NCHU-SF : Ch. 2-11 SUPERCRITICAL FLUIDS FOR SEPARATION.
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Transcript of NCHU-SF : Ch. 2-11 SUPERCRITICAL FLUIDS FOR SEPARATION.

NCHU-SF : Ch. 2-1
SUPERCRITICAL FLUIDS
FOR
SEPARATION

NCHU-SF : Ch. 2-2
What for
do we need phase equilibrium?
Design of solvent cycle (process)
Objectives

NCHU-SF : Ch. 2-3
Solubility of the compounds
Change of solubility with process conditions
Capacity of the solvent
Solubility of solvent in condensed phase
Distribution of compounds between the phases (separation factor, selectivity)
Two-phase area
What do we need to know about phase equilibrium?
Objectives

NCHU-SF : Ch. 2-4
For what type of systems (chemical compounds) do we need phase
equilibrium?
CO2, C3H8, H2O, .... (gases)
Paraffins, glycerides, vitamins, ...
Terpenes, sesquiterpenes, mono-, di-, tri-
....
....
Objectives

NCHU-SF : Ch. 2-5
Extraction with Supercritical Fluids
The need for phase equilibria:
Solubility, K-factor, Separation factor, Two-phase region
Flow scheme of gas extraction (SFE)

NCHU-SF : Ch. 2-6
Kennedy 1950
Solubility of quartz in water

NCHU-SF : Ch. 2-7
Poynting-effect
Vapor pressure enhancement E.U. Franck 1956____ 25 oC, ------ 500 oC
.d
d 0
G
L
TV
V
P
P
,ln 0102
01
PPRT
V
P
P L P02/P01 VL

NCHU-SF : Ch. 2-8
Poynting-Factor
System: Ethanol - Water, 343 K
Ethanol Water
kPa
10 1.0022 1.00061000 1.022 1.006510000 1.2425 1.0667
01
02
PP

NCHU-SF : Ch. 2-9
Density CO2 (calc. Bender EOS)

NCHU-SF : Ch. 2-10
Silan, Vapor Curve
1,E-05
1,E-04
1,E-03
1,E-02
1,E-01
1,E+00
1,E+01
1,E+02
75 125 175 225 275
Temperature, K
Pre
ssu
re, b
ar
Vapour Pressure vs. Temperature

NCHU-SF : Ch. 2-11
Density of supoercritical Fluid responsible for solvent power
(increasing with pressure, decreasing with temperature)
Hydrostatic pressure enhances effective vapour pressure
(Poynting effect, small)
Temperature increases vapour pressure
(exponentially, big effect)
Influences on Solute Concentration in Gaseous Phase

NCHU-SF : Ch. 2-12
Solubility of Caffeine in CO2
Gährs 1984Ebeling, Franck 1984Johannsen, Brunner 1994

NCHU-SF : Ch. 2-13
Tsekhanskaja 1964
So
lub
ility
[g
/l]
Solubility of Naphthalene in Ethylene

NCHU-SF : Ch. 2-14
Brunner 1978
Oleic acid - ethylene

NCHU-SF : Ch. 2-15
Solubility of oleic acid in various gases
Brunner 1978

NCHU-SF : Ch. 2-16
Solubility of Triglycerides in sc Gases
Triglycerides of palm oil
Brunner 1978

NCHU-SF : Ch. 2-17
Solubility in sc CO2

NCHU-SF : Ch. 2-18
Solubility of Xanthines in dry sc CO2
Johannsen and Brunner 1994

NCHU-SF : Ch. 2-19
P,T,x-diagram of a binary system

NCHU-SF : Ch. 2-20
P,x-diagram ethane - heptane
Kay 1938

NCHU-SF : Ch. 2-21
Kay 1938
T,x-diagram ethane - heptane

NCHU-SF : Ch. 2-22
Melting point temperature of B higher than critical temperature of A
Phase equilibria of a binary system

NCHU-SF : Ch. 2-23
Phase equilibrium in a binary system
Melting point temperature of B higher than critical temperature of A;Interrupted critical curve.

NCHU-SF : Ch. 2-24
P,T- projections of phase boundary lines

NCHU-SF : Ch. 2-25
Phase behaviour of a ternary system
Temperature dependence
Pressure dependence

NCHU-SF : Ch. 2-26
CO2 - benzene - oleic acid

NCHU-SF : Ch. 2-27
Ethylene - DMF - C18 fatty acids

NCHU-SF : Ch. 2-28
Solubility Enhancement by a Modifier

NCHU-SF : Ch. 2-29
Sch
mitt
198
4Solubility Enhancement by Entrainer (Modifier)

NCHU-SF : Ch. 2-30
Gährs 1984
Solubility of Caffeine in CO2
Influence of nitrogen

NCHU-SF : Ch. 2-31
Influence of propane
Prausnitz, Joshi 1984
Solubility of Phenanthrene in CO2

NCHU-SF : Ch. 2-32
Phase Equilibrium in a Ternary System
Brunner 1983

NCHU-SF : Ch. 2-33
Brunner 1983
Solubility in a gas with a modifier
Influence of temperature

NCHU-SF : Ch. 2-34
Brunner 1983
Separation Factor
Influence of entrainer

NCHU-SF : Ch. 2-35
Influence of concentration
Brunner 1983
Separation Factor

NCHU-SF : Ch. 2-36
Three Phase Equilibrium

NCHU-SF : Ch. 2-37
P,T-diagrams of Complex Mixtures

NCHU-SF : Ch. 2-38
Measuring Phase Equilibrium

NCHU-SF : Ch. 2-39
Measuring Phase Equilibrium

NCHU-SF : Ch. 2-40
Modeling of Phase Equilibrium with EOS
HPW modification of RK-EOS

NCHU-SF : Ch. 2-41
Gas-Liquid Phase Equilibrium
Two different ways:
A
= standard fugacity i = activity coefficient: gE-models)
B
= fugacity coefficient: Equations of state
LVii ff
0iiii fxf
0if
Pxf iii
i
Thermodynamic Equilibrium

NCHU-SF : Ch. 2-42
VLE-Calculation:
With the simplification:
since
:
LVii ff
Pyfx iiiiiV0
Pyfx iiSATiii
V
SATi
SATi
SATi Pf PyPx iii
SATSATiii
V
Calculation of Phase Equilibrium

NCHU-SF : Ch. 2-43
Low pressure High pressure
.0iiiii pxPyp
.0
P
pK iii
0
0
jj
iiij p
p
.0iiiii pxPy
.i
ioi
i P
pK
.0
0
ijj
jiiij p
p
Phase Equilibrium: Non Ideal Solutions

NCHU-SF : Ch. 2-44
P = 101 kPa
Methanol - water Chloroform - acetone
= 1
= 1
Concentration dependence of separation factor

NCHU-SF : Ch. 2-45
Concentration dependence of separation factor

NCHU-SF : Ch. 2-46
1lim
1
TPT
TfK
si
sireines
si
ixi
P
H
P
fK
vi
isvi
iii
xi
,,
0
0lim
T = const.
VLE
T = const.
VLE
xsf = const.
xsf = solvent free concentrations in liquid phase
Limiting values of the partition coefficient K
Phase Equilibrium

NCHU-SF : Ch. 2-47
jr
vjs
ijjr
vj
vireines
si
si
ijx H
TPf
TPT
i
,
0
,
1lim
jr
si
ijx H
P
i
lim1
0,
0
0 ,,
,,lim
jsfl
j
sfvvj
vi
iiij
x fxvT
yvTf
i
s
s
x P
P
2
1112
0lim
1
Limiting values of separation factor
Binary system i-j in a multicomponent system At low pressure
s
s
sf
s
x P
P
H
P
22
1112
1lim
1
Binär:
Phase Equilibrium

NCHU-SF : Ch. 2-48
Murphy´s Law of Thermodynamics
THINGS GET WORSE
UNDER PRESSURE