L
pm
1p1m
1m
m
hh
HH
V
F
hh
hh
V
F
hh
HH
V
LVL
(50)
(51)
If the feed is a saturated liquid, the last term in eq.
(51) drops out.
If the feed is a saturated vapor, the middle term on
the right side of eq. (51) drops out.
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In liquid mixture / solution the molal enthalpy of the
mixture at a given T and P is the sum of the partial molal
enthalpies of the components composing the mixture.
ni
im hh (52)
In regular / ideal mixtures:
oiii hxh (53)
For gaseous / vapor mixtures at normal T and P:
ni
ii
n
iim yhH (54)