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MARCH 2012 LCGC NORTH AMERICA VOLUME 30 NUMBER 3
1
Coupling Supercritical Fluid Chromagraphy
with Evaporative Light Scattering Detection:
A Study of the Relevant Parameters Ruling
Response
The complex phenomena involved in the use of evaporative light
scattering detection (ELSD) with high performance liquid chromatography
(HPLC) are fairly well described. Because the mobile phase is nebulized
to produce droplets, however, the use of supercritical fluids as mobile
phase with this low-pressure detection method is favored because of the
fluid depressurization, before the detector entrance, which allows the
aerosol formation. Despite the use of ELSD coupled with supercritical fluid
chromatography (SFC) for various applications, however, there has been no
study of the ELSD response variation with supercritical carbon dioxide–based
mobile phases. Nor has any comparison with HPLC in terms of response (peak
area) been reported. These points are partially addressed in this article.
T
E. Lesellier and C. West are with the
Institut de Chimie Organique et Analytique,
at the Université d’Orléans in Orléans,
France. T. Bizet, A. Valarché, and
M. Dreux are with Sedere in Orléans,
France.
he use of evaporative light scattering detection (ELSD) with
high performance liquid chromatography (HPLC) overcomes some of
the drawbacks and limitations of using
ultraviolet (UV) detection — ELSD can
be used for the detection of compounds
lacking a chromophore group, provides
no baseline deviation during gradient
elution, and can be used with solvents
having a high degree of UV absorption
(1,2). The principle of ELSD is based
on nebulization of the mobile phase, a
process by which an aerosol is produced
by the addition of a nebulizer gas (nitrogen) (3–8). This process takes place in a
nebulizing chamber that can have various dimensions and volumes depending on the manufacturer. It can also be
adapted to the type of chromatography
used — HPLC, ultrahigh-pressure LC
(UHPLC), or micro-LC. The droplets,
consisting of the analyte molecules and
an unknown amount of solvent, are
introduced into a drift evaporative tube
and heated at varied temperatures. The
droplet size is reduced by further solvent
evaporation as the droplets pass through
this tube. Finally, the droplets go through
a light source, and the deflected light is
collected by a photomutiplier.
The response depends on the particle
(droplet) size, which seems to increase
with the increasing compound concentration and which is related to numerous
physical properties of the solvents composing the mobile phase: viscosity, surface tension, and volatility. This explains
that the response (A) variation with the
concentration (m) is generally nonlinear
for noncapillary columns, and follows
the relation:
A = a·mb
[1]
Consequently, to follow a linear trend,
calibration curves should be plotted with
double logarithmic coordinates:
log A = b·log m + log a
[2]
Equation 2 also can be written for identical injected volumes:
log A = b·log c + log a
[3]
Consequently, using a gradient elution
in reversed-phase HPLC, that is, increas-
2
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LCGC NORTH AMERICA VOLUME 30 NUMBER 3 MARCH 2012
(a)
2500
Peak area
2000
1500
1000
y=127.41x + 26.885
R2=0.9999
500
0
0
2
4
6
8
10
12
14
16
Injected volume (μL)
(b)
3.60
3.40
y=1.394x + 1.7207
R2=0.9998
3.20
Log A
3.00
2.80
2.60
2.40
2.20
2.00
0.00
0.20
0.40
0.60
0.80
1.00
1.20
1.40
Log V inj
Figure 1: (a) Peak area (A) variation with injected volume (V inj ) of caffeine.
Each value is calculated based on six measurements. Blue diamonds: ELSD; pink
squares: UV 210 nm. (b) Log A vs. log V inj with ELSD (from 2 to 15 µL).
700
Peak area
600
500
400
300
200
100
0
0
1
2
3
4
5
Nebulizer gas pressure (bar)
Figure 2: Variation of peak area with pressure of nebulizer gas. Blue diamonds: Sedex
55 nebulizing chamber; green circles: Sedex 85 nebulizing chamber.
ing the organic solvent content in the
mobile phase, leads to changes in the
droplet size that favor the response of the
compounds in relation to their retention
time (4,9,10). A compensation gradient
added after the column makes it possible
to limit this drawback by keeping the
mobile-phase composition at the detector entrance constant (10,11).
Other parameters induce great
response changes, such as the atomization pressure (3,4), which is related to
the flow rate of the nebulizer gas; the
geometry of the nozzle (mainly the capillary diameter) (7,8); and the location
of the mixing point of the mobile phase
with this gas. The wavelength of the
light source used also plays a role in the
response intensity (6).
On the other hand, because of the
nebulization process required, coupling
supercritical fluid chromatography (SFC)
with ELSD has been successfully done in
the past (12–18). The specificity of the
carbon dioxide–modifier (an organic
solvent) mobile phase used in SFC is the
pressure required at the column outlet
to ensure the dense state of the fluid.
This back-pressure is achieved with a
back-pressure regulator or a restrictor,
located after the column. However, after
the back-pressure regulator or restrictor,
carbon dioxide returns back to a gaseous
state, thus favoring aerosol formation in
the nebulizer chamber. However, this
carbon dioxide depressurization cools
the outlet capillary, which can induce
dry-ice formation and possibly plug the
capillary. Heating, provided either by the
back-pressure regulator or by an additional transfer line, avoids this drawback.
Beyond these studies addressing this
coupling of SFC to ELSD, however, few
studies are available to describe the varied
effects of the numerous chromatographic
parameters affecting SFC separations.
The difficulty of interfacing SFC with
a low-pressure detector, given the phase
separation between the liquid solvent
and gaseous carbon dioxide, has been
addressed (19), but no clear comparison
has been performed between SFC and
HPLC to evaluate how the use of carbon
dioxide instead of a liquid affects ELSD
responses in terms of area or sensitivity. That comparison is the topic of this
paper. In this study, we use a Sedex 85
ELSD system (Sedere, Orléans, France)
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MARCH 2012 LCGC NORTH AMERICA VOLUME 30 NUMBER 3
700
680
Peak area
660
640
620
600
580
560
80
100
120
140
160
180
200
Outlet pressure (bar)
Figure 3: Variation of peak area with the column outlet pressure. Blue diamonds:
ELSD; pink squares: UV at 210 nm.
800
700
Peak area
600
500
400
300
200
3
regulator tube (internal diameter 0.25
mm) was heated to 60 °C to avoid dry
ice formation during the carbon dioxide depressurization. The ELSD system
(Sedex 85, Sedere, Orléans, France) was
connected to the outlet capillary. The
nebulizer tubing was slightly different
from the one used with HPLC, in that
the capillary diameter was 150 µm. The
nebulizer gas (nitrogen) pressure was 2
bar and the drift temperature was 50
°C. Chromatograms were recorded using
Azur software (Datalys, France).
The main column used was a 250
mm × 4.6 mm, 5-µm dp Synergi Fusion
RP column (Phenomenex, Torrance,
California), the mobile phase was 90:10
carbon dioxide–ethanol (except for the
study of the modifier percentage), the
temperature was 25 °C, the outlet pressure was 15 MPa, and the flow rate was
3 mL/min. Caffeine was provided by
Sigma-Aldrich (St. Louis, Missouri). The
injected volume was 5 µL for most studies, and the concentration was 2.5 mg/
mL. Other columns used included a 250
mm × 4.6 mm, 5-µm dp Cyano column
(Princeton, Cranbury, New Jersey) and a
250 mm × 4.6 mm, 5-µm dp Uptisphere
HDO column (Interchim, Montluçon,
France).
Results and Discussion
100
0
30
40
50
60
70
80
Drift evaporative tube temperature (°C)
Figure 4: Variation of peak area with the drift evaporative tube temperature.
with a slightly adapted nebulizer, mainly
with carbon dioxide–ethanol mobile
phases, with the goal of using green chromatographic conditions.
Experimental
Chromatographic separations were performed using equipment manufactured
by Jasco (Tokyo, Japan). Two model
980-PU pumps were used, one for carbon dioxide and another for the modifier. Control of the mobile-phase composition was performed by the modifier
pump. The pump head used for carbon
dioxide was cooled to −2 °C by a cryostat (Julabo F10c, Seelbach, Germany).
When the two solvents (modifier and
carbon dioxide) were mixed, the fluid
was introduced into a dynamic mixing
chamber (model PU 4046, Pye Unicam,
Cambridge, UK) connected to a pulsation damper. The injector valve was supplied with a 20-µL loop (model 7125,
Rheodyne, Cotati, California).
The columns were thermostated by an
oven (Jetstream 2 Plus, Thermotechnic,
Langenzersdorf, Germany). A UV detector with a high pressure–resistant cell was
set to control the injection repeatability
and volume (HP 1050, Hewlett-Packard). The detection wavelength was 210
nm. After the detector, the outlet column
pressure was controlled by a Jasco 88081 back-pressure regulator. The outlet
A first series of experiments was performed to study basic parameters:
injected volume, additional gas pressure,
outlet column pressure, drift temperature, and flow rate of the mobile phase.
To ensure accuracy of the quantitative
value studied, no split was used for these
experiments. That means that the entire
volume of supercritical mobile phase
eluted from the column was introduced
into the detector. By using a Jasco backpressure regulator, the transfer capillary
(around 10 cm in length) was heated to
60 °C. This was sufficient to avoid dryice formation and plugging of the transfer line.
Figure 1a shows the variation of the
caffeine peak area with the injected volume from 2 to 15 µL, with both the UV
and evaporative light scattering detectors.
As expected, the UV response displays a
linear variation, showing the accuracy
of tested volumes. The variation of the
ELSD response appeared to be exponential. Figure 1b shows, by using double
4
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LCGC NORTH AMERICA VOLUME 30 NUMBER 3 MARCH 2012
1200
1100
1000
Peak area
900
800
700
600
500
400
300
200
1
2
3
4
5
6
Mobile-phase flow rate (mL/min)
Figure 5: Variation of peak area with the mobile-phase low rate. Blue diamonds:
ELSD; pink squares: UV at 210 nm.
8
ELSD
3%; 3 mL/min
15 MPa; 25 °C
UV
4
150
Response (mV)
0
-4
100
2
4
6
8
50
3%; 5 mL/min
15 MPa; 25 °C
0
2
4
6
8
Time (min)
Figure 6: SFC separation of diastereoisomers. Column: Uptisphere HDO; mobile
phase: 97:3 (v/v) carbon dioxide–ethanol; temperature: 25 °C; Pout: 15 MPa. ELSD conditions: nitrogen pressure: 3 bar; drift temperature: 50 °C.
logarithmic coordinates, that the relationship between the response and the
injected volume is linear. This behavior is classical in comparison to the one
observed in HPLC. [AUTHOR: What
is meant by “classical” in the preceding sentence? Do you mean “typical”?
And what are you saying then about
the behavior in HPLC?] The standard
deviation measured for 10 injections of
10 µL was 0.5% for ELSD and 1.0% for
UV detection.
Figure 2 shows the detector response
compared to the nebulizer gas pressure,
from 0 to 4 bar (5 µL injected). For this
study, the nebulizer chamber of a Sedex
55 ELSD system was also tested with the
same nebulizer, because this model had
been used for analysis of carbohydrates
by SFC in the 1990s (13). The difference
between the two chambers is mainly the
length, with the chamber of the Sedex 85
system being about twice as long as that
of the Sedex 55 system.
The highest response values were
obtained with the longer nebulizing
chamber (Sedex 85) at 3 mL/min, which
seemed to be the optimal value. With
this longer chamber, the addition of the
nebulizer gas improved the response.
Finally, the optimal nebulizer gas pressure was close to the pressure usually
used in HPLC, despite the gaseous carbon dioxide introduced into the chamber
in SFC. As reported elsewhere (20,21),
the increase in the nebulizer gas flow rate
induces both the shift of the droplet size
toward smaller droplets and the increase
of the number of droplets. These two
effects should provide opposite response
changes, but the second effect must be
greater to explain the observed result
(20). The strong effect of gas pressure on
response was noticed also with HPLC
(4). In contrast to our results, other studies report a rapid response decrease with
an increase in the additional gas flow rate
(22,23), but the design of the nebulizer
nebulizing chamber, and the interface
section between the chamber and the
drift evaporative tube are not identical
from one detector to another (24) and
those differences may well be responsible
for the opposite observations.
Nevertheless, the responses obtained
without additional gas (Figure 2) are not
dramatically lower than those obtained
with additional nebulizer gas, showing a
rather good production of droplets as a
result of the carbon dioxide depressurization.
The outlet pressure (Pout) applied to the
chromatographic system was also studied from 9 to 19 MPa (Figure 3). With
both detection methods, but mainly for
ELSD, the response was enhanced by an
increase in outlet pressure. Increasing
Pout enhances the fluid density before
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MARCH 2012 LCGC NORTH AMERICA VOLUME 30 NUMBER 3
(a)
500
3
400
1
4
Response (mV)
300
2
200
100
0
1
2
3
4
5
Time (min)
(b)
1
Response (mV)
225
150
75
3
4
2
0
1
2
3
4
5
Time (min)
Figure 7: Separation of four pharmaceutical compounds. Column: Cyano; mobile
phase: 90:10 (v/v) carbon dioxide–ethanol; temperature: 25 °C; Pout: 15 MPa. ELSD
conditions: nitrogen pressure: 3 bar; drift temperature: 40 °C. UV detection wavelength: 210 nm. ELSD detection (a); 3 mL/min (blue signal); 7 mL/min (red signal); UV
detection (b); 3 mL/min (blue signal); 7 mL/min (red signal). Peaks: 1 = theophyline; 2
= cortisone; 3 = hydrocortisone, 4 = dexamethasone.
5
the back-pressure regulator, leading to
a reduction in the linear speed of the
mobile phase that enhances the residence
time of the compounds in the cell; the
increased residence time explains the
response increase, mainly from 11 to 16
MPa (a refractive index change in the cell
also can modify the UV response) (25).
The greater amount of carbon dioxide
before the back-pressure regulator also
results in an enhanced fluid speed in the
nebulizer (after the back-pressure regulator), which seems to favor the ELSD
response.
The temperature of the drift evaporative tube was also studied from 40 °C to
70 °C (Figure 4). With caffeine, a semivolatile compound, the increase in this
evaporative temperature leads to a regular decrease in response. This classical
behavior has been reported with HPLC
(3) and results from the reduction of particle size by vaporization with increasing
temperature.
The flow rate of the mobile phase was
also studied from 2 to 5 mL/min (Figure 5). With both detectors the response
decreases when flow rate increases. For
UV, a concentration detection method,
this behavior is expected; the residence
time in the cell decreases as the mobilephase flow rate increases. As reported
previously, the nonlinear decrease of
the UV response also could be caused
by varied effects related to the fluid
density change. However, for ELSD, a
mass detection method, these flow-rate
changes would not modify the amount
of compound going through the detection system.
In HPLC, varied trends have been
observed. An increase in response with
the flow rate (from 0.1 to 1 mL/min)
was reported for a concentric nebulizer
by direct solute injection (no chromatographic column) (23), whereas the
opposite was seen with different mobile
phases, different compounds, and drift
temperatures (6,21,26).
From the Nukiyama–Tanasawa equation (27), the increase in the mobilephase f low rate should improve the
average particle diameter. Larger droplet
diameters are supposed to enhance ELSD
response (up to a limit value) (6,28), but
they also favor droplet condensation and
precipitation on the walls of the nebulizing chamber, thus decreasing the num-
6
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LCGC NORTH AMERICA VOLUME 30 NUMBER 3 MARCH 2012
3% ethanol
150
20% ethanol
5% ethanol
100
15% ethanol
10% ethanol
50
0
2
4
6
8
Figure 8: Separation of diastereoisomers depending on ethanol percentage. Other
conditions as in Figure 6.
5,5
5
4,5
y=1.4467x+2.5637
R2=0.9982
log A
4
3,5
3
y=1.5558x-1,3216
R2=0.9977
y=1.7888x-0.6206
R2=0.9997
y=1.8468x-0.5279
R2=0.9995
2,5
2
y=1.904x-0.0044
R2=0.9981
1,5
1
0.6
0.8
1
1.2
1.4
1.6
1.8
log C
Figure 9: Log A vs log C for different mobile phases in HPLC and SFC. Column: Synergi Fusion RP. Black triangles: methanol–water; green circles: acetonitrile–water;
red squares: ethanol–water; blue diamonds: SFC at 1 mL/min (90:10 carbon dioxide–
methanol); pink diamonds: SFC at 3 mL/min. [AUTHOR: Mobile phase correct for SFC
at 1 mL/min?]
ber of droplets that can enter the drift
evaporative tube. Nonetheless, this equation describes the primary droplet size
distribution (the distribution obtained
just after the nebulizer), whereas the
measured response is that of the ternary
distribution (after evaporation and loss
of larger droplets by impaction) (24,29),
limiting the relevance of this equation
to describe the phenomena encountered. Moreover, this equation does not
take into account the flow conditions,
which are more often turbulent than
laminar (29). [AUTHOR: Meaning OK
in preceding sentence?] Consequently,
several works report the poor calcula-
tion of the droplet size distribution from
this equation in some cases (30). In particular, investigating the effect of a flow
rate increase on the droplet size, it was
observed that the droplets were smaller
than estimated based on the equation
(31).
Whatever the cause, this decrease is
observed in packed-column SFC, where
the total liquid flow rate entering the
nebulizer is 0.2–0.5 mL/min (the mobile
phase was 90:10 [v/v] carbon dioxide–
ethanol, 2–5 mL/min). The fluid depressurization induces a cooling effect, which
increases with the flow-rate increase. As
a result, the condensation of droplets
increases, meaning that the amount of
compound going through the light beam
decreases.
Figure 6 shows the response variation
for a diastereoisomer separation at two
mobile-phase flow rates. As expected, for
the two signals, the retention and peak
width are lower, and the height of the
peak is quite constant with UV. However,
for the ELSD response, both the peak
height and area are dramatically reduced
for the higher flow rate, suggesting a
strong modification in the droplet size
distribution. Figure 7 shows the separation and detection of various pharmaceutical compounds in carbon dioxide–ethanol mobile phase. Theophylline, which
is included in this set of compounds, displays a log P equal to –0.32, explaining
why this compound is often studied by
hydrophilic interaction chromatography
(HILIC) (32–34). The other compounds
display higher log P values (1.16 for dexamethasone, 1.20 for cortisone, and 1.66
for hydrocortisone) (35). The separation
of these four compounds is achieved in
carbon dioxide–ethanol mobile phase
without any additives (acidic or basic),
with good peak symmetry. The response
of at least three compounds (cortisone,
hydrocortisone, and dexamethasone) is
higher with ELSD detection than with
UV detection, regardless of the flow rate
used, 3 or 5 mL/min.
As expected, the peak intensity
decreases with ELSD when increasing the mobile phase flow rate, but the
ELSD response is still higher than the
UV response, despite the very low wavelength used (210 nm) with the SFC
mobile phase. The amount of organic
solvent added to carbon dioxide was also
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MARCH 2012 LCGC NORTH AMERICA VOLUME 30 NUMBER 3
3.0000
y=0.4514x+2.063
R2=0.9847
2.5000
b
2.0000
y=0.4705x+2.098
R2=0.9184
y=0.5381x+3.6099
R2=0.6742
1.5000
y=0.5584x+1.4152
R2=0.9201
1.0000
-2.000
-1.000
0.000
1.000
2.000
3.000
4.000
5.000
6.000
Log a
Figure 10: Log b vs. log a. Blue diamonds: 14 compounds in SFC; red squares: tricaprylin in nonaqueous reversed-phase HPLC with acetonitrile–dichloromethane mobile
phase with different organic postcolumn additions (data from reference 39); pink
crosses: ceramides by direct injection in pure organic solvents (data from reference
16); green triangles: neomycin in HPLC with different aqueous mobile phases (data
from reference 43).
studied (3–20% ethanol).
As reported previously, the mobilephase composition induces response
changes, both in HPLC (9) and SFC
(10), leading to the use of an additional
inverse gradient to maintain a constant
response (10). The use of organic solvent is reported to shift the droplet size
toward smaller values (36).
Figure 8 shows that the increase in ethanol favors the compound elution (diastereoisomers), but dramatically reduces
their ELSD response. This means that
isocratic conditions should be preferred
for SFC–ELSD and that the stationary
phase should be carefully selected to
allow good separation with the smallest
modifier proportion. Classifications of
stationary phases in SFC favoring this
choice are available (37,38).
To compare the HPLC and SFC
responses, studies were carried out for
caffeine with different mobile phases
(methanol–water, ethanol–water, acetontrile–water, and carbon dioxide–ethanol), having close eluting power to maintain identical retention factors (k).
With all mobile phases, the column
provided symmetrical peaks. Figure 9
shows a log–log plot of peak area versus
concentration for these mobile phases.
Two flow rates (3 and 1 mL/min) were
studied in SFC. Satisfactory linearity is
reported up to 50 ppm in all cases (log–
log coordinates). The response increases
from methanol–water to acetonitrile–
water, and ethanol–water, then SFC at
3 mL/min. The response is multiplied
by three from methanol to acetonitrile
or ethanol in HPLC, and by three again
from acetonitrile or ethanol in HPLC
to SFC with 10% ethanol (3 mL/min).
Moreover, at 1 mL/min, the signal is dramatically higher in SFC. The b coefficient
regularly decreases in the order methano
l<ethanol<acetontrile<SFC at 1 mL/min.
Numerous studies report that this coefficient is related to the droplet size (see
ref in 39) [Author: are you pointing to
a specific reference within reference 39?
If so, please indicate which one(s)]. The
higher the value of b, the lower the droplet size. Does that mean that in SFC, as
a result of the lower b value, the droplets
are bigger? Another study reported the
reverse effect in packed-capillary SFC by
using 2-propanol as modifier (39). However, the use of capillary columns, that
is, of very low flow rates and injected
volumes, seems to affect the response
7
significantly because of the direct linear
relationships between the peak area and
the concentration observed in such conditions (8,40–42).
Whatever the reasons, the peak area
in SFC is dramatically improved. Lower
droplet condensation is observed in SFC
conditions because of the lower amount
of liquid in the mobile phases (10% for
our studies), apparently favoring the
transfer of analyte from the nebulizer to
the drift evaporative tube.
The difference observed for the two
flow rates in SFC could be a result of
varied cooling effects of the nebulization chamber — greater at higher flow
rates — which induces a greater droplet
condensation on the wall (the overall signal decreases from 1 to 3 mL/min) and a
larger droplet size of the ternary aerosol,
which explains the lower b value at 1 mL/
min.
Finally, there is an experimental linear correlation in HPLC between the
two coefficients, b and log a (24). Figure
10 shows this correlation for 14 varied
compounds in SFC: palmitic and linolenic acid, tripalmitoyl- and trilinonenoylglycerol, cholesterol, hexadecanol,
octadecanol, eicosanol, docosanol, theophylline, ketoprofen, hydrocortisone,
caffeine, and 4-hydroxybutylparaben. A
linear relationship is observed in SFC
with 90:10 (v/v) carbon dioxide–ethanol
mobile phase (blue diamonds). Furthermore, other data obtained in HPLC were
added to Figure 10. With a Sedere 75
detector in a nonaqueous reversed-phase
LC separation (acetontrile–dichloromethane) (39), the values for one compound (tricaprylin) with different postcolumn addition (red squares) are very
close to the values obtained in SFC with
various compounds. The slopes of the
tendency curves are also very close for
direct injection of ceramide with various pure organic solvents (pink line) (26)
and for HPLC analysis of neomycin with
aqueous mobile phases with a Sedere
75 detector (green line) (43). The main
differences are noticed on the intercept,
which appears to be strongly improved
with aqueous mobile phases and lowered
with direct injection in pure organic solvents.
Conclusion
The use of ELSD with SFC is favored by
8
LCGC NORTH AMERICA VOLUME 30 NUMBER 3 MARCH 2012
the nature of the mobile phase in SFC,
which enables aerosol formation and thus
improves the peak area, at least for the
carbon dioxide–ethanol mixture. The b
coefficient is smaller, possibly indicating that the particle size is greater. Conversely, the log a value is greater, explaining the higher response obtained in SFC
conditions. From the numerous analytical parameters studied, the mobile-phase
flow rate and the amount of modifier
mixed with carbon dioxide are the main
parameters affecting peak area. The outlet pressure also plays a role in response
by affecting the speed of fluid in the nebulizer. Finally, these studies show that
using a heated back-pressure regulator,
the slightly modified nebulizer chamber
of the Sedere 85 is well suited for SFC
analysis.
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E.Lesellier and C. West are with the Institut de Chimie Organique et Analytique, at
the Université d’Orléans in Orléans, France.
T. Bizet, A. Valarché, and M. Dreux are
with Sedere in Orléans, France.
For more information on this topic,
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