36
March 2015 Volume 18 Number 1 www.chromatographyonline.com LC TROUBLESHOOTING Identifying the causes of method failure GC CONNECTIONS GC ovens COLUMN WATCH The possibilities of SFC Principles, advantages, and potential problems Translating Methods from HPLC to UHPLC

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March 2015

Volume 18 Number 1

www.chromatographyonline.com

LC TROUBLESHOOTING

Identifying the causes of method

failure

GC CONNECTIONS

GC ovens

COLUMN WATCH

The possibilities of SFC

Principles, advantages, and potential problems

Translating Methods from HPLC to UHPLC

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T O M A K E

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3

Editorial P olicy:

All articles submitted to LC•GC Asia Pacific

are subject to a peer-review process in association

with the magazine’s Editorial Advisory Board.

Cover:

Original materials: traffic_analyzer/Getty Images

Columns17 LC TROUBLESHOOTING

Listen to the Data

John W. Dolan

A stepwise process is described to help isolate and identify the

cause of a method failure.

22 GC CONNECTIONS

Gas Chromatography Ovens

John V. Hinshaw

The transit of peaks through a gas chromatography (GC) column

depends strongly on the thermal profile they encounter on the way.

Gas chromatographers primarily rely on the classic hot-air-bath

type of oven, but several alternatives are also in use. This

instalment examines ovens for GC in several forms plus how oven

thermals affect peak retention behaviour.

27 COLUMN WATCH

Modern Supercritical Fluid Chromatography — Possibilities

and Pitfalls

Torgny Fornstedt and Ronald E. Majors

There has been a revival of supercritical fluid chromatography

(SFC) in recent years, especially in the chiral preparative field,

but also more recently in the analytical area. However, SFC is

considerably more complex than liquid chromatography (LC),

mainly because of the compressibility of the mobile phase. One

can say that SFC is a “rubber variant” of LC where everything

considered constant in LC varies in SFC. In this review, we

go through advances in theory, instrumentation, and novel

applications.

Departments33 Events

34 Application Notes

COVER STORY 6 Translations Between Differing Liquid Chromatography

Formats: Advantages, Principles, and Possible

Pitfalls

Patrik Petersson, Melvin R. Euerby,

and Matthew A. James

The numerous advantages of

translating gradient chromatographic

methods between the differing

formats of LC have been explored

and discussed. While translations

in principle obey well defined

chromatographic theories, the authors

investigate a number of potential pitfalls

that may result in poor translations as

exhibited by selectivity differences,

changes in efficiency, and hence failure to

meet resolution system suitability criteria.

March | 2015

Volume 18 Number 1

www.chromatographyonline.com

ES572943_LCA0315_003.pgs 02.20.2015 22:25 ADV blackyellowmagentacyan

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4 LC•GC Asia Pacific March 2015

The Publishers of LC•GC Asia Pacific would like to thank the members of the Editorial Advisory Board

for their continuing support and expert advice. The high standards and editorial quality associated with

LC•GC Asia Pacific are maintained largely through the tireless efforts of these individuals.

LCGC Asia Pacific provides troubleshooting information and application solutions on all aspects

of separation science so that laboratory-based analytical chemists can enhance their practical

knowledge to gain competitive advantage. Our scientific quality and commercial objectivity provide

readers with the tools necessary to deal with real-world analysis issues, thereby increasing their

efficiency, productivity and value to their employer.

Editorial Advisory Board

Kevin AltriaGlaxoSmithKline, Harlow, Essex, UK

Daniel W. ArmstrongUniversity of Texas, Arlington, Texas, USA

Michael P. BaloghWaters Corp., Milford, Massachusetts, USA

Brian A. BidlingmeyerAgilent Technologies, Wilmington,

Delaware, USA

Günther K. BonnInstitute of Analytical Chemistry and

Radiochemistry, University of Innsbruck,

Austria

Peter CarrDepartment of Chemistry, University

of Minnesota, Minneapolis, Minnesota, USA

Jean-Pierre ChervetAntec Leyden, Zoeterwoude, The

Netherlands

Jan H. ChristensenDepartment of Plant and Environmental

Sciences, University of Copenhagen,

Copenhagen, Denmark

Danilo CorradiniIstituto di Cromatografia del CNR, Rome,

Italy

Hernan J. CortesH.J. Cortes Consulting,

Midland, Michigan, USA

Gert DesmetTransport Modelling and Analytical

Separation Science, Vrije Universiteit,

Brussels, Belgium

John W. DolanLC Resources, Walnut Creek, California,

USA

Roy EksteenSigma-Aldrich/Supelco, Bellefonte,

Pennsylvania, USA

Anthony F. FellPharmaceutical Chemistry,

University of Bradford, Bradford, UK

Attila FelingerProfessor of Chemistry, Department of

Analytical and Environmental Chemistry,

University of Pécs, Pécs, Hungary

Francesco GasparriniDipartimento di Studi di Chimica e

Tecnologia delle Sostanze Biologica-

mente Attive, Università “La Sapienza”,

Rome, Italy

Joseph L. GlajchMomenta Pharmaceuticals, Cambridge,

Massachusetts, USA

Jun HaginakaSchool of Pharmacy and Pharmaceutical

Sciences, Mukogawa Women’s

University, Nishinomiya, Japan

Javier Hernández-BorgesDepartment of Analytical Chemistry,

Nutrition and Food Science University of

Laguna, Canary Islands, Spain

John V. HinshawServeron Corp., Hillsboro, Oregon, USA

Tuulia HyötyläinenVVT Technical Research of Finland,

Finland

Hans-Gerd JanssenVan’t Hoff Institute for the Molecular

Sciences, Amsterdam, The Netherlands

Kiyokatsu JinnoSchool of Materials Sciences, Toyohasi

University of Technology, Japan

Huba KalászSemmelweis University of Medicine,

Budapest, Hungary

Hian Kee LeeNational University of Singapore,

Singapore

Wolfgang LindnerInstitute of Analytical Chemistry,

University of Vienna, Austria

Henk LingemanFaculteit der Scheikunde, Free University,

Amsterdam, The Netherlands

Tom LynchBP Technology Centre, Pangbourne, UK

Ronald E. MajorsAgilent Technologies,

Wilmington, Delaware, USA

Phillip MarriotMonash University, School of Chemistry,

Victoria, Australia

David McCalleyDepartment of Applied Sciences,

University of West of England, Bristol, UK

Robert D. McDowallMcDowall Consulting, Bromley, Kent, UK

Mary Ellen McNallyDuPont Crop Protection,Newark,

Delaware, USA

Imre MolnárMolnar Research Institute, Berlin, Germany

Luigi MondelloDipartimento Farmaco-chimico, Facoltà

di Farmacia, Università di Messina,

Messina, Italy

Peter MyersDepartment of Chemistry,

University of Liverpool, Liverpool, UK

Janusz PawliszynDepartment of Chemistry, University of

Waterloo, Ontario, Canada

Colin PooleWayne State University, Detroit,

Michigan, USA

Fred E. RegnierDepartment of Biochemistry, Purdue

University, West Lafayette, Indiana, USA

Harald RitchieTrajan Scientific and Medical. Milton

Keynes, UK

Pat SandraResearch Institute for Chromatography,

Kortrijk, Belgium

Peter SchoenmakersDepartment of Chemical Engineering,

Universiteit van Amsterdam, Amsterdam,

The Netherlands

Robert ShellieAustralian Centre for Research on

Separation Science (ACROSS), University

of Tasmania, Hobart, Australia

Yvan Vander HeydenVrije Universiteit Brussel,

Brussels, Belgium

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resolution, while reducing the gradient analysis time by 50%

(same velocity typically used for large molecules) to 70% (higher

velocity typically used for small molecules) and substantially

increasing productivity. This approach is vitally important for

the analysis of increasingly larger numbers of samples (that

is, to better describe a process or formulation performance),

increased utilization of instruments, the analysis of labile

samples, and rapid at-line analysis (that is, process analytical

technology).

A compromise between the approaches of increased

resolution and speed of analysis has been the use of 100-mm

columns with sub-2-µm particles, which results in a 60%

reduction in gradient time and an approximate 10% increase in

resolution for small molecules.

Reduced Solvent Consumption: Converting a standard

HPLC method that uses a 150 mm × 4.6 mm, 3–3.5 µm

column to a 100 mm × 2.1 mm, 1.7-µm or 100 mm × 1.0 mm,

1.7-µm column in theory offers a possible reduction in solvent

consumption of approximately 86% to 97%. In practice, it is less

often because of the necessity to prime the LC lines. During a

global implementation of UHPLC within AstraZeneca (during the

period of 2007–2010) involving 41 UHPLC systems, a reduction

in solvent consumption of 63% was realized compared to the

theoretical reduction of 77% (9).

KEY POINTS• Translations between differing formats of liquid

chromatography (LC) obey well-defined theories.

• Typically translations work very well.

• There are potential pitfalls that result in changes in

selectivity or poor efficiency, but these can in most

cases be addressed.

As a result of the introduction of commercially available

sub-2-µm porous particles (1), sub-2-µm, 3-µm, and 5-µm

superficially porous (2,3) particles, and ultrahigh-pressure

liquid chromatography (UHPLC) instrumentation (4,5) from

2004 onwards, there has been an increasing interest in the

ability to perform accurate translations between different

liquid chromatography (LC) formats. An example would be

translating between 150 mm × 4.6 mm, 5-µm dp formats on

standard high performance liquid chromatography (HPLC)

systems and 50 mm × 2.1 mm, sub-2-µm formats on UHPLC

systems while maintaining the same resolution. The findings

of a recent survey of major chromatographic users predicted

that the use of standard HPLC systems is expected to steadily

decline from 2011 to 2015 with a concomitantly higher usage

and purchase of UHPLC systems predicted over the same

time frame (6).

There are a plethora of reasons for this shift in LC format

usage and purchase, all of which are based on sound

chromatographic theory (5,7,8). From the extensive experience

of the authors within the pharmaceutical industry, the major

drivers for this shift appear to be increased productivity

(that is, reduced analysis time) coupled with minimal loss of

information quality or an increased quality of data with no loss of

productivity.

Advantages and DriversIncreased Resolution: Reduction of the packing material

particle size by a factor of two (that is, substitution of 3–3.5 µm

particles by 1.7-µm particles), while keeping other operation

factors constant, should result in an increase of resolution of

approximately 30–40%.

Speed of Analysis: A reduction in column length (L) and

particle size (dp) while keeping the L/dp ratio constant (for

example, substitution of a 150-mm column with 3–3.5 µm

particles for a 75-mm column with 1.7-µm particles) should

maintain the same chromatographic efficiency and hence

Translations Between Differing Liquid Chromatography Formats: Advantages, Principles, and Possible Pitfalls Patrik Petersson1, Melvin R. Euerby2,3, and Matthew A. James3, 1Novo Nordisk A/S, Måløv, Denmark, 2Strathclyde Institute

of Pharmacy and Biomedical Sciences, University of Strathclyde, Glasgow, UK, 3Hichrom Ltd, Berkshire, UK.

The numerous advantages of translating gradient chromatographic methods between the differing formats of liquid chromatography (LC) have been explored and discussed. Although translations in principle obey well-defi ned chromatographic theories, the authors investigate a number of potential pitfalls that may result in poor translations as exhibited by selectivity differences, changes in efficiency, and hence failure to meet resolution system suitability criteria. The consequences of these pitfalls are examined and the regulatory implications of method translation are explored.

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6 LC•GC Asia Pacià c March 2015

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Ease of Method Transfer: Within many industries it is often standard practice to transfer the chromatographic testing from the research and development (R&D) laboratory to a contract research organization (CRO), operation, or quality control (QC) sites. This method transfer exercise can be made even more problematic because it is now quite common for many R&D departments to develop only UHPLC methods. However, not all receiving laboratories have sufficient UHPLC capacity or experience and, thus, method translations become necessary. The reverse of this is becoming true in that QC laboratories, which have moved predominantly to UHPLC, may have to use UHPLC methods for the analysis of legacy products or methods that use HPLC columns.Increased Instrument Utilization: The drive for increased productivity and efficiency has necessitated an increased flexibility and utilization of available instrumentation. Many companies have a rolling programme to replace their worn out HPLC systems with a reduced number of UHPLC systems capable of running LC methods based on both 5-µm and sub-2-µm particles. In addition, valve arrangements are used that allow queuing of both HPLC and UHPLC methods on the

same LC system, hence a reduced number of LC systems allow continuous operation.

Principles of Method TranslationBecause many translation guides successfully describe translations of isocratic LC methodologies (10), this article will focus entirely on the translation of gradient LC methodologies, which can be more difficult to perform. In theory, the translation required to maintain the chromatographic selectivity and performance of either an isocratic or gradient separation is very simple (7,11). The additional consideration that has to be accounted for in gradient separations is that a constant ratio must be maintained between the volume of each segment in the gradient over the column dead volume (8,12–15). After the introduction of sub-2-µm particles and UHPLC in the mid-2000s, several articles were published that focused exclusively on translations between 4.6- and 2.1-mm i.d. columns (7,8,10,16–18). To assist the practicing chromatographer in all types of translations, several commercial and academic computer applications have been developed (19); however, although these computer applications undoubtedly aid chromatographers, they all possess certain drawbacks to successful method translation.

In contrast to previous publications, this article only briefly describes the underlying theory and equations relating to chromatographic method translation principles (readers are encouraged to see the sidebar “Theory for Translations” for more information). Instead, this article will focus on how to

8 LC•GC Asia Paciàc March 2015

Petersson et al.

(a)

(b)

1 tR 0.53 min

2 3 4 5

6 7

8

9 tR 1.95 min

3 4 7

8

9 tR 2.80 min

1 tR 0.53 min

(c)

3 4 7

8

9 tR 2.77 min

1 tR 1.37 min

Figure 1: An illustration of how a larger VD/VM for the translated method can be compensated using a delayed sample injection (Δ negative). The data also illustrates how VD/VM differences can affect the selectivity. The chromatograms have been scaled by alignment of the first and last eluted peaks. (a) binary model 1290 Agilent system, VD/VM = 1.8, injection in mainpass; (b) quaternary model 1290 Agilent system, no correction, VD/VM = 9.0, injection in mainpass; (c) quaternary model 1290 Agilent system, 0.93-min injection delay, VD/VM = 8.2, injection in bypass. Other conditions for (a)–(c): column: 50 mm × 2.1 mm, 1.8-µm dp; flow rate: 0.75 mL/min; mobile-phase A = 0.1% formic acid in water; mobile-phase B = 0.1% formic acid in acetonitrile; gradient: 5–27% B in 2 min; temperature: 40 °C. Peaks: 1 = paracetamol, 2 = 4-hydroxybenzoic acid, 3 = caffeine, 4 = 3-hydroxybenzoic acid, 5 = salicylamide, 6 = acetanilide, 7 = aspirin, 8 = salicylic acid, 9 = phenacetin.

0.00 2.00 4.00 6.00 8.00 10.00 12.00 14.00 16.00 18.00 20.00 22.00 24.00

4+5

1+2

3 6 7

8 9

10

11

5

1+2

3 6 7

8 9 10

11

4

(a)

(b)

Time (min)

Figure 2: An illustration of how a translation from one column to another may affect both retention and selectivity if the translation is incorrectly performed (that is, assuming equal porosity between materials). Conditions: (a) Column: 150 mm × 2.1 mm, 3.6-µm dp, 3.2 µm dcore, VM = 0.27 mL, 200-Å superficially porous particle Aeris widepore XB-C18; flow rate: 0.3 mL/min; gradient: 27–65% B in 30 min; mobile-phase A: 0.1% trifluoroacetic acid in water; mobile-phase B: 0.08% trifluoroacetic acid in acetonitrile; temperature: 40 °C. Conditions (b): Gradient scaled assuming the same porosity as for 300 Å porous particles, that is, VM = 0.38 mL and a gradient time of 41.8 min. Other conditions same as (a). Sample: proteins with pI ranging from 3.6 to 9.3 (Sigma-Aldrich I3018 IEF mix 3.6–9.3).

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The whole is more than the sum of its parts – the value of 2 dimensions by PSS.

Thinking Forward.

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perform successful translations of gradient chromatographic methods between HPLC and UHPLC systems, the accuracy that can be expected, and the potential pitfalls that chromatographers must be aware of and how to successfully avoid them. If the necessary precautions are taken, it is the experience of the authors that gradient translations work extremely well. For example, 11 LC methods were translated to or from UHPLC within AstraZeneca; the maximum deviations in relative retention times were only between 0.02 and 0.05, which was deemed acceptable (9,18).

ExperimentalExperimental work was performed on Agilent 1100, 1260, and 1290 LC systems of which the dwell volume and system volumes had been previously well characterized. Any experimental data including the injector programmes used can be supplied by the authors on request. For the delayed injection work on the Agilent LC systems, the injector must be in the bypass mode (that is, no flow through the injector). After the calculated delay time, the flow was returned to the mainpass position (that is, flow through the injector), then after a predefined time (time = [5 × [injection volume + 5]]/flow rate) to flush the sample onto the column, the flow was returned to the bypass position. At the top of the gradient the flow was returned to the mainpass position to wash the injector

with the mobile phase to avoid carryover and subsequently flush the injector with the starting mobile phase composition prior to the next injection. Zorbax Eclipse XDB C18 columns (Agilent Technologies) of 1.8-, 3.5-, and 5-µm particle sizes were selected for the small molecule work because they exhibit a good scalability with respect to efficiency and particle size (R2 = 0.9 for N versus 1/dp) (20).

Translations were made using a Microsoft Excel spreadsheet and the equations described in the sidebar “Theory for Translations.” A corresponding software application for these types of translations is now freely accessible at the ACD/Labs website (21). In addition, a more complete set of translation tools is included in version 2014 of the ACD/Chrom Workbook software (22).

Potential Pitfalls in Method TranslationsObserved Selectivity Anomalies as a Result of Differences

in Dwell Volume: The system dwell volume (VD) is defined as the volume from the point where the two solvents A and B first meet to the inlet of the column. For accurate translation of gradient methods it is of critical importance that the ratio between the dwell and dead volume (VM) is kept constant; that is, the difference in ratio between the system dwell volume and the column dead volume needs to be negligible (Δ = [VD/VM]

original – [VD/VM]new must approach 0). If this is not the case, then

Theory for TranslationsIn theory a volumetric translation of a chromatographic method is simply a matter of keeping the ratio between the volume of each segment in the gradient and the column dead volume constant

tG1iF1

=V

M1

tG2iF2

VM2

[1]

where subscript 1 corresponds to the method being translated, subscript 2 the translated method, tGi the time for segment i in the gradient, F is the flow rate, and VM the column dead volume (12–15). The dead volume can be measured by injecting a dead time marker such as uracil or thiourea for reversed-phase LC. This step is strongly recommended to get an accurate translation. The dead volume can also be estimated by the following approximation:

VM≈π Lε

pp

d

2

2

[2]

where d is the internal diameter of the column, L the length of the column, and εpp is the porosity of the column (typically ~0.6 for 100 Å porous particles).

In previous publications and software related to translations, it is assumed that the porosity of the columns is the same

and VM in equation 1 can be replaced with d2L. However, when translating between a porous and a superficially porous particle it is unacceptable since the dead volume is reduced by the solid core of the latter. Differences in porosity will result in inaccurately scaled gradient times. For example, when translating from a porous particle to a superficially porous wide pore material the error in gradient time will be 36% (for the Aeris phase, dp = 3.6 µm and dcore = 3.2 µm).

Based on the knowledge of the diameter of the particle (dp) and the solid core (dcore) it is possible to estimate the porosity of the column packed with superficially porous particles.

εspp

= (xinter

+x intra

)εpp [3]

xinter

=

π

61– [4]

xintra

=– d 3

core)π(d 3

p

6d 3p

[5]

where xintra and xintra are the fraction of the dead volume corresponding to inter- and intraparticle volume of mobile phase, respectively.

Since the porosity of columns packed with porous particles varies significantly, up to ±28% as described in the text, it is necessary to use experimentally

determined dead volumes to obtain accurate translations.

The flow rate is often scaled against column internal diameter to obtain the same linear velocity for columns with the same porosity.

F2=

F1d 2

2

d 21

[6]

UHPLC is usually operated at higher linear velocities than HPLC because of the more favourable van Deemter curves. Thus, going from HPLC to UHPLC requires a flow higher than the scaled flow and vice versa. To translate to a flow rate scaled for another particle size, the reduced interstitial linear velocity (43) should be kept constant. This can be achieved by a scaling based on the following equation:

F2=

F1d

p1d 2

2

dp2

d 21

[7]

Translating flow rates, however, is difficult for superficially porous particles since both the A term and the C term in the van Deemter equation are smaller than for porous particles with the same diameter. In addition, it should not be assumed that the original method is running at an optimal flow rate. To make a translation to a truly optimal flow rate it is therefore recommended to translate

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differences in chromatographic selectivity and relative retention

time shifts may be observed. One such example is shown in

Figure 1, where a series of analgesic related drugs have been

chromatographed on the same 50 mm × 2.1 mm, 1.8-µm dp

column using a binary high-pressure mixing system with low

dwell volume (that is, 202 µL) and a quaternary low-pressure

mixing system with a higher dwell volume (that is, 990 µL). Note

that in this example a translation from a system with VD/VM = 1.8

(Figure 1[a]) to a system with VD/VM = 9 (Figure 1[b]) resulted in

coelution (peaks 7 and 8) as well as a reversal of elution order

(peaks 3 and 4).

To compensate for a larger VD/VM on the translated method

(that is, Δ = [VD/VM]original – [VD/VM]new = negative), the gradient

must be started before injecting the sample — so-called

injection delay or pre-injection volume — which can be easily

implemented on certain LC systems (such as the Agilent 1290

or the Waters Acquity H-class systems). Equations 9 and 10 in

the sidebar describe this process in detail. It should be noted

that it is only necessary to determine the VD (23) once for a

certain LC configuration. Figure 1 illustrates how the injection

delay principle can be used to compensate for VD differences

and thereby maintain the original selectivity and relative retention

(Figure 1[a] versus 1[c]).

To compensate for a smaller VD/VM on the translated method

(that is, Δ = [VD/VM]original – [VD/VM]new = positive) the translated

gradient must possess an isocratic hold before commencing

the gradient.

A small VD/VM results in a gradient with sharp changes

(a Z-shaped gradient), whereas larger VD/VM will result in

smoother, more S-shaped changes. This difference in gradient

shape may also result in selectivity changes, mainly for fast

separations on short columns (for example, 2-min gradients

on 50 mm × 2.1 mm columns). To address this problem with

possible selectivity changes, Agilent Technologies developed

an approach (24) in which the company’s model 1290 UHPLC

systems can mimic the gradient shape of systems with a larger

system dwell volume.

Observed Selectivity Anomalies as a Result of Incorrect

Dead Volume Estimation: The column dead volume is

a fundamental parameter that has a significant impact on

translations and their subsequent accuracy (equations 1, 9–13

in the sidebar). To the best of our knowledge, all available

translation applications erroneously assume an equal porosity

for all stationary phases irrespective of their nature (equation

2 in the sidebar). In cases where this assumption is not valid,

significant errors in translated gradient times are possible.

For example, large differences in porosity and hence dead

volume can be expected and observed between porous and

superficially porous particles (that is, 10–29% difference was

observed for seven different types of superficially porous

to a series of flow rates using equation 1

and thereby determine the optimal flow

experimentally.

An approximate estimation of the

maximal pressure for the translated

method can be determined based on a

pressure reading of the maximal pressure

for the original method. Maximal pressure

is obtained at approximately 20% (v/v)

acetonitrile or 50% (v/v) methanol in

water. It should be noted, however, that

this estimate may be unreliable since

both packing procedures and particle

size distributions differ between columns

and vendors (20). Furthermore, the

system’s contribution to the pressure

also differs.

Δp2=

Δp1d 2

1d 2

p1 F

2L

2

d 22 d 2

p2F

1L

1

[8]

For an accurate scaling it is of critical

importance that the ratio between dwell

and dead volume is kept constant; that

is, the difference in ratio between the

system’s dwell volume and the column

dead volume needs to be negligible.

VD1

– =ΔV

M1

VD2

VM2

[9]

where VD is the system dwell volume

and Δ the difference in dwell and dead

volume ratio between the systems.

The dwell volume for an HPLC system

is typically 1–2 mL and for a UHPLC

system it is 0.1–0.5 mL depending

on configuration and model. For an

accurate translation it is recommended

to measure (23) the dwell volume (only

necessary once for a certain instrument

model and configuration).

If Δ is positive, it is necessary to

introduce an initial isocratic step of z min

to the translated method corresponding

to

z =∣Δ∣

VM2

F2

[10]

If Δ is negative, it is necessary to start

the gradient z min before the sample is

injected, a function available in certain

chromatographic data systems. A delayed

injection after the start of the gradient

can be easily implemented on certain

LC systems (such as the Waters Acquity

H-class system or the Agilent 1290

system). Another alternative that partially

solves the problem is to use a larger

column internal diameter (equation 9).

If the translated method is not

corrected for, it may display different

relative retention times and potentially

also different selectivity. The injection

volume is scaled against the dead

volume to obtain the same relative

amount on column.

Vinj2=

Vinj1V

M2

VM1

[11]

Because of the higher efficiency

of sub-2-µm and superficially porous

columns, asymmetry will be higher for

overloaded peaks due to the higher

concentration at peak apex. This can

be compensated for by a scaling

against the number of plates for a

nonoverloaded peak chromatographed

under isocratic conditions.

V ′inj2=

Vinj1

N1V

M2

N2V

M1

[12]

For porous particles the efficiency

is proportional to the ratio of column

length or particle size. Thus, for porous

particles:

V ′inj2≈

Vinj1

L1d

p2V

M2

L2d

p1V

M1

[13]

To minimize poor efficiency for early

peaks it is important to match the

column dead volume with the system’s

contribution to peak volume:

N =V

M (1+k)

σ2col+σ

2ext

√ [14]

where k is the retention factor and σ

is the contribution to the peak volume

from band broadening in column

(σcol) and system (σext) expressed as

standard deviation.

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columns [25] and 13–37% predicted difference according to equations 2–5 in the sidebar). Consequently, translated gradient times may have an error of the same magnitude; for nonporous particles the error will be even greater (that is, 52%).

Equations 2–5 in the sidebar describe how VM can be estimated for columns based on superficially porous particles using their reported particle and core diameters. However, these and other VM estimates are all associated with an error that can be quite substantial. The use of quoted particle sizes may be misleading because there are many differing ways that particle size can be determined and reported (20). The pore size of the particles also affects the porosity (100-Å columns have a porosity of ~0.60, whereas 300-Å columns have a porosity of ~0.75). VM estimations may also be inaccurate because of the fact that columns packed with different particle sizes are often packed with different pressures, which can result in lower porosities for columns designed for UHPLC. Consequently, for columns packed with porous particles, the difference between theoretical and measured dead volumes can be quite substantial. A comparison of 14 brands of modern columns from various vendors packed with porous particles exhibited a dead volume prediction error of ±28% (25). This value corresponds to an error in gradient time of up to 28%. Figure 2 exemplifies how a 29% error in VM can affect retention time as well as chromatographic selectivity.

Figure 2(a) demonstrates the experimental chromatogram derived by using a 200-Å superficially porous material with a dp and dcore of 3.6 µm and 3.2 µm, respectively, with a measured VM for the column of 0.27 mL. In comparison, when the methodology is translated using the same column (to eliminate any stationary-phase selectivity differences), but assuming that it is 300 Å and fully porous in nature, the VM is calculated as 0.38 mL and the new gradient yields a significant change in selectivity (see Figure 2[b]).

Given the above discussion, the authors strongly recommend that VM values are experimentally determined to obtain accurate translations. VM can be easily determined by injecting a reversed-phase-LC dead time marker such as uracil or thiourea.Observed Selectivity and Peak Width Anomalies as a

Result of Differences in Column Thermostat Design

Between LC Instrumentation: Differences in column thermostat design used by differing LC instrument vendors will result in different temperatures being achieved within the column despite identical “set-point and feedback” temperatures being recorded in the column compartment. The extent of this temperature deviation is dependent on instrument design, flow rate, and temperature set point. According to our experience, deviations of 5 °C or more are commonplace (25). This degree of temperature difference is sufficient to cause significant selectivity differences when transferring a method from one type of LC instrument to another. Consequently, when translating from HPLC to UHPLC or transferring a method from one type of HPLC system to another, it is very likely that observed selectivity differences are related to differences in column temperature.

Column thermostat design affects not only selectivity, but also efficiency. It has been found that a precolumn heat exchanger in combination with a still air column compartment can reduce radial temperature gradients in the column and thereby results in narrower peaks compared to a water bath or a thermostat based on a forced air flow principle (26,27).

To address this problem, we recommend that the system suitability test (SST) section of the method describes how the

resolution is affected by temperature and how corrections can be employed; this description can be achieved, for example, by illustrating chromatograms corresponding to 30 °C, 35 °C, and 40 °C for a method developed on an instrument at 35 °C or by the construction of van ’t Hoff plots (that is, log k versus 1/temperature). By following this procedure, users can see in what direction and approximately how much the temperature

12 LC•GC Asia Paciàc March 2015

Petersson et al.

1

2 3

3

(a)

(b)

(c)

(d)

3+4

3+4

4

4

5

6

78 9

10

11 tR 37.0 min

11 tR 12.9 min

11 tR 12.4 min

11 tR 13.7 min

Figure 3: A translation while maintaining constant linear velocity from an HPLC method based on (a) a 150 mm × 4.6 mm, 5-µm column to the corresponding UHPLC method based on a 50 mm × 2.1 mm × 1.8 µm column (b) without and (c) with dwell volume compensation. The chromatograms have been scaled by alignment of the first and last eluted peaks. (a) binary Agilent 1100 system, VD/VM

= 0.8 (injection in mainpass), 103 bar; (b) binary Agilent 1290 system, no correction, VD/VM = 1.9 (injection in mainpass), 231 bar; (c) binary Agilent 1290 system, 0.12 min injection delay, VD/VM = 1.0 (injection in bypass), 228 bar; (d) as in (b) but with a postcolumn restrictor, 714 bar. Conditions (a): Flow rate: 1 mL/min; gradient: 5–100% B in 40 min; mobile-phase A: 20 mM monobasic potassium phosphate (pH 2.7) in water; mobile-phase B: 20 mM monobasic potassium phosphate (pH 2.7) in 65:35 (v/v) acetonitrile–water; temperature: 40 °C. Conditions for (b), (c), and (d) are the same as (a) except for a gradient time of 13.3 min, a flow of 0.208 mL/min. Peaks: 1 = terbutaline, 2 = N-acetylprocainamide, 3 = phenol, 4 = eserine, 5 = quinoxaline, 6 = quinine, 7 = ARD12495, 8 = diphenhydramine, 9 = carvediol, 10 = amitriptyline, 11 = reserpine.

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needs to be changed to meet the SST acceptance criteria.

This approach is supported by the United States, European,

and Japanese pharmacopeias in that they allow a ±5 °C

adjustment of temperature to obtain the right selectivity

(23,40,44).

Observed Selectivity Anomalies as a Result of Differences

in Heat of Friction: When the mobile phase is depressurized

in the column, frictional heat is generated, resulting in an axial

temperature gradient. The heat generated is proportional to both

the pressure drop over the column, but also the flow has an

impact on heat generation and dissipation (28,29). On a 2.1-mm

i.d. column operated at a pressure close to 1000 bar, the

difference between the column outlet and inlet temperature can

be on the order of 5–10 °C for a 150-mm column and 10–18 °C

for a 50-mm column (28,29).

Selectivity differences caused by heat of friction can

be compensated for by increasing the temperature when

translating from UHPLC to HPLC and thereby compensate

for the reduced heat of friction. Alternatively, the temperature

is decreased to compensate for an increased heat of friction

when translating from HPLC to UHPLC. One approach that is

recommended is to change the temperature ±2 °C, 4 °C, 6 °C,

and 8 °C and thereby investigate if the observed change in

selectivity is related to heat of friction and can be compensated

for (18).

Observed Selectivity Anomalies as a Result of Differences

in Pressure: A change in pressure affects the molar volume of

solvated analytes as well as their degree of ionization (30–34).

This effect typically results in an increased retention as pressure

increases; however, there are exceptions to this rule (34).

Differing degrees of pressure-induced retention changes can

result in either enhanced or reduced chromatographic resolution.

It has been reported that proteins are more sensitive to

pressure-induced retention effects than lower-molecular-weight

analytes because their secondary and tertiary structures are

additionally affected by pressure and flow (35).

The majority of previous studies on pressure-induced

retention effects have been conducted with a postcolumn

restrictor to increase the pressure while maintaining the same

flow rate and do not reflect typical chromatographic conditions.

Furthermore, it has been suggested that heat of friction should

counteract pressure-related retention and selectivity changes

to some extent (28,35). Nevertheless, pressure-related

selectivity differences are also seen during typical

chromatographic conditions and for quite modest differences

in pressure (for example, 142 bar) (36). Figure 3 illustrates

a typical example of a translation from an HPLC method

based on a 150 mm × 4.6 mm, 5-µm column (Figure 3[a])

to a UHPLC method based on a 50 mm × 2.1 mm, 1.8-µm

column (Figure 3[c]) where a pressure increase of only 125 bar

resulted in a significant change in selectivity (peaks 3 and 4).

Unfortunately, it is difficult to compensate for these types of

pressure effects. While it does not provide a solution, adding

a postcolumn restrictor can enable confirmation that pressure

is the cause of the problem (Figure 3[d]). To compensate for

pressure-related selectivity changes, it is probably necessary

to reoptimize the method by adjustments of parameters such

as gradient shape and temperature.

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Poor Efficiency Because of Differences in Extracolumn

Band Broadening Between LC Instrumentation: Efficiency

is dependent on retention as well as the ratio between column

dead volume and the volume of the peak (equation 14 in the

sidebar). Since the dead volume of an HPLC column is typically

much larger than that of an UHPLC column, it is necessary to

reduce the UHPLC instrument’s contribution to peak volume

significantly (7). This extracolumn band broadening (ECBB) —

usually measured as 4σ — is typically in the order of 30–50 µL

and 10 µL for HPLC and UHPLC, respectively. Even the low

volume associated with modern UHPLC instrumentation has

been found to be insufficiently low to compensate completely

for the extracolumn band broadening contribution associated

with peaks of low retention (7,37). This effect is illustrated in

Figure 4, where an isocratic translation from HPLC to UHPLC

exhibited the expected efficiency for late eluted peaks; however,

the efficiency observed for early eluted peaks was significantly

lower. Figure 5 illustrates the efficiency versus the retention factor

for the same separation for other combinations of column and LC

system ECBB volumes. In this example as well as in reference

7, the expected plate numbers are not reached until a retention

factor of approximately 4 is reached when translating to a

50 mm × 2.1 mm column operated on an UHPLC system.

Modifying the ECBB of an LC system is usually quite difficult

(38). A more realistic alternative is to increase the column internal

diameter. Today, 3-mm i.d. UHPLC columns are commercially

available, and they can significantly reduce this problem. The

drawback to this approach is that a flow rate twice as high as

for a 2.1-mm i.d. column must be used, resulting in a reduced

saving in solvent consumption and a potential for increased heat

of friction, which could cause band broadening and selectivity

differences (29).

In general, the minimized ECBB associated with UHPLC

systems is advantageous; however, there is a possibility that

it may cause significant band broadening when performing

HPLC methods with the sample dissolved in a high proportion of

organic solvent compared to the initial mobile phase. This may

appear contradictory, but it can be explained by the narrower

capillaries on the UHPLC system reducing the mixing between

the sample and the mobile phase and thereby reducing peak

focusing of the sample on top of the column. The solution to

this problem is to reduce the sample volume or the amount of

organic solvent in the sample solution. Alternatively, the capillary

between the injection valve and the column can be replaced with

a large internal diameter capillary to increase the mixing.

Differences in Linearity, Response, or Repeatability Related

to Injector Design: Different LC systems possess differing

injection flow principles and materials in their autosampler

construction. For example, in a loop injector the sample is

typically exposed to larger surface areas and other materials

than in a flow through needle injector design. This larger

surface area may result in a more pronounced adsorption and,

consequently, also a more pronounced nonlinear response at

low concentrations for loop injectors.

Other potential problems can be related to differences in the

internal diameter of the injector needle and capillaries. UHPLC

systems have significantly narrower injector needle and capillary

diameters, which can result in poor injection repeatability

because of bubble formation if the draw speed is set too high in

relation to the viscosity of the sample. Another related problem

is that differences in viscosity between samples and standards

because of matrix differences may result in differing amounts

being injected, thereby the sample concentration can be under

or over-estimated.

Consequently, it is important to validate linearity, response,

and repeatability of the LC method when transferring a method

from one type of LC system to another.

Differences in Peak Asymmetry Related to Differences in

Efficiency: The transfer of HPLC methodology to UHPLC when

overloaded peaks are involved results in more-pronounced

14 LC•GC Asia Paciàc March 2015

Petersson et al.

Nu

mb

er

of

theo

reti

cal p

late

s (N

)

Retention factor (k)

20000

18000

16000

14000

12000

10000

8000

6000

4000

2000

00 2 4 6

100 × 2.1 mm, 1.8-μm, ECBB 9 μL

100 × 2.1 mm, 1.8-μm, ECBB 11 μL

100 × 2.1 mm, 1.8-μm, ECBB 23 μL

150 × 4.6 mm, 3.5-μm, ECBB 9 μL

150 × 4.6 mm, 3.5-μm, ECBB 11 μL

150 × 4.6 mm, 3.5-μm, ECBB 23 μL

250 × 4.6 mm, 5-μm, ECBB 23 μL

Figure 5: Number of theoretical plates versus retention factor

for the separations shown in Figure 4 and for five additional

combinations of columns and LC systems with different ECBB

contributions.

(a)

1

k = 0.1

N = 8727

3

k = 1.3

N = 13,294

4

k = 3.4

N = 14,971

5

k = 5.6

N = 17,707

tR = 17.3 min

k = 0.1

N = 3602

k = 1.4

N = 8571

k = 3.9

N = 17,108 k = 6.4

N = 18,699

tR = 7.7 min

(b)

2

Figure 4: An isocratic translation from (a) a 250 mm × 4.6 mm,

5-µm column and a binary Agilent 1100 HPLC system to (b) a

100 mm × 2.1 mm, 1.8-µm column and a quaternary Agilent

1290 UHPLC system, showing how ECBB becomes critical for

peaks with low retention when using columns with small dead

volumes. The chromatograms have been scaled by alignment

of the first and last eluted peaks. Flow rate (a): 1.0 mL/min;

flow rate (b): 0.21 mL/min; mobile phase: 2:400:600 (v/v/v)

phosphoric acid 85% w/v–acetonitrile–water; temperature:

22 °C. Peaks: 1 = 4-hydroxybenzoic acid, 2 = acetylsalicyclic

acid, 3 = salicylic acid, 4 = acetylsalicylsalicylic acid,

5 = salsalate.

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peak asymmetries being observed even

if injection volumes have been correctly

scaled against column volume. The

explanation for this phenomenon is that

the higher efficiency associated with

the UHPLC method results in higher

concentrations of the analyte at the apex

of the peak and thus a higher degree of

overloading is observed (39). Despite

this overloading, the resolution of peaks

adjacent to the overloaded peak is

typically higher in the UHPLC method

than in the HPLC method. It is possible

to compensate for this overload effect

by simply scaling the injection volume

against column dead volumes as well as

the isocratic efficiencies (equations 12

and 13 in the sidebar).

Other Issues: In the early days

of UHPLC, selectivity differences

were commonly observed between

columns of nominally the same

material but differing particle size.

These differences were impossible to

explain by differences in the heat of

friction or pressure differences (20).

It was assumed that the base silica

of the smaller particle size material

was subtly different compared to its

larger particle size counterparts. Today

this difference is less of a problem.

However, if a selectivity difference is

observed that cannot be compensated

for by either increasing or decreasing

the temperature by a few degrees to

mimic heat of friction or by adding

a postcolumn restrictor to mimic a

pressure-induced retention change, it is

more than likely that it is related to subtle

differences in the heterogeneity of the

base silica used.

Regulatory AspectsThe degree of revalidation that is required

for a translated method depends on the

intended purpose for that method and

where in the R&D process it is to be

used.

For pharmacopeia methods, LC

translations can, in principle, be made

without any formal validation exercise

being performed provided that the

operating ranges described in the

appropriate monographs (23,40,44) are

not exceeded. Unfortunately, the current

operating ranges limit the ability to

translate from HPLC to UHPLC. However,

the United States Pharmacopeia (40)

recently opened up for translation of

isocratic methods from 5-µm porous

particles to sub-2-µm porous particles.

Hopefully other pharmacopoeias will

also follow this example and, in addition,

allow translations of gradient methods

as long as the specified selectivity

and efficiency is maintained (that is,

by maintaining or increasing the ratio

between column length and particle

diameter [41]).

For original pharmaceutical products

it is necessary to validate all versions of

the method that are used for analysis

of samples to be used in toxicological

or clinical studies. Do both the HPLC

and the UHPLC methods require

a full International Conference on

Harmonisation (ICH) validation (42)?

From a scientific point of view, it should

be sufficient to submit a full ICH

validation for either the HPLC or the

UHPLC version of the method. For the

other version, it should be sufficient to

submit a minimalistic validation report

claiming that the translation has been

made according to first principles

(that is, fundamental chromatographic

theory). In principle, it should be enough

to validate selectivity and linearity for

15www.chromatographyonline.com

Petersson et al.

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(7) D. Guillarme, D.T.T. Nguyen, S. Rudaz, and J.L. Veuthey, Eur. J. Pharm.

Biopharm. 66, 475–482 (2007).(8) D. Guillarme, D.T.T. Nguyen, S. Rudaz, and J.L. Veuthey, Eur. J. Pharm.

Biopharm 68, 430–440 (2008).(9) P. Petersson, “Implementation of U(H)PLC within a Global

Pharmaceutical Company - A New Way of Working, Advances in High Resolution and High Speed Separations,” Chromatographic Soc. Alderley Park, 2010.

(10) R.E. Majors, LCGC North Am. 29(6), 476–484 (2011).(11) J.W. Dolan, LCGC Europe 27(2), 82–86 (2014).(12) H. Engelhardt and H. Elgass, J. Chromatogr. A 158, 249–259 (1978).(13) P. Janderra, J. Chromatogr. A 485, 113–141 (1989).(14) J.W. Dolan and L. Snyder, J. Chromatogr. A 799, 21–34 (1998). (15) J.W. Dolan, LCGC Europe 27(3), 138–142 (2014).(16) A.P. Schellinger and P.W. Carr, J. Chromatogr. A 1077, 110–119 (2005).(17) P. Janderra, J. Chromatogr. A 1126, 195–218 (2006).(18) A.Clarke, J. Nightingale, P. Mukherjee, and P. Petersson,

Chromatography Today, May/June, 4–9 (2010). (19) www.unige.ch/sciences/pharm/fanal/lcap/telechargement.htm(20) P. Petersson and M.R. Euerby, J. Sep. Sci. 30, 2012–2024 (2007).(21) www.acdlabs.com/translatemymethod (22) www.acdlabs.com/products/spectrus/workbooks/chrom/ (23) European Pharmacopoeia 7th Edition, 2.2.46, “Chromatographic

separation techniques”, European Pharmacopoeia (European Directorate for the Quality of Medicines, Strasbourg, France, 2011).

(24) A.G. Huesgen, Agilent Technologies, www.agilent.com, Publication Number 5990-5062EN.

(25) P. Petersson and M.R. Euerby, personal communication; unpublished data; 16 March 2014.

(26) A. de Villiers, H. Lauer, R. Szucs, S. Goodall, and P. Sandra, J.

Chromatogr. A 1113, 84–91 (2006).(27) K. Kaczmarski, F. Gritti, and G. Guiochon, J. Chromatogr. A 1177,

92–104 (2008).(28) Y. Zhang, X. Wang, P. Mukherjee, and P. Petersson, J. Chromatogr. A

1216, 4597–4605 (2009).(29) F. Gritti and G. Guiochon, Anal. Chem. 80, 5009–5020 (2008).(30) M.M. Fallas, U.D. Neue, M.R. Hadley, and D.V. McCalley, J. Chromatogr.

A 1209, 195–205 (2008).(31) M.M. Fallas, U.D. Neue, M.R. Hadley, and D.V. McCalley, J. Chromatogr.

A 1217, 276–284 (2010).(32) F. Gritti and G. Guiochon, Anal. Chem. 81, 2723–2736 (2009).(33) P. Szabelski, A. Cavazzini, K. Kaczmarski, X. Liu, J. Van Horn, and G.

Guiochon, J. Chromatogr. A 950, 41–53 (2002).(34) M.R. Euerby, M. James, and P. Petersson, J. Chromatogr. A 1228,

165–174 (2012).(35) S. Fekete, J.L. Veuthey, D.V. McCalley, and D. Guillarme, J. Chromatogr.

A 1270, 127–138 (2012).(36) M.R. Euerby, M.A. James, and P. Petersson, Anal. Bioanal. Chem. 405,

5557 (2013).(37) N. Wu, A.C. Bradley, C.J. Welch, and L. Zhang, J. Sep. Sci. 35,

2018–2025 (2012).(38) A.J. Alexander, T.J. Waeghe, K.W. Himes, F.P. Tomasella, and T.F.

Hooker, J. Chromatogr. A 1218, 5456–5469 (2011).(39) P. Petersson, P. Forssen, L. Edstöm, F. Samie, S. Tatterton, A. Clarke,

and T. Fornstedt, J. Chromatogr. A 1218, 6914–6921 (2011).(40) United States Pharmacopeia General Chapter <621>

“Chromatography” First Supplement to USP 37-NF 32 (United States Pharmacopeial Convention, Rockville, MD, USA).

(41) U.D. Neue, D. McCabe, V. Ramesh, H. Pappa, and J. DeMuth, Pharmacopeial Forum 35, 1622–1626 (2009).

(42) International Conference on Harmonisation, ICH Q2(R1), Validation

of Analytical Procedures: Text and Methodology (ICH, Geneva, Switzerland, 2005).

(43) U.D. Neue, HPLC columns: Theory, technology and practice (Wiley-ICH, New York, USA, 1997), pp. 14.

(44) Japanese Pharmacopoeia 16th Edition, section 2.01 “Liquid Chromatography” (JP XVI 2.01, Pharmaceuticals and Medical Devices Agency, Shin-Kasumigaseki Building, 3-3-2 Kasumigaseki, Chiyoda-ku, Tokyo 100-0013 Japan, 2011).

Patrik Petersson is a principal scientist with Novo Nordisk A/S

in Måløv, Denmark. Please direct correspondence to ppso@

novonordisk.com

Melvin R. Euerby is a professor at the Strathclyde Institute

of Pharmacy and Biomedical Sciences in the University of

Strathclyde in Glasgow, UK and the head of research and

development and training at Hichrom Ltd. in Berkshire, UK.

Matthew A. James is a research analyst with Hichrom Ltd.

the translated version of the method. It is advisable, at least

during this transition period, to perform a full ICH validation

and be prepared to submit the “missing” parts of the validation

if requested by the authorities. It may also be prudent to

include both the HPLC and UHPLC versions of the method

in the experimental design used for validation of intermediate

precision.

Postsubmission changes to methods are possible according

to both the European Medicines Agency (EMA) and the Food

and Drug Administration (FDA) regulations. However, it is

uncertain what is required in the rest of the world. In addition, the

cost associated with a postapproval change is often considered

prohibitive.

ConclusionsThis article demonstrates how the practical advantages of

translating existing HPLC methodologies to those using newer

column formats and UHPLC instrumentation can be realized.

Advantages include increased resolution, enhanced speed of

analysis, reduced solvent consumption, more efficient utilization

of LC equipment, and ease of method transfer between HPLC

and UHPLC. The authors describe a number of potential pitfalls

that must be taken into consideration and avoided if accurate

and reliable translations are to be achieved. These pitfalls

include differences in LC instrumentation dwell volumes, which

can lead to coelution of peaks and even reversal of elution

order. The difference between the original and new VD/VM ratios

must be accounted for: In the case of the new methodology

having a larger VD/VM, a delayed injection must be used, or

if it has a smaller VD/VM, an isocratic hold must be inserted

before commencing the gradient. Errors in translated gradient

times of up ~30% can be encountered unless experimentally

determined VM values are used. This may affect both retention

and selectivity. Hence, the authors strongly recommend that

chromatographers practically determine their VM values.

The effect of instrument differences between HPLC and

UHPLC models have been highlighted as possible sources of

translation error; these include differences in column thermostat

design, the effect of extracolumn band broadening, and the

influence of differing injector design. In addition, the effect of

only moderately elevated pressures on selectivity has been

demonstrated, coupled with the effect of increased heat of

friction associated with smaller particles and the influence of

increased efficiency on peak asymmetry has been described.

A free translation tool is available to assist the successful

translation between HPLC and UHPLC methods (21). The tool

is based on the principles described in this article and permits

scaling of gradient times, flow rates, and injection volume as

well as accounting for differences in VD/VM ratios between LC

systems. A more comprehensive translation tool will also be

available (22).

References(1) J.W. Thompson, J.S. Mellors, J.W. Eschelbach, and J.W. Jorgenson,

LCGC North Am. 24(s4), 16–21 (2006). (2) J.J. Kirkland, F.A. Truszkowski, C.H. Dilks Jr., and G.S. Engel, J.

Chromatogr A 890, 3–13 (2000).(3) J.J. DeStefano, T.J. Langlois, and J.J. Kirkland, J. Chromatogr. Sci. 46,

254–260 (2008).(4) M. Swartz, LabPlus International 18, 6–9 (2004).(5) J.R. Mazzeo, U.D. Neue, M. Kele, and R.S. Plumb, Anal. Chem. 77,

460A–467A (2005).(6) Strategic Directions International (SDi) Tactical Sales and Marketing

Report (HPLC: End Users Influencing Development for Advanced HPLC Systems, Columns and Chemistry). (2013).

16 LC•GC Asia Paciàc March 2015

Petersson et al.

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17www.chromatographyonline.com

LC TROUBLESHOOTING

One of the most frequent times that

we discover a problem with a liquid

chromatography (LC) method is when

we examine a data set following the

analysis of a batch of samples. This

month’s “LC Troubleshooting” looks

at some data submitted by a reader

who suspected that something wasn’t

right with their results. These data

give us a good example of how we

can examine data for abnormalities

and formulate some experiments to

try to identify the problem source so

we can correct the problem. I have

somewhat obfuscated the details so

that the reader and company remain

anonymous. The sample comprises a

pharmaceutical formulation that was

being assayed for potency following

a particular stress test. A single

batch of product was divided into 12

samples, which were then treated

in the same manner. For analysis,

two subsamples were weighed from

each sample, diluted, and injected,

for a total of 24 sample injections.

The potency was determined by

comparing the area response of

each injection to the response of

a reference standard. The method

stipulates that if the two subsamples

disagree by more than 1.0% in assay

value, the source of disagreement

must be investigated. The reader

reported that normally these

“duplicate” samples agree within

0.5%.

The data I received are listed in

the first two columns of Table 1.

Each sample is numbered, and

the associated letter identifies the

subsample (for example, 1a and

1b are subsamples of sample 1). I

have noted the absolute difference

between the two subsamples in the

third column. The abnormality that

triggered the reader’s inquiry was the

1.41% difference between samples

4a and 4b. This difference exceeded

the limit allowed by the method and

required that the chemist perform an

investigation to identify the source

of the problem so that it could be

corrected.

Initial Examination

When I try to solve a problem like

this, I like to examine the data in

several ways. Often I find that a

table of data, such as that of Table 1,

makes my eyes glaze over. I do much

better with a graphic representation.

To get an idea of how atypical the

1.41% difference is, I constructed

the frequency plot shown in Figure 1.

Here I simplified the data set by

“binning” the absolute differences into

groups with 0.25% increments, so you

can see, for example, that there were

five samples in which the difference

between injections was 0–0.25%.

All the data points except the 1.41%

value were <0.75% difference.

The big gap between the 11 good

sample pairs and the one bad one

makes the problem pair seem like an

obvious outlier. But is there any more

quantitative measure of this? One

simple technique to test for outliers

is the Dixon’s Q -test. A test value is

calculated as:

|suspect – nearest|/(largest – smallest)

[1]

For this example, |1.41 – 0.73|/(1.41 –

0.07) = 0.51. The critical value of Q

for n ≥ 10 is 0.464 (1), meaning that

any test value larger than the critical

value is an outlier. Now we have

some statistical support in stating

that the difference in assay values

for sample 4 is an outlier. As I look

at the results of the Q -test, however,

it looks to me like the 1.41 value isn’t

very much of an outlier. I checked this

by looking at different suspect values

using the data set of Table 1, and it

is easy to show that the critical value

is exceeded only when the suspect

value is >1.3%. This says to me that

if the current data set is typical for

this method, the requirement for

differences of <1.0% may be a bit

too tight. That is, a value >1.0% will

trigger an investigation, but unless

it is >1.3%, it is not likely that it can

be proven an outlier with the Dixon’s

Q -test. Such limits should be set as

part of the method validation, where

large data sets are available and the

normal variation of the method can be

determined more easily than with the

limited data available here.

Digging a Bit Deeper

Sometimes it is useful to examine

the data for any trends that might

be obvious. An easy way to make a

first pass at this is to simply plot the

assay values over time. In Figure 2, I

have plotted the assay values in order

for the 24 injections. There doesn’t

seem to be any trend to larger or

smaller values over the course of the

analysis. The variability for the first

12 injections seems to be larger than

for the last 12, but these were run

on two separate days, so it may be

a day-to-day difference as much as

anything. The overall variability in the

data is shown at the bottom of Table 1

with the percent relative standard

deviation (%RSD) of only 0.5%.

Considering that many autosamplers

have %RSD in the 0.3–0.5% range

using reference standards under

carefully controlled conditions, it

looks to me like this method (including

the autosampler) is operating with

acceptable precision.

Listen to the DataJohn W. Dolan, LC Resources, Lafayette, California, USA.

A stepwise process helps isolate and identify the cause of a method failure.

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LC•GC Asia Paciàc March 201518

LC TROUBLESHOOTING

Although the %RSD is good when

comparing samples, I wondered

how good the precision was for

the same sample with multiple

injections. I asked the reader if

such data were available, and I was

supplied with the data in Table 2.

In Table 2, I have shown the results

for the original data from Table 1

(4a and 4b), the reinjection data of

the same vials (4a-ri and 4b-ri), and

the transfer data of the contents to

a new vial before reinjection (4a-nv

and 4b-nv). I am considering all 4a

samples to be equivalent and 4b

samples to be equivalent. You can

see from the data at the bottom of

the table that the variability (≤0.5%)

is approximately the same as it is

for the between-sample variability

for the data of Table 1 (0.5%). This

reinforces the conclusion I drew

in the previous paragraph that the

injection process is working properly.

What Is at Fault?

At this point, we’ve observed that

sample 4 exceeded the maximum

allowable difference between

subsamples and confirmed that the

difference between subsample 4a

and 4b is indeed an outlier using the

Dixon’s Q-test. We have also shown

that the results for both samples

4a and 4b have the same level of

precision as the remaining samples,

so it appears that the problem is not

related to the injector. Let’s see if we

can further narrow the source of the

problem to the primary sample 4 or

one of the subsamples 4a or 4b. We

have enough data now that we can

compare the assay values and see if

they are consistent.

First, let’s compare sample 4a

and 4b. With the three “equivalent”

injections for each sample from

Table 2, we can see if there is a

statistical difference between the

mean assay value of 4a and 4b.

We do this with the Student’s t-test

that is available as part of the

data analysis add-in for Microsoft

Excel. We select the two-tailed test

because we want to know if there is a

difference in the mean values. From

the six data points in Table 2, we can

calculate a test value of t = 3.19; for

a probability α = 0.05, the critical

value is t = 2.78, so the Student’s

t-test shows that there is indeed a

significant difference between the

mean assay values of sample 4a

and 4b. The Excel report (not shown)

refines this a bit and indicates that

there is only a 3.3% chance that

there is not a significant difference in

means.

Now we know that samples 4a and

4b are not equivalent. Can we extend

the process further and decide if

one or both of them are likely to have

an error in assay value? We can do

the same Student’s t-test for sample

4a and sample 4b compared to

the remaining samples. One might

argue that this is stretching the test

a bit, because the larger data set

compares variation between samples,

whereas 4a and 4b test within-sample

variation, but let’s ignore that for the

moment and see what we get. First,

we’ll take the data from Table 1 and

remove the injections for 4a and 4b,

leaving 22 data points. Then we’ll take

the three data points for 4a and run

the t-test comparison, then repeat it

for 4b.

When we compare the larger data

set to sample 4a, we get a test value

0

1

2

3

4

5

6

0 0.25 0.5 0.75 1 1.25 1.5

Subsample difference

Fre

qu

en

cy

Figure 1: Frequency distribution of subsample differences from Table 1,

binned into 0.25-unit increments.

Table 1: Percent assay values

for individual injections of a

pharmaceutical product.

Sample* % Assay Difference†

1a 86.180.49

1b 85.69

2a 86.450.45

2b 86.90

3a 86.100.55

3b 86.65

4a 86.111.41

4b 87.52

5a 85.810.14

5b 85.67

6a 86.640.73

6b 85.91

7a 86.180.14

7b 86.32

8a 86.680.24

8b 86.44

9a 86.580.07

9b 86.51

10a 86.830.59

10b 86.24

11a 86.580.45

11b 86.13

12a 86.160.19

12b 85.97

Average 86.34

SD 0.42

%RSD 0.5%

*Samples 1–12 are divided into

subsamples a and b, which should be

equivalent. †Difference in assay value

between subsamples a and b of each

sample.

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LC•GC Asia Paciàc March 201520

LC TROUBLESHOOTING

What’s Next?

Now that we’ve identified sample 4b

as being an outlier, what else can we

do to track down the source of the

problem? First, we should eliminate

the simple and obvious possibilities.

The ones that come to my mind are

transcription errors and integration

errors. If the analytical balance has

a printer attached, check the printer

tape to make sure that the weight for

sample 4b was transcribed correctly

into the calculation of the assay value.

For example, the reported weight (not

shown) was 100.29 mg; if the decimal

values were reversed in transcription

from a true value of 100.92, the

correct weight (100.92 mg) would

change the 87.52 assay value to

86.92, and the difference between

4a and 4b would drop from 1.41% to

0.86%, and would pass the maximum

difference test (1.0%) and bring

sample 4b within 1.5 SD of the mean.

Another possible error is in integration

of the peak; double-check that the

baseline was drawn properly.

At this point, you may feel that

the investigation is complete. We’ve

identified sample 4b as an outlier, and

its companion 4a gives a reasonable

value. Depending on your laboratory’s

standard operating procedures

(SOPs), you may be able to drop 4b

from the data set and use the data

from 4a for reporting purposes. Write

up your investigation report and you

are done. Of course, you should keep

your eyes open for similar failures in

the future to determine if there is a

of t = 0.76, whereas the critical value

is t = 2.07. This tells us that there is

no statistical difference between the

mean assay value for sample 4a and

that of the remaining samples. With

sample 4b, the test value of t = 3.20,

which exceeds the critical value,

means we can conclude that there is

a significant difference between the

mean assay value for sample 4b and

the remaining samples. We may get

a better concept of this if we view

the data in Figure 3. In Figure 3, I

have binned all the assay values

from Table 1 into 0.25% increments.

As expected, the general form is

that of a Gaussian distribution,

which would be the case for a large

number of points containing random

error. The mean (bottom of Table 1)

is 86.34, which falls in the 86.5

bin. The value for 4a (86.11) falls in

the 86.25 bin, which confirms what

we found above: sample 4a is not

significantly different than the mean

of the remaining 22 values. The

value for 4b (87.52), however, falls in

the 87.5 bin at the extreme right of

Figure 3. With a standard deviation

(SD) of 0.42 for the data of Table 1

this means that 4b is 2.8 SD from the

mean; for a Gaussian distribution,

99.4% of the values will fall within

±2.8 SD of the mean. Contrast this to

the smallest value of Table 1 (85.67),

which is 1.6 SD below the mean;

89% of values should fall within ±1.6

SD of the mean, so it is much less

likely that 85.67 is an outlier than is

87.52.

high enough frequency of failure to

merit further investigation.

If you want to investigate further,

you need to consider all the possible

sources of variation and determine

if they are potentially important

and if they can be reduced in

magnitude. If the sources are

independent of each other, the

overall coefficient of variation

(CV = %RSD/100) can be determined

as the square root of the sum of

squares of each variable:

CV = (CV12 + CV2

2 + . . . + CVn2)0.5

[2]

where the subscripts represent

each independent operation. The

operations that come to mind in this

instance are sampling, weighing,

dilution, mixing, filtration, injection,

and integration; there are probably

others I’ve overlooked. Each of these

will contribute uncertainty to the overall

measurement. Sampling errors reflect

how representative the subsamples

are. For example, if the sample were

granular sugar or a cup of coffee, the

primary sample is very homogeneous,

so taking a random sample should be

fairly representative of the whole. On

the other hand, if the sample were a

bag of M&M candies, the distribution

of the different colours in a small

subsample would likely have much

more variation. Thus, the homogeneity

of the sample and the ability to take a

representative sample would influence

the sampling step. The variation in

weighing could be tested by weighing

a fixed standard weight multiple times.

The reader did not specify how dilution

Table 2: Data for multiple injections of

samples 4a and 4b.

Sample* % Assay Sample* % Assay

4a 86.11 4b 87.52

4a-ri 86.33 4b-ri 86.67

4a-nv 85.98 4b-nv 86.87

Average 86.14 Average 87.02

SD 0.18 SD 0.44

%RSD 0.2% %RSD 0.5%

*a and b are original values from Table

1; ri is a reinjection of the original sample

from the same vial; nv is a reinjection

of the original sample after it was

transferred to a new vial.85.0

85.5

86.0

86.5

87.0

87.5

88.0

Injection order

Ass

ay v

alu

e

1 5 10 15 20

Figure 2: Plot of assay values from Table 1 in injection order.

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21www.chromatographyonline.com

LC TROUBLESHOOTING

was done; however, more uncertainty

would be expected if a graduated

cylinder were used to measure the

liquid as compared to preparing the

sample in a volumetric flask. Is the

mixing sufficient for the concentrated

sample and the diluent? Should

mixing time be extended, agitation

or sonication increased, or other

variations in the mixing process be

changed to improve the homogeneity

of the diluted sample? Does filtering

the sample affect the final result? This

possible effect could be checked by

comparing centrifugation to filtering

and seeing if the results were any

different. Check the precision of the

injector by making replicate injections

of a well-behaved analyte. If errors are

constant, such as an error of ±0.1 mg

on the analytical balance, a fixed

volumetric error with a volumetric flask,

or ±0.2 µL for sample injection, they

can usually be reduced by increasing

the sample mass, dilution volume,

or injection volume, respectively, to

reduce the percent contribution of the

fixed error to the total.

Before embarking on a detailed

investigation of the method CV, you

should step back and consider if it

is likely that you will really improve

the results of the analysis. A basic

principle of statistics tells us that for

independent errors, as in equation

2, the largest error will have the most

influence on the overall error, that the

overall error will never be smaller than

the error of the largest contribution,

and that the overall error will usually

fall between the value of the largest

error and twice that value. We

determined in Table 1 that the overall

method %RSD was 0.5% based on

single injections of multiple samples.

An autosampler that is operating well

should have errors in the range of

0.3–0.5%, so it is unlikely that the

overall error can be reduced much

below the observed value of 0.5%.

In other words, after a brief mental

evaluation of the problem, I don’t think

I’d waste my time trying experiments

to reduce the overall error. Instead,

I’d stay alert to see if I could correlate

future failures to some pattern in the

analysis.

Conclusions

Let’s review what we’ve been able to

observe about the present problem:

• An error was found when the

difference in assay values between

equivalent subsamples exceeded

the 1.0% threshold.

• By evaluating the difference

between subsamples 4a and 4b

both visually (Figure 1) and with the

Dixon’s Q-test, we showed that the

difference was indeed an outlier

from the remaining samples.

•We also concluded from the Q-test

that the 1.0% threshold may have

been a bit too tight because, based

on the current data set, differences

of 1.0–1.3% would fail the test

criteria, but would not be proven

outliers by the Q-test.

• Based on multiple injections of

samples 4a and 4b, we used the

Student’s t-test to show that there

was statistical difference between

the mean assay values of the two

samples, so they are not equivalent.

•We also used the t-test to find that

the assay value for sample 4a

fit within the normal range of the

remaining samples, whereas sample

4b did not. This test correlated the

cause of the problem with sample

4b, not 4a.

•We confirmed the association of the

problem with sample 4b by plotting

a frequency distribution of the assay

values in Figure 3. Sample 4b was

clearly at the extreme edge of the

plot, whereas the value for 4a was

near the middle.

• Before concluding the investigation,

it was suggested that we check

for obvious errors in numeric

transcription and peak integration.

•We mentally evaluated possible

sources of uncertainty with the

method and concluded that it was

unlikely that a thorough investigation

of these sources would yield

information that would reduce overall

uncertainty of the method.

Although the present discussion

centred on a specific data set, it

illustrates how we can use simple

graphic and statistical tools to

investigate the failure. We were able

to assign the error to a single sample

(4b) and demonstrate that its paired

subsample (4a) behaved in the same

manner as the remaining samples, so

it may be possible to use its results to

obtain reliable assay data.

References(1) J.C. Miller and J.N. Miller, Statistics for

Analytical Chemistry (Ellis Horwood

Limited, 1984).

“LC Troubleshooting” Editor John Dolan

has been writing “LC Troubleshooting”

for LCGC for more than 30 years.

One of the industry’s most respected

professionals, John is currently the Vice

President of and a principal instructor for

LC Resources in Lafayette, California,

USA. He is also a member of LCGC

Asia Pacific’s editorial advisory board.

To contact John directly please e-mail:

[email protected]. To

contact the editor-in-chief, Alasdair

Matheson, please e-mail: amatheson@

advanstar.com

0

1

2

3

4

5

6

7

8

85.5 85.75 86 86.25 86.5 86.75 87 87.25 87.5

Assay value

Fre

qu

en

cy

Figure 3: Frequency distribution of assay values for all samples from Table 1,

binned into 0.25% increments.

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LC•GC Asia Pacià c March 201522

GC CONNECTIONS

Gas chromatography (GC) ovens

were not developed for cooking

purposes, but rather to provide a

suitable thermal environment for the

elution of chromatographic peaks

from GC columns. That being said, I

have seen a number of inappropriate

applications for GC ovens including

reheating of cold pizza for lunch

and the warming of casseroles for

company potluck dinners. Some of

us have even been known to trick out

the oven door switch and use an idle

GC system as a room heater on cold

days.

GC ovens have gone through an

evolutionary development just like

other GC components have. Today,

the majority of GC ovens use rapidly

circulating air inside an insulated

enclosure to transfer heat to and from

the column, much like the convection

ovens found in many high-end

kitchen ranges. Some readers may

be familiar with other means that

chromatographers use to control the

thermal environment surrounding

a column; some of these are quite

ingenious. First, though, let’s take

a look at what kind of thermal

conditions a column needs to deliver

excellent separation performance.

GC Oven Requirements

In gas chromatography, the

relationship between peak

retention and column temperature

is fundamental. Changes in

temperature cause significant

exponential retention shifts, so GC

instruments control solute retention

times by carefully managing the

column temperature along with the

column pressure drop. In general,

retention times decrease by a factor

of two for every 15–20 °C increase

in column temperature (Tc). Peak

retention depends differently on

column temperature with isothermal

versus temperature-programmed

elution, but in both cases tight

control of the temperature is

paramount. This same temperature

dependency also causes minor

temperature shifts to randomize peak

retention times by a small amount

from one run to the next. Slightly

higher overall oven temperatures

cause peaks to be eluted a little

earlier, and lower temperatures

shift retentions to longer times.

In addition to changes in the

average oven temperature from

one run to the next, other important

temperature variabilities include

spatial fluctuations along the column

because of temperature gradients in

the GC oven and dynamic short-term

oven temperature fluctuations

because of electronic and software

temperature-control processes.

If large enough, such spatial and

short-term changes will affect peak

shapes and resolution.

Run-to-Run Average Temperature DeviationsIn general, run-to-run retention

time deviations should stay within

a window of about ±10% of the

peak width at base. That way there

is little ambiguity concerning peak

identification by absolute retention

time, including for partially separated

peaks. The narrowest practical peak

widths will put the most demands on

the oven temperature repeatability.

Relatively short, 10-m long, 0.20-mm

i.d., thin-film capillary columns

elute significantly retained peaks

— those with retention factors of

two or greater — with base widths

of about 1.5 s minimum. This figure

assumes that the column operates

at an optimum average linear

helium carrier gas velocity of about

30 cm/s with the best theoretical

efficiency. Chromatographers can

obtain narrower peaks by operating

columns at higher than optimum

carrier-gas velocities, or by choosing

narrower or shorter columns — in

other words, by going to “fast” GC.

But in general this is about as fast as

peaks go for the vast majority of GC

systems in operation today.

The oven is not the only factor

that contributes to run-to-run

retention time variations. The

pneumatic system also influences

retention times significantly, and the

data handling system introduces

other uncertainties including its

determination of the exact run start

time and the peak apex or centroid.

I assembled a statistical analysis

of these factors and the GC oven

using typical values for modern

GC instrumentation and columns.

Gas Chromatography OvensJohn V. Hinshaw, Severon Corporation, Oregon, USA.

The transit of peaks through a gas chromatography (GC) column depends strongly on the thermal proà le they encounter on the way. Gas chromatographers primarily rely on the classic hot-air-bath type of oven, but several alternatives are also in use. This instalment examines ovens for GC in several forms plus how oven thermals affect peak retention behaviour.

GC ovens have gone through an evolutionary development just like other GC components have. Today, the majority of ovens use rapidly circulating air inside an insulated enclosure to transfer heat to and from the column.

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23www.chromatographyonline.com

GC CONNECTIONS

Interested readers can refer to

a website for this supplemental

information (1). In this analysis,

the room temperature and GC line

voltage supply are assumed to

be stable and to not influence the

actual oven temperature and column

pressure drop. This is not always the

case, of course, and such problems

fall into the category of instrument

“environmental” difficulties that

should be resolved before attempting

to obtain the best retention time

reproducibilities.

Isothermal Elution: According

to this analysis, the average oven

temperature needs to repeat from

run to run within less than ±0.05 °C

to hold retention times inside a

window of ±10% of peak base

widths, for commonly encountered

solutes. Lee, Yang, and Bartle

cite a similar requirement in their

1984 book (2). These figures are

for typical test mixture solutes

separated at moderate isothermal

temperatures on short narrow-bore

thin-film capillary columns, which

represent the more difficult cases.

Columns with thicker stationary

films, columns that are longer,

wide-bore columns, and, of course,

packed columns generate broader

peaks and may tolerate a less

stringent temperature environment

while still delivering retention time

repeatability that is adequate for

peak identification purposes. On

the other hand, fast GC separations

performed on microbore columns

with inner diameters under 0.2 mm,

on short columns under 10 m, or

with elevated carrier-gas velocities

over 100 cm/s, may require better

temperature control to contain

retention times within a ±10% of

base-width window.

Temperature Programming: With

isothermal elution, peak base

widths increase approximately in

proportion to the retention time,

but with single-ramp programmed

temperature elution the base widths

stay approximately constant across

a GC run, for peaks that are eluted

during the temperature ramp. Most

peaks are essentially immobilized

upon injection at the initial column

temperature; as the oven temperature

increases, solutes begin to move

along the column. Each spends

about the same time moving through

the column (3), which results in the

peaks having approximately the

same widths as they are eluted. For

temperature programming, oven

temperature ramps need to repeat

the time and temperature curve with

the same precision as required for

isothermal elution. The oven heating

system must have sufficient power

to maintain a linear programme

ramp from the start temperature to

the final temperature. The maximum

rate at which the oven temperature

can increase linearly is related

to the thermal mass of the oven

cavity, including the column, the

power that the heater can dissipate

into the oven, the efficiency of the

oven boundary insulation, and the

differential temperature between the

inside of the oven and the external

environment.

One principal difference between

isothermal and programmed elution

is the slight time lag between the

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LC•GC Asia Paciàc March 201524

GC CONNECTIONS

the average column temperature

along the length of the column. Minor

temperature fluctuations of less than

1 °C along the column do not affect

retention times seriously, as long

as these gradients are stable and

repeatable. Unstable gradients that

change from run to run, however,

will impose additional uncertainty on

retention times because they affect

the average temperature that solutes

experience.

Some temperature gradients

are normal and necessary. The

column inlet and outlet connect to

the injector and detector, which are

normally at elevated temperatures

relative to the oven. Where GC

column ends are positioned inside

the inlet and detector, a negative

temperature gradient exists from the

inlet into the column and a positive

gradient out into the detector. The

net effect on retention is negligible,

since solutes will be weakly retained,

if at all, in the short sections of

heated column ends, which act more

like connecting tubing. Gradients

also exist close to the oven walls

because of heat losses or gains

from cooler oven walls or warmer

heated inlets and detectors. In a

conventional air-bath oven, the

column is normally positioned in

the centre of the oven to immerse it

in the most thermally uniform area.

These stable temperature gradients

do not seriously affect performance if

they are stable both during a run and

in the long term from run to run.

Gradients that fluctuate from run to

run will affect retention time stability,

but gradients that fluctuate rapidly

during a run will affect peak shapes.

A poorly sealed air-bath oven can

generate this type of gradient. A

controlled amount of air normally

circulates through an air-bath oven,

to prevent the buildup of explosive

hydrogen gas. This is done in such

a way that significant temperature

gradients are not generated. But if

the oven door or vent isn’t sealed

properly, significant amounts of

cold air can enter and blow directly

on the column and create a rapidly

fluctuating localized temperature

gradient. For fused-silica columns

in particular, with their thin walls

and rapid thermal time constants,

fluctuating gradients will alternately

trap and release portions of solute

actual column temperature and

the setpoint temperature of the

temperature ramp. As the oven

temperature controller increases

the setpoint temperature according

to the demands of the programme

ramp, the actual oven temperature

lags behind by a small amount and

the temperature inside the column

lags a little more. The temperature

lag is larger at higher programme

rates. This temperature differential

is a necessary by-product of both

the nature of temperature-control

algorithms and the physics of heat

transfer from the heater to the

column. For our purposes, it is the

temperature in the column itself that

counts.

The electronics and software

must repeat not only the same time

and temperature profile across

the run, but also the thermal

conditions in the oven must be

consistent. This is one reason why

temperature-programmed ovens

require a temperature equilibration

period after cooling down before

a new run can commence. Shortly

after the oven cools down, the oven

temperature probe may indicate the

initial oven temperature, but there

is still a significant amount of heat

remaining in the oven; the walls and

the column can be significantly hotter

than the indicated temperature. This

is the reverse of the temperature lag

encountered with oven heating, and

good practice dictates that sufficient

time be allowed to dissipate the

residual oven heat and bring the

column as close as possible to

the initial oven temperature. An

equilibration time of 2–4 min is

typical for most air-bath GC ovens

with temperature programming

capability. With isothermal elution, no

equilibration time is required after the

oven reaches its temperature for the

first time, because the temperature is

not changed during the run.

Oven Gradients: A high degree

of run-to-run average temperature

repeatability ensures the best

retention time precision. GC ovens

also must maintain a uniform and

stable temperature profile across the

column during elution. The process

of solute partitioning and migration

along the column averages out

temperature gradients so that peaks

are eluted as if they experienced

bands as they pass by, which will

distort the peak shapes and may

even split peaks up into apparent

multiples.

GC operators play an important

role in ensuring the minimum

possible gradients, by installing

columns correctly. As much as

possible, columns should be centred

within the column oven, with no

length of the column closer than

about 1 in. (2.5 cm) from the oven

walls, except of course for the inlet

and detector connections. Column

mounting brackets provided by the

manufacturer are the best way to

provide secure and centred column

mounting.

Oven Heating Schemes

Over the years, GC researchers

have envisioned and built a wide

variety of column heating schemes.

Early workers were well aware of

the requirements imposed by the

sensitivity of GC retention times

to temperature changes and by

the problem of transient thermal

gradients. They had it easier than

present-day chromatographers,

however, because they had to

accommodate packed columns and

metal or thick-walled glass capillary

tubing, but not fused-silica tubing.

Thin-walled fused-silica tubing

responds more rapidly to oven

temperature changes and is more

susceptible to the effects of rapidly

changing oven gradients. The newest

generation of GC ovens includes

features designed to maximize

performance with all columns.

Oven heating schemes fall into

two broad categories: those that

rely on a fluid to transfer heat to and

from the column, and those that

use solid-state materials for heating

purposes. Today, of course, air is

the heat-transfer fluid of choice for

most of us, but that was not always

the case. Chromatographers have

experimented with various vapours

and liquids, as well. Solid-state ovens

have been applied to temperature

programming metal capillary

columns, and small, completely

solid-state ovens are found primarily

in portable instruments because of

their low power requirements and

good long-term stability. Columns

installed inside resistively heated

metal tubing or directly heated

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25www.chromatographyonline.com

GC CONNECTIONS

column tubing, suspended inside a

conventional air-bath oven, deliver

very fast programming rates for

high-speed GC.

Fluid Ovens: The earliest report

I could find of a fluid oven for GC

involves the suspension of the

column inside a vapour bath over

a boiling pure substance (4). This

technique of temperature regulation

had been used in various related

disciplines even before partition GC

came into its prime in the 1950s, and

it was a natural step to use it for the

then-new technique. The operator

could change the temperature of the

vapour bath up or down by regulating

the pressure inside a sealed oven

container. For example, p-xylene

boils at 138 °C at 1 atmosphere and

temperatures down to about 30 °C

lower were attainable at reduced

pressures (5). Changing the oven

temperature outside this limited

range was not very convenient

because the pure substance had

to be exchanged for another with a

higher or lower boiling point. This

arrangement produced a fairly stable

thermal environment for the column,

as long as the atmospheric pressure

didn’t change too much. There were

also problems with decomposition

of the boiling substance at higher

temperatures, as well as the

flammability of the vapours, and

chromatographers abandoned this

heating system fairly early.

Oil baths were also used as oven

thermostats (6). After the operating

temperature was reached, if the

heating vessel was well insulated

and efficiently stirred, a very uniform

thermal environment was possible.

Temperature control circuitry

provided fairly good temperature

stability. Such baths could be

temperature programmed, but at

a limited rate because of the large

heat capacity of the oil. A main

drawback of oil bath ovens was

the inconvenience of working with

high-molecular-weight oils that would

coat the column and connections.

The slightest leak would permit the

oil to enter and destroy the column

or, at the very least, drastically

modify its retention characteristics.

Changing the column was difficult

and messy. A water bath was also

used, but with a limited temperature

range.

Air-Bath Ovens: GC researchers

understood at the onset that an

air-bath oven was potentially superior

to liquid or vapour bath designs.

The temperature in an air bath

could be varied rapidly over a wide

range without changing the working

fluid, and it would be much easier

to change columns. However, early

air-bath oven designs from the 1950s

suffered from large temperature

gradients and a significant lag

time between the oven setpoint

and actual column temperatures.

Improved fans and better insulation

helped to remedy the situation, and

by the mid-1960s the air-bath oven

was almost universally accepted.

The subsequent introduction of

microprocessor temperature control

in the 1970s and the adoption

of a number of other important

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LC•GC Asia Paciàc March 201526

GC CONNECTIONS

separation, but this is certainly an

impressive capability. This type of

hybrid arrangement is available as

a special oven door with integrated

electronics and controller.

ConclusionGas chromatographers have invented

and adapted various methodologies

for controlling column temperature.

Far removed from simple cake

baking requirements, the physics

and chemistry of GC separation and

elution determine the requirements

for temperature control. The need for

application flexibility or specificity

determines the kind of heating

system that is appropriate. A broadly

applicable system such as the

conventional air-bath oven gives the

greatest flexibility at the expense

of portability, power consumption,

and space. Dedicated systems

in which the column and heater

are permanently mated yield low

power consumption, portability, and

compactness. Interest in high-speed

and high-resolution GC will continue

to spur developments in column

heating technologies.

References(1) See http://wiki.hrgc.com

(2) M.L. Lee, F.J. Yang, and K.D Bartle,

Open Tubular Gas Chromatography.

Theory and Practice (Interscience, New

York, USA, 1984), p. 106.

(3) J.C. Giddings, J. Chem Educ. 39, 569

(1962).

(4) A.T. James and A.J.P. Martin, Biochem.

J. 50, 679–690 (1952).

(5) A.I.M. Keulemans, Gas

Chromatography (Reinhold Publishing

Corp., New York, USA, 1957), pp.

59–61.

(6) D.H. Desty and B.H.F Whyman, Anal.

Chem. 29, 320–329 (1957).

(7) L.S. Ettre, J. Chrom. Sci. 15, 90–110

(1977).

(8) L.S Ettre, Amer. Lab 31(14), 30–33

(1999).

(9) S.R. Lipsky and M.L. Duffy, J. High

Resolut. Chromatogr. 9(376–382),

725–730 (1986).

John V. Hinshaw is a senior scientist

at Serveron Corporation in Beaverton,

Oregon, USA, and is a member of the

LCGC Asia Pacific editorial advisory

board. Direct correspondence about

this column should be addressed

to “GC Connections”, LCGC Asia

Pacific, Honeycomb West, Chester

Business Park, Chester, CH4 9QH,

UK, or e-mail the editor-in-chief,

Alasdair Matheson, at amatheson@

advanstar.com

asbestos tape. A variable voltage

gave rudimentary temperature control

(7). Another approach connected a

source of electrical current across

the metal packed column itself, and

at least one commercial GC used this

method (8). This approach has also

been applied to metallic open-tubular

columns and metal-coated

fused-silica columns (9).

A different solid-state column

heating design packages the

column and a separate heater into a

monolithic block. One or more metal

capillary columns are wound with a

heating element around a core and

the entire assembly is then encased

in thermoplastic resin. The column

tubing terminates outside the oven

assembly in adjacent valves, inlet

systems, and detectors, and the

entire assemblage is placed inside

an insulated enclosure. This type of

construction is attractive for portable

isothermal GC systems because

once heated, it doesn’t require a lot

of power to maintain temperature

and it can be very small in size.

Changing the column requires a

complete exchange of the inner oven

assembly, however.

Micro GC: GC systems that use

nonconventional micromachined

inlet, column, and detector modules

have experienced significant

development in the past decade.

Such devices may use columns

etched into a planar substrate

with integral or attached heating

elements. Small both in size and

power consumption, these GC

systems are finding a niche in field

portable applications.

Hybrid Ovens: Some of the most

recent high-speed GC arrangements

for benchtop instruments use a

hybrid combination of an air-bath

that surrounds solid-state heated

columns. By using short columns

with smaller internal diameters in

combination with fast heating, such

a device can deliver the resolution

of longer, larger diameter columns

in less time. In one arrangement,

the column runs coaxially inside a

coiled, externally insulated metallic

tubular heater that is suspended

on a cage in the air-bath GC oven.

Such devices can achieve ramp

rates up to 1200 °C/min, although

at such rates the oven temperature

will likely get ahead of or escape the

features —  including improvements

made specifically for fused-silica

columns — resulted in modern GC

oven designs that are ubiquitous

today. GC air-bath ovens are

available in both cylindrical and

cubic forms.

Common features among air-bath

ovens include high-speed fans for

turbulent mixing that minimizes

internal gradients. The columns and

temperature sensor are shielded

from direct thermal radiation emitted

by the oven heating element.

Incrementally positioned oven

vents supply regulated amounts of

cooling air for improved control at

temperatures close to ambient and

open fully for maximum cool-down

rates.

These ovens can routinely deliver

retention time repeatability well

within the criteria cited earlier in this

article. Today, GC ovens are capable

of linear temperature programming

rates up to at least 75 °C/min with a

standard heating element. However,

the maximum linear programme rate

declines to around 20–30 °C/min at

temperatures above about 175 °C

because of increasing heat losses

through the temperature gradient,

through the oven insulation, and out

to the surrounding environment. More

powerful oven heaters available with

some instruments can yield higher

programming rates up to 120 °C/min

that are suitable for higher speed

GC separations. When the columns

occupy only a fraction of the full

oven volume, even faster heating and

cooling are obtainable by reducing

the oven air volume with an internal

insulating blanket.

The fastest GC total run-to-run

times require not only fast heating,

but also rapid cooling back to the

initial oven temperature. The use

of an extra fan that forces cooling

air through the oven vents helps to

speed cool-down time. Cryogenic

cooling is another option that

minimizes cool down, but is not

always convenient or available.

Solid State Ovens: GC

experimenters also developed

a number of different solid-state

column heating schemes over the

years. An early design used heating

wire that was simply wrapped

around a straight or U-shaped

packed column and insulated with

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COLUMN WATCH

Recently, both instrumental manufacturers and the pharmaceutical industry have increased their interest in supercritical fluid chromatography (SFC) because of the lower environmental impact and the considerably shorter separation times compared to traditional high performance liquid chromatography (HPLC). The use of low-viscosity carbon dioxide as the main solvent enables operation at higher flow rates as compared to liquid chromatography (LC) (1), and the low toxicity of this mobile phase and its ease of recycling have created another important incentive. Even though the SFC revival has focused on preparative chiral separations (2), it has also been successfully used in many achiral applications. However, LC still dominates analytical applications because of its versatility and, so far, its superior robustness compared to SFC. If the reproducibility of modern SFC could be considerably improved, we believe its revival would be strongly boosted.

The inherent problem with SFC that makes it so much more complex than LC is the compressibility of the mobile phase, which makes SFC a “rubber variant of LC”. Everything considered as constant in LC is not constant in SFC (3,4). This ultimately results in radial and axial density and temperature gradients

in the column that affect the thermodynamics of adsorption and cause a volumetric flow rate gradient through the column (5–7). The practical consequences are serious. We cannot be guaranteed that the set operational conditions reflect the true conditions over the columns like we can in LC. This results in poor system-to-system reproducibility and transfer between analytical methods, which in turn hampers the wider use of SFC in the pharmaceutical industry. These phenomena also result in poor predictions in scaling up from analytical SFC instruments to preparative SFC instruments (8). The consequence is that optimization in process- and preparative-scale SFC must be done in the large scale, which costs money and energy and may even be impossible in some cases. Therefore, a proper understanding of how operational parameters such as pressure, temperature, and solvent composition affect the separation and its reproducibility is of paramount importance.

In this brief investigation, with both new and review material, we start out with some illustrative examples of poor method transfer among different analytical systems. Thereafter, we report on recent investigations on which experimental parameters are the most important to improve reproducibility and method of transfer in SFC. Some

guidelines to users and some advice for improvements to manufacturers is also provided.

Results and DiscussionExamples of Poor Reproducibility

Between Systems: First, the reproducibility between different SFC systems was studied by injecting 20 µL (full-loop) of 350 g/L antipyrine solution on four different SFC systems using identical instrumental settings and the same column (see Figure 1). Liquid carbon dioxide was supplied to systems 1, 3, and 4 (AGA Gas AB, Sweden) and system 2 was fed gaseous carbon dioxide. The same 150 mm × 4.6 mm Kromasil silica column, packed with 5-μm nominal particle size, 100-Å pore size media (AkzoNobel Eka) was used for all systems. The back pressure (P) was 150 bar, the column temperature was 35 °C, and the eluent composition was 85:15 (v/v) carbon dioxide–methanol. All experiments were carried out at volumetric flow of 2 mL/min.

Modern Supercritical Fluid Chromatography — Possibilities and Pitfalls Torgny Fornstedt1 and Ronald E. Majors2, 1Karlstad University, Karlstad, Sweden, 2Column Watch Editor

There has been a revival of supercritical fl uid chromatography (SFC) in recent years, especially in the chiral preparative fi eld, but also more recently in the analytical area. However, SFC is considerably more complex than liquid chromatography (LC), mainly because of the compressibility of the mobile phase. One can say that SFC is a “rubber variant” of LC where everything considered constant in LC varies in SFC. In this review, we go through advances in theory, instrumentation, and novel applications.

The inherent problem

with SFC that makes it so

much more complex than

LC is the compressibility

of the mobile phase,

which makes SFC a

“rubber variant of LC”.

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LC•GC Asia Paciàc March 201528

COLUMN WATCH

The resulting overloaded elution

profiles, corrected for system void

volumes, is clearly system dependent

as can be seen in Figure 1. This

figure also shows that the elution

volume is larger on system 4 while

systems 1 and 2 have lower, and

similar, retention volumes. However,

system 3 (same instrument model as

system 1) had a retention volume that

was more than 0.5 mL larger than

that of system 1 when using the same

column and the same set conditions.

This observation indicates that either

the set conditions are not manifested

in the systems or that the operational

column conditions were different,

although identical set values were

used. We further investigated if the

volumetric flow rate was the reason

for the observed difference between

the elution profiles shown in Figure 1,

but the column dead volume was

determined and was estimated to

be approximately 1.9 mL on each

system. This observation means that

the volumetric flow rate was more

or less identical on all systems;

otherwise the void volumes would

have been different.

Other important parameters

governing retention are the density

of the mobile phase, the fraction

of organic modifier (CM), and the

column temperature (T ). The density

is a nonlinear function of pressure

(P) and temperature; to calculate the

density of the carbon dioxide and

methanol stream inside the column,

the pressure at the column inlet and

outlet as well as the actual column

temperature must be known. An

immediate conclusion was that none

of the systems measure pressure

directly before or after the column,

only at a point upstream from the

column. Furthermore, this pressure

reading cannot simply be correlated

between different systems because

the pressure drop upstream to the

back-pressure regulator will be

divided between capillaries and

column. Pressure drop from the

capillaries will depend on their length

and diameter, which cannot be

assumed to be identical between the

different systems. So the reason for

the problem is probably due to the

fact that in SFC — in contrast to LC

— the set operational values are not

necessarily identical with the actual

operational values.

12System 1

System 2

System 3

System 4

6

Co

nce

ntr

ati

on

(g

/L)

0

5 6 7

Volume (mL)

8

Figure 1: Experimental chromatograms recorded on the various SFC systems. The

set volumetric flow was 2 mL/min and the injection volume was 20 µL of a 350-g/L

sample.

160

150

Back

pre

ssu

re (

bar)

140

Methanol content (%)

14

7.2

0

7.0

06.8

0

6.6

0

6.4

0

6.2

0

15 16

Figure 2: Retention volume of analytical peaks as a function of methanol content

and pressure determined using 14, 14.5, 15, 15.5, and 16 (v/v) % methanol content at

140, 145, 150, 155, and 160 bar on system 1. All analytical injections were 5 µL of a

0.35-g/L sample.

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LC•GC Asia Paciàc March 201530

COLUMN WATCH

Deeper Investigation of the

Causes of the Poor Reproducibility

Between Systems:

Initial Experiments: We used a

design-of-experiment (DoE)-based

approach (9) to find out the most

important parameters affecting

the reproducibility of retention for

different neutral model compounds

in this system and similar ones. In

DoE, the effects of variations of

operational parameters on a certain

response, such as retention factors

or selectivity in chromatography,

are statistically investigated under

controlled experiments. For this

particular study, we had to find out

the real temperature, pressures,

and the cosolvent fractions inside

the column. Thus, we used external

devices to measure the real mass

flows over the column and external

sensors for measuring temperature

and pressure at different positions

along the column (5).

Before the DoE-based experiments

and modelling, we investigated

experimentally how retention volumes

are affected by changes in system

back pressure and modifier content

(10). Analytical injections of 5 µL

of 0.350-g/L antipyrine solutions

were performed at back pressures

of 140–160 bar and modifier

fractions of 14–16%, on system 1

(see Figure 2). As seen in Figure 2,

the retention volume was strongly

affected by changes in the modifier

concentration and to a smaller extent

to the “set” back pressure. When

performing the system reproducibility

experiments described in the

previous section, we noticed that

system 4 had a much lower pressure

drop compared to systems 1 and 2.

5

-5

Co

eff

cien

ts ×

100

-10

-15

P

CM

P.C

M

CM

.T

P.T

C2

M

P 2

T 2T P

CM

P.C

M

CM

.T

P.T

C2

M

P 2

T 2T

0

-5

-10

-15TSO k1

TSO k2

BINOL k1

BINOL k2

0

(a) (b)

7

CM (

v/v

%)

CM (

v/v

%)

24

19

14140 160

P (bar)

k1 BINOL k

2 BINOL

P (bar)

180 200 140 160 180 200

5

3

130 170 210 130 170 2102

6

9

6

3

8(a) (b)

(c) (d)

k2

TSOk1

TSO

k TSO

k B

INO

L

4

Figure 3: Centred and normalized coefficients from the model fit for the first and

second retention factor, respectively, for (a) TSO and (b) BINOL. The error bars

represent the 95% confidence interval of the coefficients. The height of a negative

or positive bar in the plot shows the relative degree of impact of corresponding

parameter. Adapted with permission from reference 9.

Figure 4: Contour plots showing the retention factor (k) as a function of pressure

and amount of methanol in the eluent: (a) k1 for TSO, (b) k2 for TSO, (c) k1 BINOL,

and (d) k2 BINOL. Adapted with permission from reference 9.

SFC is a complicated

chromatographic

method and the same

instrumental set

conditions do not

necessarily give the

same actual working

conditions over the

column on different

systems for a variety of

reasons.

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31www.chromatographyonline.com

COLUMN WATCH

This sensitivity and back pressure

difference between systems probably

explains the observed differences in

retention volumes mentioned earlier.

Design of Experimental-Based

Investigation: We used DoE to

investigate the impact on retention by

cosolvent, pressure, and temperature

in the column (9). These three

factors and their interactions were

studied for two different solutes.

The coefficients of the second

order polynomial were estimated

by least squares regression. The

regression model for each response

was evaluated with analysis of

variance (ANOVA). The model was

refined by first removing statistical

outliers and then removing any

statistically insignificant terms from

the polynomial at a 95% confidence

level.

To study the dependency

and variation of common

chromatographic parameters such

as retention factors, selectivity, and

productivity with parameters such as

amount of cosolvent, temperature,

and pressure, the true parameter

values in the chromatographic

column must be used rather than the

values set on the instrument. The

true values were determined by using

external measurements of pressure,

temperature, and mass flow. To

verify the set volumetric flow rate,

the corresponding density of the

mobile phase fluid was calculated

using the Kunz and Wagner equation

of state as implemented by the

National Institute of Standards and

Technologies in a database software

used in science research (11).

Interestingly, the deviation between

the set and estimated volumetric flow

rate, temperature, and pressure was

found to be relatively small for most

experimental conditions used.

Parameters of Importance

for Retention Factors: Before a

successful method development can

be performed in SFC, it is essential

to have knowledge about and to be

able to predict how the retention

factor is affected by a certain

change of the operating parameters

(that is, the variables). The centred

and normalized coefficients for

the retention factor models are

presented in Figure 3. Here the test

solutes studied were trans-stilbene

oxide (TSO) and 1,1′-bi-2-naphthol

(BINOL). In particular, Figure 3

shows the impact of different

operation parameters on the retention

factors for the first and second

enantiomer of TSO and BIONOL. The

height of positive or negative bar in

the plot shows the relative degree

of impact of the corresponding

operational parameter. The

operational parameters are

denoted in the x-axis: pressure

(P), methanol fraction (CM), and

column temperature (T ); significant

values of the quadratic and more

complex term on the x axis indicate

nonlinear dependencies. In Figure 3,

it is clear that the volumetric CM

was the most important parameter,

which is represented by the largest

coefficient value for methanol. The

methanol fraction also had a large

quadratic term (C2M), meaning that

the methanol dependence is not

linear. Pressure was the second most

important factor for the retention

factor, and the retention factors all

have similar pressure dependencies

with a slight nonlinearity (see

Figure 3). In Figure 3, it can also be

seen that the interaction terms are all

significant, that is, the coefficients

of the interaction terms are shown

to be significant. These interaction

terms would be missed if one factor

at a time were varied. Interestingly,

the effect of temperature in the

investigated region was low for both

components enantiomers, however,

slightly larger for BINOL (see

Figure 3).

Figure 4 contains contour

plots illustrating the combined

dependency of the retention factors

on methanol fraction and pressure

for TSO and BINOL, respectively,

at the fixed column temperature

30 °C. For both enantiomers of both

components, we can see that the

larger the methanol fraction and the

larger the pressure the lower (more

blue colour) the retention factors

(see Figure 4). The highest values

of the retention factors are obtained

for the second enantiomer (for both

TSO and BINOL) at combined low

methanol fractions and low pressures

(deeply red colour). It is evident

that the retention factors for both

solutes have similar trends when

studied in the methanol–pressure

plane, despite the different density

variations seen between the

experimental conditions for TSO and

BINOL.

(a) (b)TSO

2

0

Co

eff

cien

ts X

10

-224 29 34

0.4

3

5

71.2

0.8

P CM C2

MT

T (°C)

CM (

v/v

%)

pr (m

gm

in)

Figure 5: Centred and normalized coefficients with 95% confidence interval from the

model fit to the productivity for the optimum touching-band chiral separation of TSO

are plotted. In (b) the productivity is plotted as a function of the amount of modifier in

the eluent and the temperature. Adapted with permission from reference 9.

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LC•GC Asia Paciàc March 201532

COLUMN WATCH

Parameters of Importance for

Productivity: In preparative chromatography, it is important to purify the desired components at the desired purity and for maximum productivity (that is, the amount of purified product per unit time). In a separation of the enantiomers of a racemate, the first step is to find suitable separation systems. This is achieved by screening combinations of chiral stationary phases (CSPs) and cosolvents. Typically, selectivity is maximized while k ´ is minimized. Loading studies utilizing maximum sample concentration on suitable candidate systems can then be performed. In this study, the dependency and variation of productivity on cosolvent, pressure, and temperature was studied. Either of the enantiomers of TSO was selected as target. The optimal chromatogram was chosen to maximize injection volume while maintaining touching-band separation (that is, having a yield of 100%). The productivity was calculated by assuming that stacked injections could be performed for the separation of either enantiomer of TSO at 30 °C, 160 bar, and 5% methanol. The trends in productivity were very clear and analysis of parameter importance revealed that the most important factor to increase productivity was to increase the fraction of cosolvent followed by an increase of temperature (see Figure 5[a]). Therefore, by simultaneously increasing methanol content and temperature, the productivity in this case could be efficiently maximized as can be seen in Figure 5(b). By decreasing pressure, the productivity could be further increased but only marginally (data not shown). It should be noted that a complete optimization would also entail further work on the volumetric flow or concentration of the sample, but that was beyond the scope of this study. Interestingly, the selectivity for the separation of TSO increases with decreasing methanol content. Hence, in this case, maximizing selectivity will yield lower productivity.

ConclusionsThis study shows that SFC is a complicated chromatographic

method and that the same instrumental set conditions do not necessarily give the same actual working conditions over the column on different systems for a variety of reasons. Recorded elution profiles for the model compound antipyrine injected onto the same silica column on three different systems at the same set conditions were clearly different. This means that it can be hard to transfer an established separation method from one system to another, even if one is using the same column and identical instrument settings. This method transfer difficulty has implications both for analytical methods and preparative applications. For example, different separation methods are usually screened on an analytical instrument and then the selected method is transferred to a larger preparative system. A design of experimental approach was used to study the impact of a change of the most common operational parameters using neutral model compounds on mostly chiral systems. The model systems presented here — except for antipyrine separated with a silica column — consisted of racemic mixtures of TSO and BINOL and were separated using a chiral cellulose-derivative silica-based column. All input parameters were carefully measured using external sensors. The parameters investigated were column temperature, pressure, and cosolvent fraction. The methanol fraction was the most important factor for governing the retention factors, and the pressure was the second most important factor. On the other hand, the temperature did not have a significant effect on the retention factor. Increasing either the temperature or the pressure resulted in reductions of the retention factors. Although not reported here, this result was also obtained with another chiral system studied (racemic 1-phenyl-1-propanol as an analytical model compound) (10).

For preparative purification of either enantiomer of TSO, the most important parameters were found to be methanol content and temperature. The selectivity for the separation of TSO increases

with decreasing methanol content. Therefore, in this case, maximization of the selectivity will yield lower productivity. As in most forms of chromatography, compromises must also be made in SFC.

References(1) G. Guiochon and A. Tarafder, J.

Chromatogr. A. 1218, 1037–1114 (2011).

(2) A. Rajendran, J. Chromatogr. A. 1250, 227–249 (2012).

(3) A. Tarafder, K. Kaczmarski, D.P. Poe, and G. Guiochon, J. Chromatogr. A. 1258, 136–151 (2012).

(4) K. Kaczmarski, D.P. Poe, and G. Guiochon, J. Chromatogr. A 1218, 6531–6539 (2011).

(5) M. Enmark, P. Forssén, J. Samuelsson, and T. Fornstedt, J. Chromatogr. A 1312, 124–133 (2013).

(6) F. Kamarei, F. Gritti, and G. Guiochon, J. Chromatogr. A 1306, 89–96 (2013).

(7) M. Enmark, J. Samuelsson, E. Forss, P. Forssén, and T. Fornstedt, J.

Chromatogr. A 1354, 129–138 (2014). (8) A. Tarafder, C. Hudalla, P. Iraneta, and

K.J. Fountain, J. Chromatogr. A 1362, 278–293 (2014).

(9) D. Åsberg, M. Enmark, J. Samuelsson, and T. Fornstedt, J. Chromatogr. A 1374, 254–260 (2014).

(10) M. Enmark, D. Åsberg, J. Samuelsson, and T. Fornstedt, Chrom. Today 7, 14–17 (2014).

(11) E.W. Lemmon, M.L. Huber, and M.O. McLinden, NIST Standard

Reference Database 23: Reference

Fluid Thermodynamic and Transport

Properties-REFPROP, Version 9.1, (National Institute of Standards and Technology, Standard Reference Data Program, Gaithersburg, Maryland, USA, 2013).

Torgny Fornstedt is a professor in analytical chemistry and heads the internationally competitive Fundamental Separation Science Group (www.separationscience.se) at Karlstad University. The group develops and applies numerical tools to characterize, validate, and optimize analytical and preparative separation methods and has recently turned towardssupercritical fluid chromatography.Ronald E. Majors is the editor of “Column Watch,” an analytical consultant, and a member of LCGC

Asia Pacific ’s editorial advisory board. Direct correspondence about this column should be addressed to “Column Watch”, LCGC Asia

Pacific, Honeycomb West, Chester Business Park, Wrexham Road, Chester, CH4 9QH, UK, or e-mail the editor-in-chief, Alasdair Matheson, at [email protected]

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33

31st International Symposium on MicroScale Bioseparations

The 31st International

Symposium

on MicroScale

Bioseparations (MSB

2015) will be held from

26–29 April 2015 at the

Crowne Plaza Hotel,

Harbour City, Pudong,

Shanghai, P.R. China.

The symposium series

was first established

to support the field

of high-performance

capillary electrophoresis,

but now covers all major microscale bioseparation techniques including

capillary electrophoresis, nano-liquid chromatography, microfluidics, mass

spectrometry, hyphenated detection methods, pharmaceutical analysis,

biotechnology, clinical diagnostics, food and health, nanoparticles, and

advanced detection and instrumentation.

Around 70% of the planned programme will be built from submitted

abstracts, where a blind peer review with an enhanced submission requirement

has been developed to ensure a very high calibre of science being presented.

A layer of confidentiality has been introduced to protect conversations and

presentations to allow the discussion of unpublished work. The format of

MSB 2015 has evolved to create a new biotechnology track with a focus on

the practical applications of microscale separations. The presentation format

has been adapted to create an extended discussion period with each paper,

moderated by a session chair. The top three posters presented at the meeting

will be selected for oral presentation in a special session as part of the finale

of the symposium. Overall, it is the intent of this symposium to foster the

exchange of ideas at the frontiers of separation science.

Four short courses are scheduled before the conference on 26 April,

including “Immunoaffinity Capillary Electrophoresis for use in Biotechnology

Applications” presented by Prof. Norberto Guzman from New Jersey,

USA; “Multidimensional HPLC” presented by Dr. Gerard Rozing from

Karlsruhe, Germany; and “Microfluidic Devices in the Life Science: Basics

and Applications” presented by Prof. Jörg P. Butter from the University of

Copenhagen, Denmark. More details are available from the website.

Current printer and laser technology has enabled a method termed print,

cut, and laminate (PCL) fabrication that is capable of creating printable

microfluidic devices in a simple, cost-effective, and rapid manner, using

relatively commonplace office equipment. Professor James Landers will

present a lecture discussing the theory and methodology associated with each

of the steps, as well the material challenges associated with substrates and

chemistries used in this method. This will be followed by a hands-on part of

the workshop, where those involved will carry out PCL fabrication using the

necessary materials and some standard microfluidic designs.

The historical city of Shanghai has been chosen for this meeting, which will

provide excellent networking opportunities to perform scientific discussions.

On the 28 April, the organizers have planned the MSB Gala Banquet that

promises food, live music, and the opportunity to network. Registration for

the event will be limited to 395 participants to establish a “smaller meeting”

ambience with a focus on the vigorous scientific exchange between delegates.

E-mail: [email protected]

Website: msb2015.org

Co-Chairs: Yukui Zhang, Pengyuan Yang, Norman Dovichi, and Amy Y. Guo

15–17 April 2015Vietnam Analytica 2015

Saigon Exhibition & Convention Centre,

Ho Chi Minh City, Vietnam

Contact: Eva Sauerborn

E-mail: [email protected]

Website: www.analyticavietnam.com/

en/Home

17–21 May 2015ISCC and GC×GC 2015

Hilton Fort Worth Hotel, Fort Worth,

Texas, USA

Contact: Danielle Schug

E-mail: [email protected]

Website: www.isccgcxgc2015.com

30 June–3 July 201521st International Symposium on

Separation Sciences (ISSS 2015)

Grand Hotel Union, Ljubljiana,

Slovenia

Tel: +38614760265

E-mail: [email protected]

Website: www.isss2015.si

22–24 July 20159th International Conference on

Packed Column SFC

Loews Hotel, Philadelphia, USA

Tel: +1 412 805 6296

E-mail: [email protected]

Website: www.greenchemistrygroup.

org/Registration.html

21–25 September 201543rd International Symposium

on High-Performance Liquid

Phase Separations and Related

Techniques

Beijing International Convention Center

Bejing, China

Contact: HPLC Secretariat

E-mail: [email protected]

Website: hplc2015-beijing.org/

3–6 November 2015Recent Advances in Food Analysis

(RAFA)

Clarion Congress Hotel, Prague, Czech

Republic

Tel: +386 1 4760265

E-mail: [email protected]

Website: www.rafa2015.eu

Please send any event news to

Bethany Degg

[email protected]

33www.chromatographyonline.com

EVENT NEWSP

ho

to C

red

its:

Bla

cksta

tio

n/G

ett

y I

mag

es

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34 LC•GC Asia Pacifi c March 2015

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ADC2

167.8 (±1.2%)

163.7 (±1.2%)

155.2 (±1.8%)

155.6 (±1.2%)

12.6

8.1 6.5

10.1

Mw (kDa)

Mo

lar

Ma

ss (

g/m

ol)

ADC1

ADC2

Figure 2: Molar masses for the antibody and total appended drug are calculated in the ASTRA software package based on prior knowledge of each component’s extinction coeff cent and dn/dc, allowing determination of DAR based on a nominal Mw of 1250 Da for an individual drug.

2.0x105

Molar mass vs. time

167.8 kDa

ADC1

ADC2

163.7 kDa1.8x105

1.6x105

1.4x105

1.2x105

Mo

lar

Ma

ss (

g/m

ol)

1.0x105

8.0x104

9.0 9.5 10.0 10.5Time (min)

11.0 11.5 12.0

Figure 1: Molar masses for two distinct ADC formulations are determined using SEC–MALS analysis.

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