Robledo, V. (2006) Enantiomeric screening of racemic citalopram and metabolites in human urine by entangled polymer solution capillary electrophoresis: an innovatory robustness/ruggedness study *Electrophoresis 27*,

in brain cancers: a tool for rational drug development, *Expert Opin Drug Metab*

HT receptor antagonist M100,907 prevents extracellular glutamate rising in response to NMDA receptor blockade in the mPFC. , *J Neurochem 91*, 189-199. Chu, M., Huang, Z., Qu, W., Eguchi, N., Yao, M., and Urade, Y. (2004) Chu, M. et al.

Extracellular histamine level in the frontal cortex is positively correlated with the

metabolites, demethylcitalopram (DCIT), didemethylcitalopram (DDCIT), and citalopram N-oxide (CIT-NO) in human plasma and urine (31-32). Due to lack of commercial standards of citalopram metabolite, their concentration in microdialysate could not be measured in this study.

These examples illustrate the applicability of the LC-MS/MS coupled to *in vivo* microdialysis technique to rapidly estimate the PK/PD profiles of novel substances. This technique will be a very useful tool to study the drug penetration of BBB in lead optimization of drug discovery. Compared to the traditional method for the study of drug BBB penetration (33), this technique avoids having to euthanize the animal at each time point to measure drug concentration in whole brain tissue and provides continually monitoring extracellular drug concentration in specific brain regions at each hour for a 24 hour period by using a single animal as shown in table 2.

Table 2. Comparison of drug blood-brain barrier (BBB) penetration study by using traditional method versus *in vivo* microdialysis-LC/MS/MS method.

#### **5. Conclusion**

This study demonstrated that liquid Chromatography/tandem mass spectrometry (LC-MS/MS) coupled with *in vivo* microdialysis provides a powerful method for the measurement of endogenous and exogenous substances in the brain interstitial fluid (ISF) surrounding the probe and so it represents an important tool in CNS drug discovery. 1). It can be used to measure the pharmacodynamic response of neuroactive compounds, represents the **drug efficacy**, by measuring neurotransmitters and other biomarkers; 2). A core requirement for an effective CNS drug is an ability to cross the BBB and remain in the brain ISF for sufficient duration and concentration to evoke the desired therapeutic effect. LC-MS/MS coupled with *in vivo* microdialysis can be used to evaluate the **BBB penetration** of drug candidate by measuring the free concentration of CNS drug in brain ISF; 3). The profile of time-free concentration of CNS drug in the targeted brain region provides **biophase pharmacokinetic** information which can differ significantly from pharmacokinetics in plasma. Establishing **PK-PD relationship** of the drug, especially biophase PK, allow better understanding of exposure-response relationships and help the selection of drug; 4). In some case, not parent drug, but **drug metabolite** contributes to efficacy or toxicity. LC-MS/MS coupled with *in vivo* microdialysis also can be used to study drug metabolism during drug discovery.

#### **6. Acknowledgments**

436 Tandem Mass Spectrometry – Applications and Principles

metabolites, demethylcitalopram (DCIT), didemethylcitalopram (DDCIT), and citalopram N-oxide (CIT-NO) in human plasma and urine (31-32). Due to lack of commercial standards of citalopram metabolite, their concentration in microdialysate could not be measured in

These examples illustrate the applicability of the LC-MS/MS coupled to *in vivo* microdialysis technique to rapidly estimate the PK/PD profiles of novel substances. This technique will be a very useful tool to study the drug penetration of BBB in lead optimization of drug discovery. Compared to the traditional method for the study of drug BBB penetration (33), this technique avoids having to euthanize the animal at each time point to measure drug concentration in whole brain tissue and provides continually monitoring extracellular drug concentration in specific brain regions at each hour for a 24-

Traditional Method *In vivo* microdialysis-LC/MS/MS method

 Sample from individual brain region (such as frontal cortex, striatum, hippocampus, hypothalamus) Measure extracellular drug concentration

 Using 1 animal to get 24 time points Automatic sample collection for 24 hours without supervision. Only need to implant microdialysis probe guide by brain surgery. Sample ready for LC injection

 PK and PD data (both drug and biomarker concentration)

hour period by using a single animal as shown in table 2.

Specificity Using whole brain tissue

Efficiency Using 8 animals to get 8 time points

Information PK data (drug concentration

**5.  Comparison of drug blood-brain barrier (BBB) penetration study by using

This study demonstrated that liquid Chromatography/tandem mass spectrometry (LC-MS/MS) coupled with *in vivo* microdialysis provides a powerful method for the measurement of endogenous and exogenous substances in the brain interstitial fluid (ISF) surrounding the probe and so it represents an important tool in CNS drug discovery. 1). It can be used to measure the pharmacodynamic response of neuroactive compounds, represents the **drug efficacy**, by measuring neurotransmitters and other biomarkers; 2). A

injection

in the brain)

traditional method versus *in vivo* microdialysis-LC/MS/MS method.

this study.

This work was supported in part by Excellence in Science Grant of the Johnson & Johnson Corporate Office of Science and Technology. The authors gratefully acknowledge Dr. Michael Ye (Supelco/Sigma-Aldrich Inc.) for his suggestion of using pentafluorophenyl (Discovery HS F5) column; Dr.Jiejun Wu and Kenway Hoey for LC-MS/MS technique training and support; Dr. Pascal Bonaventure for helpful discussions during the experiments and writing the chapter draft.

#### **7. References**

Evaluating PK/PD Relationship of CNS Drug

*Pharmacol 81*, 216-222.

839-849.

193.

2231-2236.

San Diego.

587.

186.

man, *J Intern Med 230*, 365-373.

*Neurosci Methods 127*, 11-17.

*Biomed Anal 40*, 492-499.

by Using Liquid Chromtography/Tandem Mass Spectrometry Coupled to *In Vivo* Microdialysis 439

Kosasa, T., Kuriya, Y., and Yamanishi, Y. (1999) Effect of donepezil hydrochloride (E2020)

Lacroix, L., Hows, M., Shah, A., Hagan, J., and Heidbreder, C. (2003) Selective antagonism at

Li, J., Shao, S., Jaworsky, M., and Kurtulik, P. (2008) Simultaneous determination of cations,

Maura, G., and Raiteri, M. (1986) Cholinergic terminals in rat hippocampus possess 5-HT1B

Millan, M., Dekeyne, A., Papp, M., La Rochelle, C., MacSweeny, C., Peglion, J., and Brocco,

Needham, S., Brown, P., and Duff, K. (1999) Phenyl ring structures as stationary phases for

Paxinos, G., and Watson, C. (1997) *The Rat Brain in Stereotaxic Coordinates,* Academic Press

Plock, N., and Kloft, C. (2005) Microdialysis--theoretical background and recent

Titier, K., Castaing, N., Scotto-Gomez, E., Pehourcq, F., Moore, N., and Molimard, M. (2003)

Trabace, L., Cassano, T., Cagiano, R., Tattoli, M., Pietra, C., Steardo, L., Kendrick, K., and

Ungerstedt, U. (1991) Microdialysis--principles and applications for studies in animals and

Yoshitake, T., Yamaguchi, M., Nohta, H., Ichinose, F., Yoshida, H., Yoshitake, S., Fuxe, K.,

Zhang, M. Y. B., C.E. (2006) Measurement of neurotransmitters from extracellular fluid in

implementation in applied life-sciences, *Eur J Pharm Sci 25*, 1-24.

clomipramine, *J Pharmacol Exp Ther 298*, 581-591.

on extracellular acetylcholine concentration in the cerebral cortex of rats *Jpn J*

dopamine D3 receptors enhances monoaminergic and cholinergic neurotransmission in the rat anterior cingulate cortex *Neuropsychopharmacology 28*,

zwitterions and neutral compounds using mixed-mode reversed-phase and cationexchange high-performance liquid chromatography *J Chromatogr A 1185*, 185-

receptors mediating inhibition of acetylcholine release, *Eur J Pharmacol 129*, 333-337.

M. (2001) S33005, a novel ligand at both serotonin and norepinephrine transporters: II. Behavioral profile in comparison with venlafaxine, reboxetine, citalopram, and

the high performance liquid chromatography electrospray ionization mass spectrometric analysis of basic pharmaceuticals, *Rapid Commun Mass Spectrom 13*,

Titier, K. et al. High-performance liquid chromatographic method with diode array detection for identification and quantification of the eight new antidepressants and five of their active metabolites in plasma after overdose *Ther Drug Monit 25*, 581-

Cuomo, V. (2001) Trabace, L. et al. Effects of ENA713 and CHF2819, two anti-Alzheimer's disease drugs, on rat amino acid levels, *Brain Res. 910*, 182-

and Kehr, J. (2003) Yoshitake, T. et al. Determination of histamine in microdialysis samples from rat brain by microbore column liquid chromatography following intramolecular excimer-forming derivatization with pyrene-labeling reagent *J*

brain by in vivo microdialysis and chromatography-mass spectrometry *J Pharm*

David, D., Bourin, M., Jego, G., Przybylski, C., Jolliet, P., and Gardier, A. (2003) David, D.J.

de Lange, E., Ravenstijn, P., Groenendaal, D., and van Steeg, T. (2005) Toward the prediction

Del Arco, A., and Mora, F. (2000) Endogenous dopamine potentiates the effects of glutamate

Felton, T., Kang, T., Hjorth, S., and Auerbach, S. (2003) Effects of selective serotonin and

Giacobini, E., Zhu, X., Williams, E., and Sherman, K. (1996) The effect of the selective

Hows, M., Lacroix, L., Heidbreder, C., Organ, A., and Shah, A. (2004) High-performance

Hows, M., Organ, A., Murray, S., Dawson, L., Foxton, R., Heidbreder, C., Hughes, Z.,

Ichikawa, J., Dai, J., and Meltzer, H. (2000) Acetylcholinesterase Inhibitors are neither

Ichikawa, J., Dai, J., O'Laughlin, I., Fowler, W., and Meltzer, H. (2002) Atypical, but not

in the nucleus accumbens or striatum *Neuropsychopharmacology 26*, 325-339. Kawashima, K., Sato, A., Yoshizawa, M., Fujii, T., Fujimoto, K., and Suzuki, T. (1994) Effects

freely moving rats *Naunyn Schmiedebergs Arch Pharmacol 350*, 523-528. Keski-Rahkonen, P., Lehtonen, M., Ihalainen, J., Sarajarvi, T., and Auriola, S. (2007)

Kissinger, P. (1989) Biomedical applications of liquid chromatography-electrochemistry, *J*

biogenic amine levels in rat cortex *Neuropharmacology 35*, 205-211.

acetylcholine from microdialysates *J Neurosci Methods 121*, 33-39.

biological samples *J Neurosci Methods 138*, 123-132.

*Pharmacol 140*, 1128-1136.

*Bull 53*, 339-345.

*Separation 19*, 37-43.

*Commun Mass Spectrom 21*, 2933-2943.

*Chromatogr. 488*, 31-52.

305.

modeling, *AAPS J 7*, E532-543.

et al. Effects of acute treatment with paroxetine, citalopram and venlafaxine in vivo on noradrenaline and serotonin outflow: a microdialysis study in Swiss mice, *Br J*

of CNS drug-effect profiles in physiological and pathological conditions using microdialysis and mechanism-based pharmacokinetic-pharmacodynamic

on extracellular GABA in the prefrontal cortex of the freely moving rat, *Brain Res*

serotonin/noradrenaline reuptake inhibitors on extracellular serotonin in rat diencephalon and frontal cortex, *Naunyn Schmiedebergs Arch Pharmacol 367*, 297-

reversible acetylcholinesterase inhibitor E2020 on extracellular acetylcholine and

liquid chromatography/tandem mass spectrometric assay for the simultaneous measurement of dopamine, norepinephrine, 5-hydroxytryptamine and cocaine in

Lacroix, L., and Shah, A. (2002) High-performance liquid chromatography/tandem mass spectrometry assay for the rapid high sensitivity measurement of basal

necessary nor desirable for microdialysis studies of brain acetylcholine *Current*

typical, antipsychotic drugs increase cortical acetylcholine release without an effect

of the centrally acting cholinesterase inhibitors tetrahydroaminoacridine and E2020 on the basal concentration of extracellular acetylcholine in the hippocampus of

Quantitative determination of acetylcholine in microdialysis samples using liquid chromatography/atmospheric pressure spray ionization mass spectrometry *Rapid*

**20**

Ju-Seop Kang

*South Korea*

*Hanyang University, Seoul,*

**Principles and Applications of LC-MS/MS for the**

*Department of Pharmacology & Clinical Pharmacology Laboratory, College of Medicine; Division of Molecular Therapeutics Development, Hanyang Biomedical Research Institute,*

Standard technology for analyte detection in clinical chemistry fields rely on indirect characteristics of an analyte, e.g. its absorption capability of light, chemical reactivity or physicochemical interaction with macro-molecules as like antigen-antibody interaction. Otherwise, analytes are detected directly from molecular characteristics as molecular mass and molecular disintegration patterns in mass spectrometric method. Thus, mass spectrometric technology are very attractive for the quantification of biomarkers or chemicals in the context of diagnostic procedures since those techniques can be provide higher quality of analysis of much higher specificity compared to standard technologies such as photometry or ligand-binding tests. Even if gas chromatography-mass spectrometry (GC-MS) is first introduced mass spectrometric methods to laboratory medicine about 40 years ago and provide highly specific and sensitive quantification of thermo-stable molecules below a molecular weight of about 500, application of GC-MS method remained restricted to few specialized institution in laboratory medicine such as mainly toxicology laboratories, medical centres, and reference laboratories. The handling and maintenance of GC-MS instruments is very demanding and time-consuming; sample preparation is very laborious and includes procedures of sample extraction and analyte derivatisations and long run time with a typical sample throughput of less than 50 samples per day. Over the past decade with introduction of atmospheric pressure ionization (API) techniques, liquid chromatography-mass spectrometry (LC-MS) has undergone tremendous technological improvement allowing for its applications to endogenous components such as proteins, peptides, carbohydrates, DNA, and drugs or metabolites. Furthermore, powerful new technologies of ion-analyses (tandem MS, timeof-flight MS, ion-trap MS) substantially increased the capabilities of MS analyzers with respect to specificity and to the extent of data read out. These developments suggest a more widespread use of MS techniques superior to other analytical methods in routine

The aims of this chapter is to comprehensively characterize the basic principles of mass spectrometric detection, recent development of MS, bottleneck of LC-MS method associate

**1. Introduction**

laboratory medicine.

**Quantitative Bioanalysis of Analytes**

**in Various Biological Samples**

Zhu, Y., Wong, P., Cregor, M., Gitzen, J., Coury, L., and Kissinger, P. (2000) Zhu, Y. et al. In vivo microdialysis and reverse phase ion pair liquid chromatography/tandem mass spectrometry for the determination and identification of acetylcholine and related compounds in rat brain. Rapid Commun Mass Spectrom *Rapid Commun Mass Spectrom 14*, 1695-1700.

### **Principles and Applications of LC-MS/MS for the Quantitative Bioanalysis of Analytes in Various Biological Samples**

Ju-Seop Kang

*Department of Pharmacology & Clinical Pharmacology Laboratory, College of Medicine; Division of Molecular Therapeutics Development, Hanyang Biomedical Research Institute, Hanyang University, Seoul, South Korea*

#### **1. Introduction**

440 Tandem Mass Spectrometry – Applications and Principles

Zhu, Y., Wong, P., Cregor, M., Gitzen, J., Coury, L., and Kissinger, P. (2000) Zhu, Y. et al. In

*Mass Spectrom 14*, 1695-1700.

vivo microdialysis and reverse phase ion pair liquid chromatography/tandem mass spectrometry for the determination and identification of acetylcholine and related compounds in rat brain. Rapid Commun Mass Spectrom *Rapid Commun*

> Standard technology for analyte detection in clinical chemistry fields rely on indirect characteristics of an analyte, e.g. its absorption capability of light, chemical reactivity or physicochemical interaction with macro-molecules as like antigen-antibody interaction. Otherwise, analytes are detected directly from molecular characteristics as molecular mass and molecular disintegration patterns in mass spectrometric method. Thus, mass spectrometric technology are very attractive for the quantification of biomarkers or chemicals in the context of diagnostic procedures since those techniques can be provide higher quality of analysis of much higher specificity compared to standard technologies such as photometry or ligand-binding tests. Even if gas chromatography-mass spectrometry (GC-MS) is first introduced mass spectrometric methods to laboratory medicine about 40 years ago and provide highly specific and sensitive quantification of thermo-stable molecules below a molecular weight of about 500, application of GC-MS method remained restricted to few specialized institution in laboratory medicine such as mainly toxicology laboratories, medical centres, and reference laboratories. The handling and maintenance of GC-MS instruments is very demanding and time-consuming; sample preparation is very laborious and includes procedures of sample extraction and analyte derivatisations and long run time with a typical sample throughput of less than 50 samples per day. Over the past decade with introduction of atmospheric pressure ionization (API) techniques, liquid chromatography-mass spectrometry (LC-MS) has undergone tremendous technological improvement allowing for its applications to endogenous components such as proteins, peptides, carbohydrates, DNA, and drugs or metabolites. Furthermore, powerful new technologies of ion-analyses (tandem MS, timeof-flight MS, ion-trap MS) substantially increased the capabilities of MS analyzers with respect to specificity and to the extent of data read out. These developments suggest a more widespread use of MS techniques superior to other analytical methods in routine laboratory medicine.

> The aims of this chapter is to comprehensively characterize the basic principles of mass spectrometric detection, recent development of MS, bottleneck of LC-MS method associate

Principles and Applications of LC-MS/MS

Fig. 1. Diagram of mass spectrometer system.

in neutralization.

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 443

ions cannot collide with any other forms of matter during the separation process. Ions of individual *m/z* values are separated and detected in order to obtain the mass spectrum. Separation of ions in an evacuated environment is mandatory. If an ion collides with neutrals in an elastic collision during ion separation process, the ion's direction of travel could be altered and ion might not reach the detector. If an ion's collision with neutral is inelastic, sufficient energy transfer may cause it to decompose, meaning that the original ion will not be detected. Close encounters between ions of the same charge can be cause deflection in the path of each. Direct contact between ions of opposite charge sign will result

Ions are positively or negatively charged atoms, groups of atoms, or molecules. The process whereby an electrically neutral atom or molecule becomes electrically charged, due to losing or gaining one or more of its extra nuclear electrons, is called ionization (Chiu & Muddiman, 2008). Although both positive and negative ions can be analyzed by MS, the majority of instruments are used to investigate positive ions because in most ion sources they are

There is a minimum amount of energy, characterized by the "ionization potential," that must be provided in order for ion formation to occur. The first ionization potential of an atom or molecule is defined as the energy input required removing (to infinite distance) a valence electron from the highest occupied atomic or molecular orbital of the neutral particle to form the corresponding atomic or molecular ion, also in its ground state. When

produced in larger number than negative ions. (Chiu & Muddiman, 2008)

with matrix effect, application fields of LC with tandem MS in basic and clinical laboratory fields such as drug discovery and development, drug metabolism and toxicology studies, quantification of biogenic amines, doping control, TDM and pharmacokinetic (PK) studies.

#### **2. Basic principles of mass spectrometric detection**

Mass spectrometry (MS) has been described as the smallest scale in the world, not because of its size of what it weighs a molecule and a microanalytical technique that can be used selectively to detect and determine the amount of a given analyte (Watson & Sparkman, 2007; Chiu & Muddiman, 2008). MS is also used to determine the elemental composition and some aspect of the molecular structure of an analyte. Unique features of MS include its capacity for direct determination of the nominal mass of an analyte, and to produce and detect fragments of the molecule that correspond to discrete groups of atoms of different elements that reveal structure features (Watson & Sparkman, 2007). The tools of MS are mass spectrometers, and data are called mass spectra that can be displayed in many different ways, which allow the desired information about the analyte to be easily extracted (Watson & Sparkman, 2007). A MS is an apparatus which produces a beam of gaseous ions from a sample, sorts out the resulting mixture of ions according to their mass-to-charge ratios, and provides output signals which are measures of relative abundance of each ionic species present. MS are usually classified on the basis of how the mass separation is accomplished, but they all can be described as ion optical devices which separate ions according to their mass-to-charge (*m/z*) ratios by utilizing electric and/or magnetic force fields (Figure. 1). The concept of MS is to form ions from a sample, to separate the ions based on their *m/z* ratio (this can be considered to be the same as the mass because the ion has only a single charge in most cases), and to measure the abundance of the ions. In modern MS instrumentation used in environmental analyses, all of the functions (ionization separation of the ions, rate of data acquisition, detection of the ions, and storage of the data) are under computer control. Gaseous molecules are ionized in the ion source to form molecular ions which some of that will fragment. By various processes, ions of differing *m/z* values pass through the mass analyzer one at a time to reach the detector. When the ions strike the detector, they are converted into an electrical signal which, in turn, is converted into a digital response that can be stored by the computer (Sparkman, 2000).

A mass specterometer does not directly determine mass but, determines the mass of a molecule by measuring the *m/z* of its ion. The knowledge of the *m/z* of the ions enables one to determine what is present, while the measured ion intensities answer the question of how much is present. In addition, systematic interpretation of the mass spectra provides a detailed picture of the ionization process which, in turn, may be utilized in the elucidation of molecular structures. This definition of the term *m/z* is important to understanding of MS. It should be noted that the *m/z* value is a dimensionless number that is always used as an adjective, e.g. the ions with *m/z* 256, or the ion has an *m/z* value of 256. A recording of the number of ions (abundance) of a given *m/z* value as a function of the *m/z* value is a mass spectrum (Watson & Sparkman, 2007). The mass component that makes up the dimensionless *m/z* unit is based on an atomic scale rather than the physical scale normally considered as mass. Only ions are detected in mass specterometer and any nonionic particles that have no charge are removed from the mass spectrometer by the continuous pumping that maintains the vacuum. The MS first must produce a collection of ions in the gas phase. These ions are separated according to their *m/z* values in a vacuum where the

with matrix effect, application fields of LC with tandem MS in basic and clinical laboratory fields such as drug discovery and development, drug metabolism and toxicology studies, quantification of biogenic amines, doping control, TDM and pharmacokinetic (PK) studies.

Mass spectrometry (MS) has been described as the smallest scale in the world, not because of its size of what it weighs a molecule and a microanalytical technique that can be used selectively to detect and determine the amount of a given analyte (Watson & Sparkman, 2007; Chiu & Muddiman, 2008). MS is also used to determine the elemental composition and some aspect of the molecular structure of an analyte. Unique features of MS include its capacity for direct determination of the nominal mass of an analyte, and to produce and detect fragments of the molecule that correspond to discrete groups of atoms of different elements that reveal structure features (Watson & Sparkman, 2007). The tools of MS are mass spectrometers, and data are called mass spectra that can be displayed in many different ways, which allow the desired information about the analyte to be easily extracted (Watson & Sparkman, 2007). A MS is an apparatus which produces a beam of gaseous ions from a sample, sorts out the resulting mixture of ions according to their mass-to-charge ratios, and provides output signals which are measures of relative abundance of each ionic species present. MS are usually classified on the basis of how the mass separation is accomplished, but they all can be described as ion optical devices which separate ions according to their mass-to-charge (*m/z*) ratios by utilizing electric and/or magnetic force fields (Figure. 1). The concept of MS is to form ions from a sample, to separate the ions based on their *m/z* ratio (this can be considered to be the same as the mass because the ion has only a single charge in most cases), and to measure the abundance of the ions. In modern MS instrumentation used in environmental analyses, all of the functions (ionization separation of the ions, rate of data acquisition, detection of the ions, and storage of the data) are under computer control. Gaseous molecules are ionized in the ion source to form molecular ions which some of that will fragment. By various processes, ions of differing *m/z* values pass through the mass analyzer one at a time to reach the detector. When the ions strike the detector, they are converted into an electrical signal which, in turn, is converted

**2. Basic principles of mass spectrometric detection**

into a digital response that can be stored by the computer (Sparkman, 2000).

A mass specterometer does not directly determine mass but, determines the mass of a molecule by measuring the *m/z* of its ion. The knowledge of the *m/z* of the ions enables one to determine what is present, while the measured ion intensities answer the question of how much is present. In addition, systematic interpretation of the mass spectra provides a detailed picture of the ionization process which, in turn, may be utilized in the elucidation of molecular structures. This definition of the term *m/z* is important to understanding of MS. It should be noted that the *m/z* value is a dimensionless number that is always used as an adjective, e.g. the ions with *m/z* 256, or the ion has an *m/z* value of 256. A recording of the number of ions (abundance) of a given *m/z* value as a function of the *m/z* value is a mass spectrum (Watson & Sparkman, 2007). The mass component that makes up the dimensionless *m/z* unit is based on an atomic scale rather than the physical scale normally considered as mass. Only ions are detected in mass specterometer and any nonionic particles that have no charge are removed from the mass spectrometer by the continuous pumping that maintains the vacuum. The MS first must produce a collection of ions in the gas phase. These ions are separated according to their *m/z* values in a vacuum where the

Fig. 1. Diagram of mass spectrometer system.

ions cannot collide with any other forms of matter during the separation process. Ions of individual *m/z* values are separated and detected in order to obtain the mass spectrum. Separation of ions in an evacuated environment is mandatory. If an ion collides with neutrals in an elastic collision during ion separation process, the ion's direction of travel could be altered and ion might not reach the detector. If an ion's collision with neutral is inelastic, sufficient energy transfer may cause it to decompose, meaning that the original ion will not be detected. Close encounters between ions of the same charge can be cause deflection in the path of each. Direct contact between ions of opposite charge sign will result in neutralization.

Ions are positively or negatively charged atoms, groups of atoms, or molecules. The process whereby an electrically neutral atom or molecule becomes electrically charged, due to losing or gaining one or more of its extra nuclear electrons, is called ionization (Chiu & Muddiman, 2008). Although both positive and negative ions can be analyzed by MS, the majority of instruments are used to investigate positive ions because in most ion sources they are produced in larger number than negative ions. (Chiu & Muddiman, 2008)

There is a minimum amount of energy, characterized by the "ionization potential," that must be provided in order for ion formation to occur. The first ionization potential of an atom or molecule is defined as the energy input required removing (to infinite distance) a valence electron from the highest occupied atomic or molecular orbital of the neutral particle to form the corresponding atomic or molecular ion, also in its ground state. When

Principles and Applications of LC-MS/MS

Encyclopedia).

variety of compounds.

**2.2 Basic principles of mass spectrometric detection**

into the ionization source such as ESI-MS (Chiu & Muddiman, 2008).

**2.2.1 Sample Introduction Techniques**

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 445

an analyzer according to their *m/z* ratios through the use of electromagnetic fields, (4) detector; the ions then pass through a detector where the ion flux is converted into a propertional electrical current and (5) date conversion; the magnitude of the ion/electrical

Fig. 3. Simplified diagram and function of instrumentation of typical mass spectromer (Image Source: The University of Hull, Mass Spectrometry Principles and Interpretation,

MS instruments consist of three modules: an ion source, which can convert gas phase sample molecules into ions (or, in the case of ESI, move ions that exist in solution into the gas phase); a mass analyzer*,* which sorts the ions by their masses by applying electromagnetic fields; and *a* detector, which measures the value of an indicator quantity and thus provides data for calculating the abundances of each ion present. The technique has both qualitative and quantitative uses. These include identifying unknown compounds, determining the isotopic composition of elements in a molecule, and determining the structure of a compound by observing its fragmentation. Other uses include quantifying the amount of a compound in a sample or studying the fundamentals of gas phase ion chemistry (the chemistry of ions and neutrals in a vacuum). MS is now in very common use in analytical laboratories that study physical, chemical, or biological properties of a great

Sample introduction was an early challenge in MS. In order to perform mass analysis on a sample, which is initially at atmospheric pressure (760 torr), it must be introduced into the instrument in such a way that the vacuum inside the instrument remains relatively unchanged (~10-6 torr). The most common methods of sample introduction are direct insertion with a probe or plate commonly used with MALDI-MS, direct infusion or injection

1) Direct insertion: Using an insertion probe/plate is a very simple way to introduce a sample into an instrument. The sample is first placed onto a probe and then directly inserted into the ionization region of the mass spectrometer, typically through a vacuum interlock.

signals is converted into a mass spectrum (Watson & Sparkman , 2007).

only one electron is removed the ion is called an atomic or molecular ion; often the term "parent ion" is used. The formation of parent ions may be considered as ionization without cleavage. The numerical magnitude of the ionization potential is influenced by such factors as the charge upon the nucleus, the atomic or molecular radius, the shielding effect of the inner electronic shells, and the extent to which the most loosely bound electrons penetrate the cloud of electric charge of the inner shells (Figure 2).

Fig. 2. Ionization potential (http://www.britannica.com/EBchecked/media/647/Firstionization-energies-of-the-elements).

Because only ions can be detected in MS, any particles that are not ionic (molecules or radicals) are removed from the MS by the continuous pumping that maintains the vacuum. When only individual ions are present, they can be grouped according to their unique properties (mass and number of charges) and moved freely from one point to another. In order to have individual ions free from any other forms of matter, it is necessary to analyze them in a vacuum, which means that the ions must be in the gas phase. It is a fundamental requirement of MS that ions be in the gas phase before they can be separated according to their individual *m/z* values and detected (Watson & Sparkman , 2007).

Due to ionization sources such as electrospray ionization (ESI) and matrix-assisted laser desorption/ionization (MALDI), MS has become an irreplaceable tool in the biological sciences. Over the past decade, MS has undergone tremendous technological improvements allowing for its application to proteins, peptides, carbohydrates, DNA, drugs, and many other biologically relevant molecules (Chiu & Muddiman, 2008).

#### **2.1 Instrumentation of mass spectrometric detection**

Mass spectrometry is a particularly powerful scientific technique because it can be successfully applied even if you have only a tiny quantity available for analysis—as little as 10-12 g, 10-15 moles for a compound of mass 1000 Daltons(Da). Compounds can be identified through mass spectrometry at very low concentrations (one part in 1012) in chemically complex mixtures. The basic mass spectrometry processes of instrumentation are consisted of (1) introduction of sample; a sample which can be a solid, liquid, or vapor is loaded onto a mass spectrometry device and is vaporized, (2) ionization; sample components are ionized by one of several available methods to create ions, (3) analyzer sorting; the ions are sorted in

only one electron is removed the ion is called an atomic or molecular ion; often the term "parent ion" is used. The formation of parent ions may be considered as ionization without cleavage. The numerical magnitude of the ionization potential is influenced by such factors as the charge upon the nucleus, the atomic or molecular radius, the shielding effect of the inner electronic shells, and the extent to which the most loosely bound electrons penetrate

Fig. 2. Ionization potential (http://www.britannica.com/EBchecked/media/647/First-

their individual *m/z* values and detected (Watson & Sparkman , 2007).

other biologically relevant molecules (Chiu & Muddiman, 2008).

**2.1 Instrumentation of mass spectrometric detection**

Because only ions can be detected in MS, any particles that are not ionic (molecules or radicals) are removed from the MS by the continuous pumping that maintains the vacuum. When only individual ions are present, they can be grouped according to their unique properties (mass and number of charges) and moved freely from one point to another. In order to have individual ions free from any other forms of matter, it is necessary to analyze them in a vacuum, which means that the ions must be in the gas phase. It is a fundamental requirement of MS that ions be in the gas phase before they can be separated according to

Due to ionization sources such as electrospray ionization (ESI) and matrix-assisted laser desorption/ionization (MALDI), MS has become an irreplaceable tool in the biological sciences. Over the past decade, MS has undergone tremendous technological improvements allowing for its application to proteins, peptides, carbohydrates, DNA, drugs, and many

Mass spectrometry is a particularly powerful scientific technique because it can be successfully applied even if you have only a tiny quantity available for analysis—as little as 10-12 g, 10-15 moles for a compound of mass 1000 Daltons(Da). Compounds can be identified through mass spectrometry at very low concentrations (one part in 1012) in chemically complex mixtures. The basic mass spectrometry processes of instrumentation are consisted of (1) introduction of sample; a sample which can be a solid, liquid, or vapor is loaded onto a mass spectrometry device and is vaporized, (2) ionization; sample components are ionized by one of several available methods to create ions, (3) analyzer sorting; the ions are sorted in

the cloud of electric charge of the inner shells (Figure 2).

ionization-energies-of-the-elements).

an analyzer according to their *m/z* ratios through the use of electromagnetic fields, (4) detector; the ions then pass through a detector where the ion flux is converted into a propertional electrical current and (5) date conversion; the magnitude of the ion/electrical signals is converted into a mass spectrum (Watson & Sparkman , 2007).

Fig. 3. Simplified diagram and function of instrumentation of typical mass spectromer (Image Source: The University of Hull, Mass Spectrometry Principles and Interpretation, Encyclopedia).

MS instruments consist of three modules: an ion source, which can convert gas phase sample molecules into ions (or, in the case of ESI, move ions that exist in solution into the gas phase); a mass analyzer*,* which sorts the ions by their masses by applying electromagnetic fields; and *a* detector, which measures the value of an indicator quantity and thus provides data for calculating the abundances of each ion present. The technique has both qualitative and quantitative uses. These include identifying unknown compounds, determining the isotopic composition of elements in a molecule, and determining the structure of a compound by observing its fragmentation. Other uses include quantifying the amount of a compound in a sample or studying the fundamentals of gas phase ion chemistry (the chemistry of ions and neutrals in a vacuum). MS is now in very common use in analytical laboratories that study physical, chemical, or biological properties of a great variety of compounds.

#### **2.2 Basic principles of mass spectrometric detection 2.2.1 Sample Introduction Techniques**

Sample introduction was an early challenge in MS. In order to perform mass analysis on a sample, which is initially at atmospheric pressure (760 torr), it must be introduced into the instrument in such a way that the vacuum inside the instrument remains relatively unchanged (~10-6 torr). The most common methods of sample introduction are direct insertion with a probe or plate commonly used with MALDI-MS, direct infusion or injection into the ionization source such as ESI-MS (Chiu & Muddiman, 2008).

1) Direct insertion: Using an insertion probe/plate is a very simple way to introduce a sample into an instrument. The sample is first placed onto a probe and then directly inserted into the ionization region of the mass spectrometer, typically through a vacuum interlock.

Principles and Applications of LC-MS/MS

and MALDI.

**2.2.3 Ionization sources**

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 447

condensed phase into the gas phase. This transfer is commonly achieved via ESI, APCI, FAB

Electron ejection achieves ionization through the ejection of an electron to produce a 1+ net positive charge, often forming radical cations. Observed most commonly with electron ionization (EI) sources, electron ejection is usually performed on relatively nonpolar compounds with low molecular weights and it is also known to generate significant fragment ions. It can provide observation of EI and can provide molecular mass as well as fragmentation information. However, it often generate too much fragmentation and can be

With the electron capture ionization method, a net negative charge of -1 is achieved with the absorption or capture of an electron. It is a mechanism of ionization primarily observed for molecules with a high electron affinity, such as halogenated compounds. It can provide observation of electron ionization and can provide molecular mass as well as fragmentation information. However, it often generate too much fragmentation and can be unclear whether the highest mass ion is the molecular ion or a fragment (Chiu & Muddiman, 2008).

The ion source is the part of the mass spectrometer that ionizes the material under analysis (the analyte). Ionization methods include the following; APCI, CI, EI, ESI, fast atom/ion bombardment (FAB), field desorption/field ionization (FD/FI), MALDI, thermospray ionization (TSP). With most ionisation methods there is the possibility of creating both positively and negatively charged sample ions, depending on the proton affinity of the sample. Before embarking on an analysis, the user must decide whether to detect the positively or negatively charged ions (Ashcroft, 2011). Prior to the 1980s, EI was the primary ionization source for mass analysis. However, EI limited chemists and biochemists to small molecules well below the mass range of common bio-organic compounds. These techniques have revolutionized biomolecular analyses, especially for large molecules. Among them, ESI and MALDI have clearly evolved to be the methods of choice when it comes to biomolecular analysis. ESI and MALDI are now the most common ionization sources for biomolecular

Fig. 4. A glance at the typical sensitivity and mass ranges allowed by different ionization techniques provides a clear answer to the question of which are most useful; EI, APCI and DIOS are somewhat limiting in terms of upper mass range, while ESI, nanoESI, and MALDI

unclear whether the highest mass ion is the molecular ion or a fragment.

mass spectrometry, offering excellent mass range and sensitivity.

have a high practical mass range (Chiu & Muddiman, 2008).

Vaccum interlock allows for the vacuum of the mass spectrometer to be maintained while the instrument is not in use. It also allows for the sample (at atomopheric pressure) to be introduced into high vacuum of the mass specterometer. The sample is then subjected to any number of desorption processes, such as laser desorption or direct heating, to facilitate vaporization and ionization.

2) Direct infusion: A simple capillary or a capillary column is used to introduce a sample as a gas or in solution. Direct infusion is also useful because it can efficiently introduce small quantities of sample into a mass spectrometer without compromising the vacuum. Capillary columns are routinely used to interface separation techniques with the ionization source of mass spectrometry. These techniques, including gas chromatography (GC) and liquid chromatography (LC), also serve to separate a solution's different components prior to mass analysis. In GC, separation of different components occurs within a glass capillary column. As the vaporized sample exits the GC, it is directly introduced into the MS.

In the 1980s the incapability of LC with MS was due largely to the ionization techniques being unable to handle the continuous flow of LC. However, ESI, APCI and atmospheric pressure photoionization (APPI) now allows LC/MS to be performed routinely. LC-MS ion chromatogram and the corresponding electrospray mass spectrum are typical technique. GC-MS produces results in much the same way as LC-MS, however, GC-MS uses an electron ionization source, which is limited by thermal vaporization (UV refers to ultraviolet and TIC is the total ion current) (Chiu & Muddiman, 2008).

#### **2.2.2 Ionization method**

Ionization method refers to the mechanism of ionization while the ion source is the mechanical device that allows ionization to occur. The different ionization methods work by either ionizing a neutral molecule through electron ejection, electron capture, protonation, cationization, or deprotonation, or by transferring a charged molecule from a condensed phase to the gas phase (Watson & Sparkman, 2007).

Protonation is a method of ionization by which a proton is added to a molecule, producing a net positive charge of 1+ for every proton added. Positive charges tend to reside on the more basic residues of the molecule, such as amines, to form stable cations. Peptides are often ionized via protonation. Pronation can be achieved via MALDI, ESI, and APCI.

Deprotonation is an ionization method by which the net negative charge of 1- is achieved through the removal of a proton from a molecule. This mechanism of ion-ization, commonly achieved via MALDI, ESI, and APCI is very useful for acidic species including phenols, carboxylic acids, and sulfonic acids.

Cationization is a method of ionization that produces a charged complex by non-covalently adding a positively charged ion to a neutral molecule. While protonation could fall under this same definition, cationization is distinct for its addition of a cation adduct other than a proton (e.g. alkali, ammonium). Moreover, it is known to be useful with molecules unstable to protonation. The binding of cations other than protons to a molecule is naturally less covalent, therefore, the charge remains localized on the cation. This minimizes delocalization of the charge and fragmentation of the molecule. Cationization is commonly achieved via MALDI, ESI, and APCI. Carbohydrates are excellent candidates for this ionization mechanism, with Na+ a common cation adduct.

The transfer of compounds already charged(=precharged) in solution is normally achieved through the desorption or ejection of the positive or negative charged species from the condensed phase into the gas phase. This transfer is commonly achieved via ESI, APCI, FAB and MALDI.

Electron ejection achieves ionization through the ejection of an electron to produce a 1+ net positive charge, often forming radical cations. Observed most commonly with electron ionization (EI) sources, electron ejection is usually performed on relatively nonpolar compounds with low molecular weights and it is also known to generate significant fragment ions. It can provide observation of EI and can provide molecular mass as well as fragmentation information. However, it often generate too much fragmentation and can be unclear whether the highest mass ion is the molecular ion or a fragment.

With the electron capture ionization method, a net negative charge of -1 is achieved with the absorption or capture of an electron. It is a mechanism of ionization primarily observed for molecules with a high electron affinity, such as halogenated compounds. It can provide observation of electron ionization and can provide molecular mass as well as fragmentation information. However, it often generate too much fragmentation and can be unclear whether the highest mass ion is the molecular ion or a fragment (Chiu & Muddiman, 2008).

#### **2.2.3 Ionization sources**

446 Tandem Mass Spectrometry – Applications and Principles

Vaccum interlock allows for the vacuum of the mass spectrometer to be maintained while the instrument is not in use. It also allows for the sample (at atomopheric pressure) to be introduced into high vacuum of the mass specterometer. The sample is then subjected to any number of desorption processes, such as laser desorption or direct heating, to facilitate

2) Direct infusion: A simple capillary or a capillary column is used to introduce a sample as a gas or in solution. Direct infusion is also useful because it can efficiently introduce small quantities of sample into a mass spectrometer without compromising the vacuum. Capillary columns are routinely used to interface separation techniques with the ionization source of mass spectrometry. These techniques, including gas chromatography (GC) and liquid chromatography (LC), also serve to separate a solution's different components prior to mass analysis. In GC, separation of different components occurs within a glass capillary column.

In the 1980s the incapability of LC with MS was due largely to the ionization techniques being unable to handle the continuous flow of LC. However, ESI, APCI and atmospheric pressure photoionization (APPI) now allows LC/MS to be performed routinely. LC-MS ion chromatogram and the corresponding electrospray mass spectrum are typical technique. GC-MS produces results in much the same way as LC-MS, however, GC-MS uses an electron ionization source, which is limited by thermal vaporization (UV refers to ultraviolet

Ionization method refers to the mechanism of ionization while the ion source is the mechanical device that allows ionization to occur. The different ionization methods work by either ionizing a neutral molecule through electron ejection, electron capture, protonation, cationization, or deprotonation, or by transferring a charged molecule from a condensed

Protonation is a method of ionization by which a proton is added to a molecule, producing a net positive charge of 1+ for every proton added. Positive charges tend to reside on the more basic residues of the molecule, such as amines, to form stable cations. Peptides are often

Deprotonation is an ionization method by which the net negative charge of 1- is achieved through the removal of a proton from a molecule. This mechanism of ion-ization, commonly achieved via MALDI, ESI, and APCI is very useful for acidic species including phenols,

Cationization is a method of ionization that produces a charged complex by non-covalently adding a positively charged ion to a neutral molecule. While protonation could fall under this same definition, cationization is distinct for its addition of a cation adduct other than a proton (e.g. alkali, ammonium). Moreover, it is known to be useful with molecules unstable to protonation. The binding of cations other than protons to a molecule is naturally less covalent, therefore, the charge remains localized on the cation. This minimizes delocalization of the charge and fragmentation of the molecule. Cationization is commonly achieved via MALDI, ESI, and APCI. Carbohydrates are excellent candidates for this

The transfer of compounds already charged(=precharged) in solution is normally achieved through the desorption or ejection of the positive or negative charged species from the

ionized via protonation. Pronation can be achieved via MALDI, ESI, and APCI.

As the vaporized sample exits the GC, it is directly introduced into the MS.

and TIC is the total ion current) (Chiu & Muddiman, 2008).

phase to the gas phase (Watson & Sparkman, 2007).

ionization mechanism, with Na+ a common cation adduct.

carboxylic acids, and sulfonic acids.

vaporization and ionization.

**2.2.2 Ionization method**

The ion source is the part of the mass spectrometer that ionizes the material under analysis (the analyte). Ionization methods include the following; APCI, CI, EI, ESI, fast atom/ion bombardment (FAB), field desorption/field ionization (FD/FI), MALDI, thermospray ionization (TSP). With most ionisation methods there is the possibility of creating both positively and negatively charged sample ions, depending on the proton affinity of the sample. Before embarking on an analysis, the user must decide whether to detect the positively or negatively charged ions (Ashcroft, 2011). Prior to the 1980s, EI was the primary ionization source for mass analysis. However, EI limited chemists and biochemists to small molecules well below the mass range of common bio-organic compounds. These techniques have revolutionized biomolecular analyses, especially for large molecules. Among them, ESI and MALDI have clearly evolved to be the methods of choice when it comes to biomolecular analysis. ESI and MALDI are now the most common ionization sources for biomolecular mass spectrometry, offering excellent mass range and sensitivity.

Fig. 4. A glance at the typical sensitivity and mass ranges allowed by different ionization techniques provides a clear answer to the question of which are most useful; EI, APCI and DIOS are somewhat limiting in terms of upper mass range, while ESI, nanoESI, and MALDI have a high practical mass range (Chiu & Muddiman, 2008).

Principles and Applications of LC-MS/MS

use two or more mass analyzers for tandem MS (MS/MS).

to the same species yet are observed at different *m/z*.

& Sparkman, 2007; Chiu & Muddiman, 2008).

**<IP_ADDRESS> Sector**

Steinwedel, 1953).

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 449

the ion (*z=q/e*). This quantity, although it is informally called the *m/z* ratio, more accurately speaking represents the ratio of the mass number, *m* and the charge number, *z*. Many MS

 With the advent of ionization sources that can vaporize and ionize biomolecules, it has become necessary to improve mass analyzer performance with respect to speed, accuracy, and resolution. More specifically, quadrupoles, quadrupole ion traps, time-to-flight (TOF), time-to-flight reflection (TOFR), and ion cyclotron resonance (ICR) mass analyzers have undergone numerous modifications and improvements over the past decade in order to be interfaced with MALDI and ESI. In the most general terms, a mass analyzer measures gas phase ions with respect to their *m/z*, where the charge is produced by the addition or loss of a proton(s), cation(s), anion(s) or electron(s). The addition of charge allows the molecule to be affected by electric fields thus allowing its mass measurement. This is important aspect to remember about mass analyzers that they measure the *m/z* ratio, not the mass itself. Multiple charging is especially common with ESI, yielding numerous peaks that correspond

 The performance of a mass analyzers can be typically be defined by the following characteristics such as accuracy, resolution, mass range, tandem analysis capabilities, and scan speed. Accuracy is the ability with which the analyzer can be accurately provide *m/z* information and is largely a function of an instrument's stability and resolution. For example, an instrument with 0.01% accuracy can provide information on a 1000 Da peptide to±0.1 Da or a 10,000 Da protein±1.0 Da. (1) The accuracy varies dramatically from analyzer to analyzer depending on the analyzer type and resolution. (2) Resolution so called resolving power is the ability of a mass spectrometer to distinguish between ions of different *m/z* ratios. Therefore, greater resolution corresponds directly to the increased ability to differentiate ions. (3) The mass range is the *m/z* range of the mass analyzer. For instance, quadrupole analyzers typically scan up to *m/z* 3000. A magnetic sector analyzer typically scans up to *m/z* 10,000 and TOF analyzers have virtually unlimited *m/z* range. (4) Tandem MS analysis is the ability of the analyzer to separate different molecular ions, generate fragment ions from a selected ion, and then mass measure the fragmented ions. The fragmented ions are used to for structural determination of original molecular ions. Typically, MS/MS experiments are performed by collision of a selected ion with inert gas molecules such as argon or helium, and the resulting fragments are mass analyzed. MS/MS analysis is used to sequence peptides, and structurally characterize carbohydrates, small oligonucleotides, and lipids. Tandem mass analysis in space is performed by consecutive analyzers whereas tandem mass in time is performed with the same analyzer, which isolates the ion of interest, fragments it, and analyzes the fragment ions. (5) Scan speed refers to the rate at which the analyzer scans over a particular mass range. Most instruments require performing a full scan; however this can vary widely depending on the analyzer. TOF analyzers, for example, complete analyses within milliseconds or less (Watson

A **sector field mass analyzer** uses an electric and/or magnetic field to affect the path and/or velocity of the charged particles in some way. The sector instruments bend the trajectories of the ions as they pass through the mass analyzer, according to their *m/z* ratios, deflecting the more charged and faster-moving, lighter ions more. The analyzer can be used to select a narrow range of *m/z* or to scan through a range of *m/z* to catalog the ions present (Paul &

Ion loses between major components of a mass spectrometer are inevitable and occur between the source and the analyzer, within the analyzer, and between the analyzer and the detector. Atmospheric pressure ion sources, such as encountered with ESI, APCI, APPI, etc., present a particular challenge with respect to efficient transfer of ions from the ion source into the *m/z* analyzer. Techniques for ionization have been key to determining what types of samples can be analyzed by MS. EI and chemical ionization(CI) are used for gases and vapors. Two techniques often used with liquid and solid biological samples include ESI and MALDI and these techniques have clearly evolved to be the methods of choice when it comes to biomolecular analysis. The idea of ESI, while not new, has been rejuvenated with its recent application to biomolecules.

Table X. Summary of event according to ionization sources (Chiu & Muddiman, 2008).

Inductively coupled plasma (ICP) sources are used primarily for cation analysis of a wide array of sample types. In the ion source technology, a 'flame' of plasma that is electrically neutral overall, but that has had a substantial fraction of its atoms ionized by high temperature, is used to atomize introduced sample molecules and to further strip the outer electrons from those atoms. The plasma is usually generated from argon gas, since the first ionization energy of argon atoms is higher than the first of any other elements except He, O, F and Ne, but lower than the second ionization energy of all except the most electropositive metals. The heating is achieved by a radio-frequency current passed through a coil surrounding the plasma. Others include glow discharge, field desorption (FD), FAB, thermospray, DIOS, Direct Analysis in Real Time (DART), APCI, secondary ion mass spectrometry (SIMS), spark ionization and thermal ionization (TIMS) (Bruins, 1991). Ion attachment ionization is a newer soft ionization technique that allows for fragmentation free analysis (Wikipedia, 2011).

#### **2.2.4 Mass analyzers**

The *m/z* analyzer (mass analyzer) is used to separate the ions according to their *m/z* ratio based on their characteristic behavior in electric and/or magnetic fields (Jennings & Dolnikowski, 1990; Farmer & McDowell, 1963). MS takes advantages of these different behaviors to separate the ions of different *m/z* values in space or time so that their abundances can be determined. Together with the particle's initial conditions, it completely determines the particle's motion in space and time in terms of *m/q*. When presenting data, it is common to use the dimensionless *m/z*, where *z* is the number of elementary charges (*e*) on the ion (*z=q/e*). This quantity, although it is informally called the *m/z* ratio, more accurately speaking represents the ratio of the mass number, *m* and the charge number, *z*. Many MS use two or more mass analyzers for tandem MS (MS/MS).

 With the advent of ionization sources that can vaporize and ionize biomolecules, it has become necessary to improve mass analyzer performance with respect to speed, accuracy, and resolution. More specifically, quadrupoles, quadrupole ion traps, time-to-flight (TOF), time-to-flight reflection (TOFR), and ion cyclotron resonance (ICR) mass analyzers have undergone numerous modifications and improvements over the past decade in order to be interfaced with MALDI and ESI. In the most general terms, a mass analyzer measures gas phase ions with respect to their *m/z*, where the charge is produced by the addition or loss of a proton(s), cation(s), anion(s) or electron(s). The addition of charge allows the molecule to be affected by electric fields thus allowing its mass measurement. This is important aspect to remember about mass analyzers that they measure the *m/z* ratio, not the mass itself. Multiple charging is especially common with ESI, yielding numerous peaks that correspond to the same species yet are observed at different *m/z*.

 The performance of a mass analyzers can be typically be defined by the following characteristics such as accuracy, resolution, mass range, tandem analysis capabilities, and scan speed. Accuracy is the ability with which the analyzer can be accurately provide *m/z* information and is largely a function of an instrument's stability and resolution. For example, an instrument with 0.01% accuracy can provide information on a 1000 Da peptide to±0.1 Da or a 10,000 Da protein±1.0 Da. (1) The accuracy varies dramatically from analyzer to analyzer depending on the analyzer type and resolution. (2) Resolution so called resolving power is the ability of a mass spectrometer to distinguish between ions of different *m/z* ratios. Therefore, greater resolution corresponds directly to the increased ability to differentiate ions. (3) The mass range is the *m/z* range of the mass analyzer. For instance, quadrupole analyzers typically scan up to *m/z* 3000. A magnetic sector analyzer typically scans up to *m/z* 10,000 and TOF analyzers have virtually unlimited *m/z* range. (4) Tandem MS analysis is the ability of the analyzer to separate different molecular ions, generate fragment ions from a selected ion, and then mass measure the fragmented ions. The fragmented ions are used to for structural determination of original molecular ions. Typically, MS/MS experiments are performed by collision of a selected ion with inert gas molecules such as argon or helium, and the resulting fragments are mass analyzed. MS/MS analysis is used to sequence peptides, and structurally characterize carbohydrates, small oligonucleotides, and lipids. Tandem mass analysis in space is performed by consecutive analyzers whereas tandem mass in time is performed with the same analyzer, which isolates the ion of interest, fragments it, and analyzes the fragment ions. (5) Scan speed refers to the rate at which the analyzer scans over a particular mass range. Most instruments require performing a full scan; however this can vary widely depending on the analyzer. TOF analyzers, for example, complete analyses within milliseconds or less (Watson & Sparkman, 2007; Chiu & Muddiman, 2008).

#### **<IP_ADDRESS> Sector**

448 Tandem Mass Spectrometry – Applications and Principles

Ion loses between major components of a mass spectrometer are inevitable and occur between the source and the analyzer, within the analyzer, and between the analyzer and the detector. Atmospheric pressure ion sources, such as encountered with ESI, APCI, APPI, etc., present a particular challenge with respect to efficient transfer of ions from the ion source into the *m/z* analyzer. Techniques for ionization have been key to determining what types of samples can be analyzed by MS. EI and chemical ionization(CI) are used for gases and vapors. Two techniques often used with liquid and solid biological samples include ESI and MALDI and these techniques have clearly evolved to be the methods of choice when it comes to biomolecular analysis. The idea of ESI, while not new, has been rejuvenated with

**Ionization Source Event**

Desorption/ionization on silicon(DIOS) Photon absorption/proton transfer Fast atom/ion bormbardment(FAB) Ion desorption/proton transfer Electron ionization(EI) Electron beam/electron transfer

Chemical Ionization(CI) Proton transfer

Inductively coupled plasma (ICP) sources are used primarily for cation analysis of a wide array of sample types. In the ion source technology, a 'flame' of plasma that is electrically neutral overall, but that has had a substantial fraction of its atoms ionized by high temperature, is used to atomize introduced sample molecules and to further strip the outer electrons from those atoms. The plasma is usually generated from argon gas, since the first ionization energy of argon atoms is higher than the first of any other elements except He, O, F and Ne, but lower than the second ionization energy of all except the most electropositive metals. The heating is achieved by a radio-frequency current passed through a coil surrounding the plasma. Others include glow discharge, field desorption (FD), FAB, thermospray, DIOS, Direct Analysis in Real Time (DART), APCI, secondary ion mass spectrometry (SIMS), spark ionization and thermal ionization (TIMS) (Bruins, 1991). Ion attachment ionization is a newer soft ionization technique that allows for fragmentation free

The *m/z* analyzer (mass analyzer) is used to separate the ions according to their *m/z* ratio based on their characteristic behavior in electric and/or magnetic fields (Jennings & Dolnikowski, 1990; Farmer & McDowell, 1963). MS takes advantages of these different behaviors to separate the ions of different *m/z* values in space or time so that their abundances can be determined. Together with the particle's initial conditions, it completely determines the particle's motion in space and time in terms of *m/q*. When presenting data, it is common to use the dimensionless *m/z*, where *z* is the number of elementary charges (*e*) on

Table X. Summary of event according to ionization sources (Chiu & Muddiman, 2008).

Electrosray ionization(ESI) Evaporation of charged droplets Nanoelectrospray ionization(nanoESI) Evaporation of charged droplets

(APCI) Corona discharge and proton transfer

(MALDI) Photon absorption/proton transfer

its recent application to biomolecules.

analysis (Wikipedia, 2011).

**2.2.4 Mass analyzers**

Atmospheric pressure chemical ionization

matrix-assisted laser desorption ionization

A **sector field mass analyzer** uses an electric and/or magnetic field to affect the path and/or velocity of the charged particles in some way. The sector instruments bend the trajectories of the ions as they pass through the mass analyzer, according to their *m/z* ratios, deflecting the more charged and faster-moving, lighter ions more. The analyzer can be used to select a narrow range of *m/z* or to scan through a range of *m/z* to catalog the ions present (Paul & Steinwedel, 1953).

Principles and Applications of LC-MS/MS

spectrometer (Watson & Sparkman, 2007). **<IP_ADDRESS> Linear quadrupole ion trap (LIT)**

(Chiu & Muddiman, 2008).

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 451

and, more popular method involving in generation of ions externally with ESI or MALDI and using ion optics for sample injection into the trapping volume. The QIT typically consists of a ring electrode and two hyperbolic endcap electrodes. The isolated ions can subsequently be fragmented by collisional activation and the fragments detected. The primary advantage of QIT is that multiple collision induced dissociation experiments can be performed quickly without having multiple analyzers, such that real time LC-MS/MS is now routine. Other important advantages of QIT include their compact size, and thier ability to trap and accumulate ions to provide a better ion signal. QIT have been utilized in a number of applications ranging from electrospray ionization MS of biomolecules to their recent interface with MALDI. LC-MS/MS experiments are performed on proteolytic digests which provide both MS and MS/MS information. This information allows for protein identification and post-translational modification characterization. The mass range (~ *m/z* 4000) of commercial LC-traps is well matched to *m/z* values generated from the ESI of peptides and the resolution allows for charge state identification of multiplecharged peptide ions. QIT-MS can analyze peptides from a tryptic digest present at the 20~100 fmol level. Another asset of the ion trap technique for peptide analysis is the ability to perform multiple stages of MS, which can significantly increase the amount of structural information. The cylindrical ion trap MS is a derivative of the QIT mass

The linear ion trap (LIT), sometimes referred to as the 2-dimensional quadrupole ion trap (2D QIT), is one of the more recent additions to the single *m/z* analyzer group (Douglas et al, 2005; Hager, 2002). The LIT makes use of the basic structure of a transmission quadrupole; i.e., an array of four electrical surfaces; however, instead of being used to filter ions of all *m/z* values except for those of a desired value from an unresolved ion beam, they are used for trapping, manipulation of ion trajectories, and *m/z*-selective ion ejection (Londry & Hager, 2003). A LIT is similar to a QIT, but it traps ions in a 2D quadrupole field, instead of a 3-dimensional (3D) quadrupole field as in a 3D QIT. The LIT differs from the 3D ion trap as it confines ions along the axis of a quadrupole mass analyzer using a 2D radio frequency (RF) field with potentials applied to end electrodes. The primary advantage to the linear trap over the 3D trap is the larger analyzer volume lends itself to a greater dynamic ranges and an improved range of quantitative analysis (Chiu & Muddiman, 2008). This toroidal shaped trap is a configuration that allows the increased miniaturization of an ion trap mass analyzer. The LIT has higher injection efficiencies and storage capacities than conventional 3D QIT (or Paul trap). 2D multipole fields are well known for their capacity to trap and manipulate ions (Gerlich, 1992). Given the power of the ion trap the major limitations of this device that keep it from being the ultimate tool for pharmacokinetics and proteomics include the following: (1) the ability to perform high sensitivity triple quadrupole-type precursor ion scanning and neutral loss scanning experiments is not possible with ion traps. (2) The upper limit on the ratio between precursor *m/z* and the lowest trapped fragment ion is ~0.3 (also known as the "one third rules"). (3) The dynamic range of ion traps is limited because when too many ions are in the trap, space charge effects diminish the performance of the ion trap analyzer. To get around this, automated scans can rapidly count ions before they go into the trap, therefore limiting the number of ions getting in. Yet this approach presents a problem when an ion of interest is accompanied by a large background ion population

#### **<IP_ADDRESS> Time-of-flight (TOF)**

The operating principles of the TOF-MS involve measuring the time required for an ion to travel from ion source to a detector usually located 1 to 2 meter from the source (Graff, 1995; Guilaus, 1995). The TOF analyzer uses an electric field to accelerate the ions through the same potential, and then measures the time they take to reach the detector. If the particles all have the same charge, the kinetic energies will be identical, and their velocities will depend only on their masses. As the ions traverse the "field-free" region between the ion source and detector, they separate into groups or packets according to velocity, which is a function of their *m/z* values, i.e. lighter ions will reach the detector first (March, 2000). As will be seen, all other types of *m/z* analyzers have upper limits for *m/z* values that can be transmitted and separated based on the way the electric and/or magnetic fields are used to separate ions of different *m/z* ratios.

#### **<IP_ADDRESS> Quadrupole**

Quadrupole mass analyzers use oscillating electrical fields to selectively stabilize or destabilize the paths of ions passing through a radio frequency (RF) quadrupole field. Only a single *m/z* ratio is passed through the system at any time, but changes to the potentials on magnetic lenses allows a wide range of *m/z* values to be swept rapidly, either continuously or in a succession of discrete hops. A quadrupole mass spectrometer acts as a mass-selective filter and is closely related to the quadrupole ion trap, particularly the linear quadrupole ion trap except that it is designed to pass the untrapped ions rather than collect the trapped ones, and is for that reason referred to as a transmission quadrupole. A common variation of the quadrupole is the triple quadrupole. Quadrupoles offer three main advantages such as tolerance to relatively high pressures, significant mass range with the capability of analyzing up to an *m/z* 4000, which is useful because ESI of proteins and other biomolecules commonly produce charge distributions from *m/z* 1000 to 3500 and relatively low cost instruments. In order to perform tandem MS analysis with a quadrupole instrument, it is necessary to place three quadrupoles in series. Each quadrupole has a separate function; the first (Q1) is used to scan across a preset *m/z* range and select an ion of interest. The second (Q2), also known as the collison cell, focuses and transmits the ions while introducing a collison gas (argon or helium) into the flight path of the selected ion. The third (Q3) serves to analyze the fragment ions generated in the collison cell (Q2) (Watson & Sparkman, 2007).

#### **<IP_ADDRESS> Quadrupole ion trap (QIT)**

The name quadrupole is derived the fact that an electric field is created between four opposing electrical poles (Watson & Sparkman, 2007). The QIT works on the same physical principles as the quadrupole mass analyzer, but the ions are trapped and sequentially ejected. Ions are created and trapped in a mainly quadrupole RF potential and separated by *m/q*, non-destructively or destructively. There are many *m/z* separation and isolation methods but most commonly used is the mass instability mode in which the RF potential is ramped so that the orbit of ions with a mass *a > b* are stable while ions with mass *b* become unstable and are ejected on the *z*-axis onto a detector. Ions may also be ejected by the resonance excitation method, whereby a supplemental oscillatory excitation voltage is applied to the endcap electrodes and the trapping voltage amplitude and/or excitation voltage frequency is varied to bring ions into a resonance condition in order of their *m/z* ratio (Schwartz et al., 2002; Lammert et al., 2006). Two method of using an ion trap for MS are involved to generate ions internally with EI, followed by mass analysis

The operating principles of the TOF-MS involve measuring the time required for an ion to travel from ion source to a detector usually located 1 to 2 meter from the source (Graff, 1995; Guilaus, 1995). The TOF analyzer uses an electric field to accelerate the ions through the same potential, and then measures the time they take to reach the detector. If the particles all have the same charge, the kinetic energies will be identical, and their velocities will depend only on their masses. As the ions traverse the "field-free" region between the ion source and detector, they separate into groups or packets according to velocity, which is a function of their *m/z* values, i.e. lighter ions will reach the detector first (March, 2000). As will be seen, all other types of *m/z* analyzers have upper limits for *m/z* values that can be transmitted and separated based on the way the electric and/or magnetic fields are used to separate ions of

Quadrupole mass analyzers use oscillating electrical fields to selectively stabilize or destabilize the paths of ions passing through a radio frequency (RF) quadrupole field. Only a single *m/z* ratio is passed through the system at any time, but changes to the potentials on magnetic lenses allows a wide range of *m/z* values to be swept rapidly, either continuously or in a succession of discrete hops. A quadrupole mass spectrometer acts as a mass-selective filter and is closely related to the quadrupole ion trap, particularly the linear quadrupole ion trap except that it is designed to pass the untrapped ions rather than collect the trapped ones, and is for that reason referred to as a transmission quadrupole. A common variation of the quadrupole is the triple quadrupole. Quadrupoles offer three main advantages such as tolerance to relatively high pressures, significant mass range with the capability of analyzing up to an *m/z* 4000, which is useful because ESI of proteins and other biomolecules commonly produce charge distributions from *m/z* 1000 to 3500 and relatively low cost instruments. In order to perform tandem MS analysis with a quadrupole instrument, it is necessary to place three quadrupoles in series. Each quadrupole has a separate function; the first (Q1) is used to scan across a preset *m/z* range and select an ion of interest. The second (Q2), also known as the collison cell, focuses and transmits the ions while introducing a collison gas (argon or helium) into the flight path of the selected ion. The third (Q3) serves to analyze the fragment

The name quadrupole is derived the fact that an electric field is created between four opposing electrical poles (Watson & Sparkman, 2007). The QIT works on the same physical principles as the quadrupole mass analyzer, but the ions are trapped and sequentially ejected. Ions are created and trapped in a mainly quadrupole RF potential and separated by *m/q*, non-destructively or destructively. There are many *m/z* separation and isolation methods but most commonly used is the mass instability mode in which the RF potential is ramped so that the orbit of ions with a mass *a > b* are stable while ions with mass *b* become unstable and are ejected on the *z*-axis onto a detector. Ions may also be ejected by the resonance excitation method, whereby a supplemental oscillatory excitation voltage is applied to the endcap electrodes and the trapping voltage amplitude and/or excitation voltage frequency is varied to bring ions into a resonance condition in order of their *m/z* ratio (Schwartz et al., 2002; Lammert et al., 2006). Two method of using an ion trap for MS are involved to generate ions internally with EI, followed by mass analysis

ions generated in the collison cell (Q2) (Watson & Sparkman, 2007).

**<IP_ADDRESS> Quadrupole ion trap (QIT)**

**<IP_ADDRESS> Time-of-flight (TOF)**

different *m/z* ratios. **<IP_ADDRESS> Quadrupole**  and, more popular method involving in generation of ions externally with ESI or MALDI and using ion optics for sample injection into the trapping volume. The QIT typically consists of a ring electrode and two hyperbolic endcap electrodes. The isolated ions can subsequently be fragmented by collisional activation and the fragments detected. The primary advantage of QIT is that multiple collision induced dissociation experiments can be performed quickly without having multiple analyzers, such that real time LC-MS/MS is now routine. Other important advantages of QIT include their compact size, and thier ability to trap and accumulate ions to provide a better ion signal. QIT have been utilized in a number of applications ranging from electrospray ionization MS of biomolecules to their recent interface with MALDI. LC-MS/MS experiments are performed on proteolytic digests which provide both MS and MS/MS information. This information allows for protein identification and post-translational modification characterization. The mass range (~ *m/z* 4000) of commercial LC-traps is well matched to *m/z* values generated from the ESI of peptides and the resolution allows for charge state identification of multiplecharged peptide ions. QIT-MS can analyze peptides from a tryptic digest present at the 20~100 fmol level. Another asset of the ion trap technique for peptide analysis is the ability to perform multiple stages of MS, which can significantly increase the amount of structural information. The cylindrical ion trap MS is a derivative of the QIT mass spectrometer (Watson & Sparkman, 2007).

#### **<IP_ADDRESS> Linear quadrupole ion trap (LIT)**

The linear ion trap (LIT), sometimes referred to as the 2-dimensional quadrupole ion trap (2D QIT), is one of the more recent additions to the single *m/z* analyzer group (Douglas et al, 2005; Hager, 2002). The LIT makes use of the basic structure of a transmission quadrupole; i.e., an array of four electrical surfaces; however, instead of being used to filter ions of all *m/z* values except for those of a desired value from an unresolved ion beam, they are used for trapping, manipulation of ion trajectories, and *m/z*-selective ion ejection (Londry & Hager, 2003). A LIT is similar to a QIT, but it traps ions in a 2D quadrupole field, instead of a 3-dimensional (3D) quadrupole field as in a 3D QIT. The LIT differs from the 3D ion trap as it confines ions along the axis of a quadrupole mass analyzer using a 2D radio frequency (RF) field with potentials applied to end electrodes. The primary advantage to the linear trap over the 3D trap is the larger analyzer volume lends itself to a greater dynamic ranges and an improved range of quantitative analysis (Chiu & Muddiman, 2008). This toroidal shaped trap is a configuration that allows the increased miniaturization of an ion trap mass analyzer. The LIT has higher injection efficiencies and storage capacities than conventional 3D QIT (or Paul trap). 2D multipole fields are well known for their capacity to trap and manipulate ions (Gerlich, 1992). Given the power of the ion trap the major limitations of this device that keep it from being the ultimate tool for pharmacokinetics and proteomics include the following: (1) the ability to perform high sensitivity triple quadrupole-type precursor ion scanning and neutral loss scanning experiments is not possible with ion traps. (2) The upper limit on the ratio between precursor *m/z* and the lowest trapped fragment ion is ~0.3 (also known as the "one third rules"). (3) The dynamic range of ion traps is limited because when too many ions are in the trap, space charge effects diminish the performance of the ion trap analyzer. To get around this, automated scans can rapidly count ions before they go into the trap, therefore limiting the number of ions getting in. Yet this approach presents a problem when an ion of interest is accompanied by a large background ion population (Chiu & Muddiman, 2008).

Principles and Applications of LC-MS/MS

multiplier.

Sparkman , 2007). **<IP_ADDRESS> Faraday cup**

**<IP_ADDRESS> Electron Multiplier (EM)**

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 453

weak AC image current is produced in a circuit between the electrodes. Other inductive detectors have also been used (Park et al., 1994). Sensitivity, accuracy, and response time are importantparameters that distinguish different ion detection system (Koppenaal et al., 2005). High accuracy and fast-response times usually are mutually exclusive features, therefore, the fast-response electron multiplier required to follow rapid scans (e.g. *m/z* 50 to 500 in 0.1 sec) probably will not provide the accuracy desired (better than ±0.1 %) in isotope ratio measurements. Such isotope ratio measurements are usually made with the Faraday cup detector (Nygren et al., 2006; Harris et al., 1984; Mckinney et al., 1950). Ideally, a statement of sensitivity should explicity define the ion current received by detector for a specified rate of sample consumption. The definition should include (1) the name of the calibration compound, (2) the *m/z* value of the ion current that is measured, (3) the resolving power of the instrument, (4) the quantity of calibration compound consumed per second, (5) the intensity of the electron beam and pressure in the ion source for CI, and (6) the ion current arriving at the detector (e.g., that impinging the conversion dynode of an electron

The EM uses the principle of secondary-electron emission to effect amplification (Harris et al., 1984). Perhaps the most common means of detecting ions involves an EM, which is made up of a series (12 to 24) of aluminum oxide (Al2O3) dynodes maintained at ever increasing potentials. Ions strike the first dynode surface causing an emission of electrons. These electrons are then attracted to the next dynode held at a higher potential and therefore more secondary electrons are generated. Ultimately, as numerous dynodes are involved, a cascade of electrons is formed that results in an overall current gain on the order of one million or higher. The high energy dynode (HED) uses an accelerating electrostatic field to increase the velocity of the ions. In the discrete-dynode version of an EM, The ion beam from the *m/z* analyzer is focused onto the conversion dynode, which emits electrons in direct proportion to the number of bombarding ions. The secondary electrons from the conversion dynode (ions to electrons) are accelerated and focused onto a second dynode, which itself emits secondary electrons (electrons to electrons). This means, amplification is accomplished through a ''cascading effect" of secondary electrons from dynode to dynode, because the number of electrons impinging on it (Fies, 1988). The efficiency of EM is dependent upon the velocity of the impinging particle (Westmacott et al., 2000), a feature responsible for the disappointing performance of channel EM arrays in MALDI-TOF/MS for high-mass ions (Chen et al., 2003). The secondary electrons are attracted along the positive electrical gradient farther on into the cornucopia. Each time these electrons collide with the wall, additional secondary electrons are expelled, thereby providing amplification. This form of the continuous dynode is curved so as to prevent positive ions from causing spurious signals or feedback signals due to seconadry ionization of residue gas molecule (Watson &

In this conventional electrical detector, positive ions impinging on the collector are neutralized by electrons dawn from groud after passage through a high-ohmic resistor. A Faraday cup involves an ion striking the dynode (BeO, GaP, or CsSb) surface which causes secondary electrons to be ejected. This temporary electron emission induces a positive charge on the detector and therefore a current of electrons flowing toward the detector. This

#### **<IP_ADDRESS> Orbitrap**

The orbitrap mass spectrometer is the latest development in trapping devices used as an *m/z* analyzer. The orbitrap ia a new mass analyzer (Hardman & Makarov, 2003; Hu et al., 2005; Makarov et al., 2006); however, it is useful to consider the orbitrap as a modified Knightstyle Kingdon trap with specially shaped inner spindle-like (axial) electrode and a outer barrel-like (coaxial) electrodes that form an electrostatic field with quadro-logarithmic potential distribution (Makarov, 2000; Makarov et al., 2006a; Hu et al., 2005). The frequency of these harmonic oscillations is independent of the ion velocity and is inversely proportional to the square root of the mass-to-charge ratio (*m/z* or *m/q*). By sensing the ion oscillation in a manner similar to that used in Fourier transform ion cyclotron resonance (FTICR)-MS, the trap can be used as a mass analyzer. Orbitraps have a high mass accuracy (1–2 ppm), a high resolving power (up to 200,000) and a high dynamic range (around 5000) (Makarov et al, 2006a; Makarov et al., 2006b). Very similar nonmagnetic FTMS has been performed, where ions are electrostatically trapped in an orbit around a central, spindle shaped electrode. Mass spectra are obtained by Fourier transformation of the recorded image currents. Similar to Fourier transform ion cyclotron resonance mass spectrometers, Orbitraps have a high mass accuracy, and high sensitivity and a good dynamic range (Hu et al., 2005).

#### **<IP_ADDRESS> Fourier transform ion cyclotron resonance**

Fourier transform mass spectrometry (FT-MS), or more precisely Fourier transform ion cyclotron resonance MS, measures mass by detecting the image current produced by ions cyclotroning in the presence of a magnetic field. Instead of measuring the deflection of ions with a detector such as an electron multiplier, the ions are injected into a Penning trap (a static electric/magnetic ion trap) where they effectively form part of a circuit. Since the frequency of an ion's cycling is determined by its *m/z* ratio, this can be deconvoluted by performing a Fourier transform on the signal. FTMS has the advantage of high sensitivity (since each ion is "counted" more than once) and much higher resolution and thus precision (Comisarow & Marshall, 1974; Marshall et al., 1998). Ion cyclotron resonance (ICR) is an older mass analysis technique similar to FT-MS except that ions are detected with a traditional detector. Ions trapped in a Penning trap are excited by an RF electric field until they impact the wall of the trap, where the detector is located. Ions of different mass are resolved according to impact time.

#### **2.2.5 Detectors**

The final element of the mass spectrometer is the detector that records either the charge induced or the current produced when an ion passes by or hits a surface. In a scanning instrument, the signal produced in the detector during the course of the scan versus where the instrument is in the scan (at what *m/q*) will produce a mass spectrum, a record of ions as a function of *m/q* (Wikipedia). Typically, some type of electron multiplier is used, though other detectors including Faraday cups and ion-to-photon detectors are also used. Because the number of ions leaving the mass analyzer at a particular instant is typically quite small, considerable amplification is often necessary to get a signal. Microchannel plate detectors are commonly used in modern commercial instruments (Dubois et al., 1999). In FT-MS and Orbitraps, the detector consists of a pair of metal surfaces within the mass analyzer/ion trap region which the ions only pass near as they oscillate. No DC current is produced, only a weak AC image current is produced in a circuit between the electrodes. Other inductive detectors have also been used (Park et al., 1994). Sensitivity, accuracy, and response time are importantparameters that distinguish different ion detection system (Koppenaal et al., 2005). High accuracy and fast-response times usually are mutually exclusive features, therefore, the fast-response electron multiplier required to follow rapid scans (e.g. *m/z* 50 to 500 in 0.1 sec) probably will not provide the accuracy desired (better than ±0.1 %) in isotope ratio measurements. Such isotope ratio measurements are usually made with the Faraday cup detector (Nygren et al., 2006; Harris et al., 1984; Mckinney et al., 1950). Ideally, a statement of sensitivity should explicity define the ion current received by detector for a specified rate of sample consumption. The definition should include (1) the name of the calibration compound, (2) the *m/z* value of the ion current that is measured, (3) the resolving power of the instrument, (4) the quantity of calibration compound consumed per second, (5) the intensity of the electron beam and pressure in the ion source for CI, and (6) the ion current arriving at the detector (e.g., that impinging the conversion dynode of an electron multiplier.

#### **<IP_ADDRESS> Electron Multiplier (EM)**

452 Tandem Mass Spectrometry – Applications and Principles

The orbitrap mass spectrometer is the latest development in trapping devices used as an *m/z* analyzer. The orbitrap ia a new mass analyzer (Hardman & Makarov, 2003; Hu et al., 2005; Makarov et al., 2006); however, it is useful to consider the orbitrap as a modified Knightstyle Kingdon trap with specially shaped inner spindle-like (axial) electrode and a outer barrel-like (coaxial) electrodes that form an electrostatic field with quadro-logarithmic potential distribution (Makarov, 2000; Makarov et al., 2006a; Hu et al., 2005). The frequency of these harmonic oscillations is independent of the ion velocity and is inversely proportional to the square root of the mass-to-charge ratio (*m/z* or *m/q*). By sensing the ion oscillation in a manner similar to that used in Fourier transform ion cyclotron resonance (FTICR)-MS, the trap can be used as a mass analyzer. Orbitraps have a high mass accuracy (1–2 ppm), a high resolving power (up to 200,000) and a high dynamic range (around 5000) (Makarov et al, 2006a; Makarov et al., 2006b). Very similar nonmagnetic FTMS has been performed, where ions are electrostatically trapped in an orbit around a central, spindle shaped electrode. Mass spectra are obtained by Fourier transformation of the recorded image currents. Similar to Fourier transform ion cyclotron resonance mass spectrometers, Orbitraps have a high mass accuracy, and high sensitivity and a good dynamic range (Hu et

Fourier transform mass spectrometry (FT-MS), or more precisely Fourier transform ion cyclotron resonance MS, measures mass by detecting the image current produced by ions cyclotroning in the presence of a magnetic field. Instead of measuring the deflection of ions with a detector such as an electron multiplier, the ions are injected into a Penning trap (a static electric/magnetic ion trap) where they effectively form part of a circuit. Since the frequency of an ion's cycling is determined by its *m/z* ratio, this can be deconvoluted by performing a Fourier transform on the signal. FTMS has the advantage of high sensitivity (since each ion is "counted" more than once) and much higher resolution and thus precision (Comisarow & Marshall, 1974; Marshall et al., 1998). Ion cyclotron resonance (ICR) is an older mass analysis technique similar to FT-MS except that ions are detected with a traditional detector. Ions trapped in a Penning trap are excited by an RF electric field until they impact the wall of the trap, where the detector is located. Ions of different mass are

The final element of the mass spectrometer is the detector that records either the charge induced or the current produced when an ion passes by or hits a surface. In a scanning instrument, the signal produced in the detector during the course of the scan versus where the instrument is in the scan (at what *m/q*) will produce a mass spectrum, a record of ions as a function of *m/q* (Wikipedia). Typically, some type of electron multiplier is used, though other detectors including Faraday cups and ion-to-photon detectors are also used. Because the number of ions leaving the mass analyzer at a particular instant is typically quite small, considerable amplification is often necessary to get a signal. Microchannel plate detectors are commonly used in modern commercial instruments (Dubois et al., 1999). In FT-MS and Orbitraps, the detector consists of a pair of metal surfaces within the mass analyzer/ion trap region which the ions only pass near as they oscillate. No DC current is produced, only a

**<IP_ADDRESS> Orbitrap**

al., 2005).

**<IP_ADDRESS> Fourier transform ion cyclotron resonance**

resolved according to impact time.

**2.2.5 Detectors**

The EM uses the principle of secondary-electron emission to effect amplification (Harris et al., 1984). Perhaps the most common means of detecting ions involves an EM, which is made up of a series (12 to 24) of aluminum oxide (Al2O3) dynodes maintained at ever increasing potentials. Ions strike the first dynode surface causing an emission of electrons. These electrons are then attracted to the next dynode held at a higher potential and therefore more secondary electrons are generated. Ultimately, as numerous dynodes are involved, a cascade of electrons is formed that results in an overall current gain on the order of one million or higher. The high energy dynode (HED) uses an accelerating electrostatic field to increase the velocity of the ions. In the discrete-dynode version of an EM, The ion beam from the *m/z* analyzer is focused onto the conversion dynode, which emits electrons in direct proportion to the number of bombarding ions. The secondary electrons from the conversion dynode (ions to electrons) are accelerated and focused onto a second dynode, which itself emits secondary electrons (electrons to electrons). This means, amplification is accomplished through a ''cascading effect" of secondary electrons from dynode to dynode, because the number of electrons impinging on it (Fies, 1988). The efficiency of EM is dependent upon the velocity of the impinging particle (Westmacott et al., 2000), a feature responsible for the disappointing performance of channel EM arrays in MALDI-TOF/MS for high-mass ions (Chen et al., 2003). The secondary electrons are attracted along the positive electrical gradient farther on into the cornucopia. Each time these electrons collide with the wall, additional secondary electrons are expelled, thereby providing amplification. This form of the continuous dynode is curved so as to prevent positive ions from causing spurious signals or feedback signals due to seconadry ionization of residue gas molecule (Watson & Sparkman , 2007).

#### **<IP_ADDRESS> Faraday cup**

In this conventional electrical detector, positive ions impinging on the collector are neutralized by electrons dawn from groud after passage through a high-ohmic resistor. A Faraday cup involves an ion striking the dynode (BeO, GaP, or CsSb) surface which causes secondary electrons to be ejected. This temporary electron emission induces a positive charge on the detector and therefore a current of electrons flowing toward the detector. This

Principles and Applications of LC-MS/MS

the EM (Chiu & Muddiman, 2008).

metastable decay (Watson & Sparkman, 2007)

**2.2.6 Vacuum techniques and systems**

**<IP_ADDRESS> The daly detector**

**<IP_ADDRESS> Array detector**

Muddiman, 2008).

**<IP_ADDRESS> Photomultiplier conversion dynode**

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 455

The photomultiplier conversion dynode detector is not as commonly used at the EM yet it is similar in design where the secondary electrons strike a phosphorus screen instead of a dynode. The phosphorus screen releases photons which are detected by the photomultiplier. One advantage of the conversion dynode is that the photomultiplier tube is sealed in a vacuum, unexposed to the environment of the mass spectrometer and thus the possibility of contamination is removed. This improves the lifetimes of these detectors over electron multipliers. A five-year or greater lifetime is typical, and they have a similar sensitivity to

The positive ion beam passing the detector slit is attracted toward an aluminized cathode (the Daly knob) held at a very large negative potential (e.g. -15,000 V) (Daly et al, 1968a; Daly et al, 1968b). Positive ions impacting the Daly knob, which essentially serves ac a conversion dynode, produces up to eight secondary electrons, which are attracted to scintillator unit held at ground potential. The Daly detector offers two significant advantages over other similar detectors. First, most of components (all except the Daly knob) are located outside the vacuum chamber, and thus can be served without distrupting the pressure regime of the mass spectrometer. Second, the large potential difference used between the Daly knob and the slit is particularly advantageous for detecting ions of high mass as a post-accelerator detector. In addition, a deceleration lens can be installed in front of Daly knob to distinguish between stable ions and those that are ionic products of

An array detector is a group of individual detectors aligned in an array format. The array detector, which spatially detects ions according to their different *m*/*z*, has been typically used on magnetic sector mass analyzers. Spatially differentiated ions can be detected simultaneously by an array detector. The primary advantage of this approach is that, over a small mass range, scanning is not necessary and therefore sensitivity is improved ( Chiu &

All mass spectrometer need a vacuum to allow ions to reach the detector without colliding with other gaseous molecules or atoms. If some collisions between molecules did occur, the instrument would suffer from reduced resolution and sensitivity. Low pressure (i.e. infrequent ion/molecule or molecule/molecule collisions) is also essential for preservation of resolving power in *m/z* analyzers. Once the direction of an ion's path has been established, any interaction with other matter can cause that direction to change (Watson & Sparkman, 2007). One of the first obstacles faced by the originators of mass spectrometer was coupling the sample source to a mass spectrometer. The sample is initially at atmospheric pressure (760 torr) before being transferred into the mass spectrometer's vacuum (~10-6 torr), which represents approximately a billion-fold difference in pressure. One approach is to introduce the sample through a capillary column (GC) or through a small orifice directly into the instrument. Another approach is to evacuate the sample chamber through a vacuum lock (MALDI) and once a reasonable vacuum is achieved (< 10-2 torr) the sample can be presented to the primary vacuum chamber (< 10-5 torr). The

detector is not particularly sensitive, offering limited amplification of signal, yet it is tolerant of relatively high pressure (Chiu & Muddiman, 2008). Faraday cup detectors have high accuracy, constant sensitivity, and low electrical noise. The principal disadvantage of the classical Faraday is tis relatively long time constant inherent in the amplification system associated with the use of a high-ohmic resistor in the circuitry (Watson & Sparkman, 2007).

#### **<IP_ADDRESS> Negative-ion detection**

Modification of a magnetic mass spectrometer to detect negative ions instead of positive ions is relatively simple and the polarity of the accelerating voltage and the magnet current must be reversed. The negative ions have sufficient injection kinetic energy (typically 3~4 kV) to impinge on the EM even though it has a negative bias on its first dynode so that secondary electrons will experience an overall positive gradient toward the last stage(Watson & Sparkman, 2007). In mass spectrometer that uses quadrupole fields no change is required in the analyzer part of the instrument because the field acts on positive and negative ions equally. In the transmission quadrupole, the repeller and acceleration voltages have to be changed from positive to negative.

#### **<IP_ADDRESS> Post-acceleration detector**

With the advent of the desorption/inonization technique MALDI, it has been possible to generate ions of extraordinarily high *m/z* values, however, it is often difficult to detect such ions efficiently because their velocity is relatively low if it depends only on the accelerating voltage of the ion source (Beuhler et al., 1991; Matthew et al., 1986). One technique for improving the detection efficiency of high *m/z* value ions is to provide a "post-acceleration" electric field to increase their velocity prior to impacting the conversion dynode of the detector (Hedin et al., 1987). Detection of macro-ions (those heavier than hundreds of kDa having a single or double charge) has been challenge in modern MS. Conventional MS has relied on ionization-based detectors, namely those producing and multiplying secondary electrons associated with particle bombardment of a metal surface; such detectors are restricted to ions having a mass less than 106 Da. An ion-to-proton conversion detector (IPD) shows promise for detecting macro-ions (Dubois et al., 1997; Dubois et al., 1999). Photosensitive detectors, relying on laser-indued fluorescence (LIF) or elastic light scattering (ELS), show promise in this area.

#### **<IP_ADDRESS> Channel Electron Multiplier Array (CEMA)**

CEMA consists of a honeycomb arrangement of many channels up to several hundred per square inch, each having a diameter on the order of 10 m made possible with fiber optic technology using metal-doped glass. A potential difference applied to opposite ends of the channels with top and bottom of the honeycomb creates an electrical gradient along the resistive but conducting surface of each channel. The ions enter the individual channels slightly off-axis so that they impinge the wall of the channel. This primary event (an ion colliding with the surface to expel electrons) has very poor efficiency; the efficiency is directly proportional to the velocity of the impacting ion, which explains the exceptionally poor response of the CEMA to massive ions. The secondary electrons resulting from ions impinging the wall continue to ricochet down the channel, producing more secondary electrons upon each impact, thereby amplifying the original ion beam (Watson & Sparkman, 2007). The CEMA is also employed in TOF-MS because it presents a simple flat surface that can be arranged perpendicular to the ion beam to preserve velocity resolution of the ion packets (Price & Milnes, 1984).

#### **<IP_ADDRESS> Photomultiplier conversion dynode**

The photomultiplier conversion dynode detector is not as commonly used at the EM yet it is similar in design where the secondary electrons strike a phosphorus screen instead of a dynode. The phosphorus screen releases photons which are detected by the photomultiplier. One advantage of the conversion dynode is that the photomultiplier tube is sealed in a vacuum, unexposed to the environment of the mass spectrometer and thus the possibility of contamination is removed. This improves the lifetimes of these detectors over electron multipliers. A five-year or greater lifetime is typical, and they have a similar sensitivity to the EM (Chiu & Muddiman, 2008).

#### **<IP_ADDRESS> The daly detector**

454 Tandem Mass Spectrometry – Applications and Principles

detector is not particularly sensitive, offering limited amplification of signal, yet it is tolerant of relatively high pressure (Chiu & Muddiman, 2008). Faraday cup detectors have high accuracy, constant sensitivity, and low electrical noise. The principal disadvantage of the classical Faraday is tis relatively long time constant inherent in the amplification system associated with the use of a high-ohmic resistor in the circuitry (Watson & Sparkman, 2007).

Modification of a magnetic mass spectrometer to detect negative ions instead of positive ions is relatively simple and the polarity of the accelerating voltage and the magnet current must be reversed. The negative ions have sufficient injection kinetic energy (typically 3~4 kV) to impinge on the EM even though it has a negative bias on its first dynode so that secondary electrons will experience an overall positive gradient toward the last stage(Watson & Sparkman, 2007). In mass spectrometer that uses quadrupole fields no change is required in the analyzer part of the instrument because the field acts on positive and negative ions equally. In the transmission quadrupole, the repeller and acceleration

With the advent of the desorption/inonization technique MALDI, it has been possible to generate ions of extraordinarily high *m/z* values, however, it is often difficult to detect such ions efficiently because their velocity is relatively low if it depends only on the accelerating voltage of the ion source (Beuhler et al., 1991; Matthew et al., 1986). One technique for improving the detection efficiency of high *m/z* value ions is to provide a "post-acceleration" electric field to increase their velocity prior to impacting the conversion dynode of the detector (Hedin et al., 1987). Detection of macro-ions (those heavier than hundreds of kDa having a single or double charge) has been challenge in modern MS. Conventional MS has relied on ionization-based detectors, namely those producing and multiplying secondary electrons associated with particle bombardment of a metal surface; such detectors are restricted to ions having a mass less than 106 Da. An ion-to-proton conversion detector (IPD) shows promise for detecting macro-ions (Dubois et al., 1997; Dubois et al., 1999). Photosensitive detectors, relying on laser-indued fluorescence (LIF) or elastic light scattering

CEMA consists of a honeycomb arrangement of many channels up to several hundred per square inch, each having a diameter on the order of 10 m made possible with fiber optic technology using metal-doped glass. A potential difference applied to opposite ends of the channels with top and bottom of the honeycomb creates an electrical gradient along the resistive but conducting surface of each channel. The ions enter the individual channels slightly off-axis so that they impinge the wall of the channel. This primary event (an ion colliding with the surface to expel electrons) has very poor efficiency; the efficiency is directly proportional to the velocity of the impacting ion, which explains the exceptionally poor response of the CEMA to massive ions. The secondary electrons resulting from ions impinging the wall continue to ricochet down the channel, producing more secondary electrons upon each impact, thereby amplifying the original ion beam (Watson & Sparkman, 2007). The CEMA is also employed in TOF-MS because it presents a simple flat surface that can be arranged perpendicular to the ion beam to preserve velocity resolution of the ion

**<IP_ADDRESS> Negative-ion detection**

**<IP_ADDRESS> Post-acceleration detector**

(ELS), show promise in this area.

packets (Price & Milnes, 1984).

**<IP_ADDRESS> Channel Electron Multiplier Array (CEMA)**

voltages have to be changed from positive to negative.

The positive ion beam passing the detector slit is attracted toward an aluminized cathode (the Daly knob) held at a very large negative potential (e.g. -15,000 V) (Daly et al, 1968a; Daly et al, 1968b). Positive ions impacting the Daly knob, which essentially serves ac a conversion dynode, produces up to eight secondary electrons, which are attracted to scintillator unit held at ground potential. The Daly detector offers two significant advantages over other similar detectors. First, most of components (all except the Daly knob) are located outside the vacuum chamber, and thus can be served without distrupting the pressure regime of the mass spectrometer. Second, the large potential difference used between the Daly knob and the slit is particularly advantageous for detecting ions of high mass as a post-accelerator detector. In addition, a deceleration lens can be installed in front of Daly knob to distinguish between stable ions and those that are ionic products of metastable decay (Watson & Sparkman, 2007)

#### **<IP_ADDRESS> Array detector**

An array detector is a group of individual detectors aligned in an array format. The array detector, which spatially detects ions according to their different *m*/*z*, has been typically used on magnetic sector mass analyzers. Spatially differentiated ions can be detected simultaneously by an array detector. The primary advantage of this approach is that, over a small mass range, scanning is not necessary and therefore sensitivity is improved ( Chiu & Muddiman, 2008).

#### **2.2.6 Vacuum techniques and systems**

All mass spectrometer need a vacuum to allow ions to reach the detector without colliding with other gaseous molecules or atoms. If some collisions between molecules did occur, the instrument would suffer from reduced resolution and sensitivity. Low pressure (i.e. infrequent ion/molecule or molecule/molecule collisions) is also essential for preservation of resolving power in *m/z* analyzers. Once the direction of an ion's path has been established, any interaction with other matter can cause that direction to change (Watson & Sparkman, 2007). One of the first obstacles faced by the originators of mass spectrometer was coupling the sample source to a mass spectrometer. The sample is initially at atmospheric pressure (760 torr) before being transferred into the mass spectrometer's vacuum (~10-6 torr), which represents approximately a billion-fold difference in pressure. One approach is to introduce the sample through a capillary column (GC) or through a small orifice directly into the instrument. Another approach is to evacuate the sample chamber through a vacuum lock (MALDI) and once a reasonable vacuum is achieved (< 10-2 torr) the sample can be presented to the primary vacuum chamber (< 10-5 torr). The

Principles and Applications of LC-MS/MS

technology mindmap (Figure 6).

NMR X-ray Simultaneous Moving Bed (SMB)

> Ligand Based Target Based

> > Experiment Simmulation

> > > Different Display

Protein Purification Protein-Protein Interaction Quantitative Proteomics Ligand-Receptor Interaction

Chiral Stationary Phase Derivatization Chiral Electrolyte Additive Optical Purity Test Absolute Configuration Determination CD Spectropolarimeter Modeling Open Column (Ion Exchange ) Prep-LC

Diffusion NMR TRNOE Spin-Echo 1H-15N Correlation SAR by NMR

2DE Image Analyzer 1D Chromatography Electrophoresis Prep-LC

> Screening Screening Labeling MS

Affinity Chromatography GPC

> Isotope Labelling MALDI-TOF Screening

Target Validation Toxicity Test Screening Chromatography CE NMR

> NMR Screening Docking Study

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 457

physical interaction with macro-molecules (Vogeser & Kirchhoff, 2011). During the past decade, LC-MS/MS technologies have substantially extended the methodologic armamentarium of clinical laboratories (Vogeser & Seger, 2008). It has become one of the essential basic technologies used in laboratory medicine that shown in the analytical

> Analytical Technology

Fig. 6. Mindmap for description of analytical technology (www.bene-technology.com).

In the MS method, in contrast, analytes are detected directly from the molecular characteristics as molecular mass and molecular disintegration patterns. Thus, MS techniques are very attractive for quantification of biomarkers or xenobiotics in the context of diagnostic procedures, since those techniques can enable analyses of much higher specificity compared to standard technologies such as photometry or ligand binding tests. With GC-MS, first MS was introduced to laboratory medicine about 40 years ago. GC-MS allowed the highly specific and sensitive quantification of thermo-stable molecules below a molecular weight of about 500 and became a key method in the toxicology field. With the respect to standardisation and quality assurance of small molecule analytical routine methods the introduction of GC-MS as a reference method was an essential progress, in particular for endocrinology. However, for the several reasons the application of GC-MS remained restricts too few specialized institution in laboratory medicine including mainly toxicological laboratories, metabolism centre, and reference laboratories. The handling and maintenance of GC-MS instruments is very demanding and time-consuming; sample preparation is very laborious and includes sample extraction and analyte derivatization; the analytical run times are long with a typical sample throughput of less than 50 samples per

Introduction of API techniques about 20 years ago made practically all potential bio-medical analytes amenable for MS. Furthermore, powerful new technologies of ion-analyses (tandem MS, TOF-MS, ion-trap MS) substantially increased the capabilities of MS analyzers with respect to specificity and to the extent of data read-out in the 1990s. These developments

Chiral Analysis

Separation

NMR

Proteomics

Chiral Generic Drug Chiral Switch

New Efficacy

day (Vogeser & Kirchhoff, 2011).

Absolute Configuration Determination Preparation

> Drug Descovery

Trace Analysis Sample Pre-treatment

Extraction & Concentration Derivatization Protein Digestion Chromatography Spectroscopy Down-stream Analysis Electrophoresis Prep-LC

LLE, SPE, SPME TLC Headspace, Purge & Trap Chiral Auxiliary ICAT Nano-LC NMR Cryogenic Tech. FT-IR/Raman

LC/MS, GC/MS, HR-MS IC

> LC-NMR/MS Multi-Dimensional LC/MS

Analysis

Collection

NMR

Experiment

Double Resonance Triple Resonance Molecular Motion NMR Experiment TROSY, CRINEPT Residual Dipolar Coupling (RDC) GFT NMR Spectrum Analysis nOe Analysis Auto Analysis Structure Building Up using nOe Molecular Modeling NMR Sample Preparation Stable Isotope Labeling

Ligand-Receptor Interaction Post-Traslation Modification

Electrophoresis Digestion MS AA Sequencer Bioinformatics (Protein DB) MALDI-TOF Q-TOF

Assignment Simmulation Preparation

MS X-ray

Proteomics

Structural Analysis

mechanical pump serves as a general workhorse for most MS and allows for an initial vacuum of about 10-3 torr to be obtained. Once a 10-3 torr vacuum is achieved, the other pumping systems, such as diffusion, cryogenic and turbomolecular can be activated to obtain pressures as low as 10-11 torr (Figure 5) (Chiu & Muddiman, 2008).

Fig. 5. A well-maintained vacuum is essential to the function of a mass spectrometer (Chiu & Muddiman, 2008).

#### **2.2.7 Conclusion**

The mass spectrometer as a whole can be separated into distinct sections that include the sample inlet, ion source, mass analyzer, and detector. A sample is introduced into the mass specterometer and is then ionized. The ion source produces ions either by electron ejection, electron capture, cationization, deprotonation or the transfer of a charged molecule from the condensed to the gas phase. MALDI and ESI have had a profound effect on mass spectrometry because they generate charged intact biomolecules into the gas phase. In comparison to other ionization sources such as APCI, EI, FAB, and CI, the techniques of MALDI and ESI have greatly extended the analysis capabilities of mass spexterometry to a wide range of compounds with detection capabilities ranging from the picomole to the zeptomole level. The mass analyzer is a critical component to the performance of any mass specterometry. Among the most commonly used are the quadrupole, quadrupole ion trap, TOF, TOFR, and FTMS. However, the list is growing as more specialized analyzers allow for more difficult questions to be addressed. For example, the development of the quad-TOF has demonstrated its superior capabilities in high accuracy tandem mass spectrometry experiments. Once the ions are separated by the mass analyzer they reach the ion detector, which is ultimately responsible for the signal we observe in the mass spectrum.

#### **3. Recent development of in high-throughput quantitative bioanalysis by liquid chromatography (LC) coupled with mass spectrometry (MS or MS/MS)**

Development of standard techniques of analytical detection in clinical chemistry relies on indirect characteristics of an analyte, e.g. its absorption of light, chemical reactivity or

mechanical pump serves as a general workhorse for most MS and allows for an initial vacuum of about 10-3 torr to be obtained. Once a 10-3 torr vacuum is achieved, the other pumping systems, such as diffusion, cryogenic and turbomolecular can be activated to

Fig. 5. A well-maintained vacuum is essential to the function of a mass spectrometer (Chiu

The mass spectrometer as a whole can be separated into distinct sections that include the sample inlet, ion source, mass analyzer, and detector. A sample is introduced into the mass specterometer and is then ionized. The ion source produces ions either by electron ejection, electron capture, cationization, deprotonation or the transfer of a charged molecule from the condensed to the gas phase. MALDI and ESI have had a profound effect on mass spectrometry because they generate charged intact biomolecules into the gas phase. In comparison to other ionization sources such as APCI, EI, FAB, and CI, the techniques of MALDI and ESI have greatly extended the analysis capabilities of mass spexterometry to a wide range of compounds with detection capabilities ranging from the picomole to the zeptomole level. The mass analyzer is a critical component to the performance of any mass specterometry. Among the most commonly used are the quadrupole, quadrupole ion trap, TOF, TOFR, and FTMS. However, the list is growing as more specialized analyzers allow for more difficult questions to be addressed. For example, the development of the quad-TOF has demonstrated its superior capabilities in high accuracy tandem mass spectrometry experiments. Once the ions are separated by the mass analyzer they reach the ion detector,

which is ultimately responsible for the signal we observe in the mass spectrum.

**3. Recent development of in high-throughput quantitative bioanalysis by liquid chromatography (LC) coupled with mass spectrometry (MS or MS/MS)**  Development of standard techniques of analytical detection in clinical chemistry relies on indirect characteristics of an analyte, e.g. its absorption of light, chemical reactivity or

& Muddiman, 2008).

**2.2.7 Conclusion**

obtain pressures as low as 10-11 torr (Figure 5) (Chiu & Muddiman, 2008).

physical interaction with macro-molecules (Vogeser & Kirchhoff, 2011). During the past decade, LC-MS/MS technologies have substantially extended the methodologic armamentarium of clinical laboratories (Vogeser & Seger, 2008). It has become one of the essential basic technologies used in laboratory medicine that shown in the analytical technology mindmap (Figure 6).

Fig. 6. Mindmap for description of analytical technology (www.bene-technology.com).

In the MS method, in contrast, analytes are detected directly from the molecular characteristics as molecular mass and molecular disintegration patterns. Thus, MS techniques are very attractive for quantification of biomarkers or xenobiotics in the context of diagnostic procedures, since those techniques can enable analyses of much higher specificity compared to standard technologies such as photometry or ligand binding tests. With GC-MS, first MS was introduced to laboratory medicine about 40 years ago. GC-MS allowed the highly specific and sensitive quantification of thermo-stable molecules below a molecular weight of about 500 and became a key method in the toxicology field. With the respect to standardisation and quality assurance of small molecule analytical routine methods the introduction of GC-MS as a reference method was an essential progress, in particular for endocrinology. However, for the several reasons the application of GC-MS remained restricts too few specialized institution in laboratory medicine including mainly toxicological laboratories, metabolism centre, and reference laboratories. The handling and maintenance of GC-MS instruments is very demanding and time-consuming; sample preparation is very laborious and includes sample extraction and analyte derivatization; the analytical run times are long with a typical sample throughput of less than 50 samples per day (Vogeser & Kirchhoff, 2011).

Introduction of API techniques about 20 years ago made practically all potential bio-medical analytes amenable for MS. Furthermore, powerful new technologies of ion-analyses (tandem MS, TOF-MS, ion-trap MS) substantially increased the capabilities of MS analyzers with respect to specificity and to the extent of data read-out in the 1990s. These developments

Principles and Applications of LC-MS/MS

**3.1.1 Basic principles of sample preparation**

analyte, but also for the individual MS/MS system.

**3.1.2 Automated off-line sample preparation**

**3.1 Sample preparation**

for the Quantitative Bioanalysis of Analytes in Various Biological Samples 459

Adequate sample preparation is a key aspect of quantitative bioanalysis and can often be the cause of bottlenecks during high-throughput analysis. Sample preparation techniques in 96 well format have been well adopted in high-thoughput quantitative bioanalysis. Four main principles of sample extraction are applied in LC: PPT by addition of organic solvents, inorganic acids and/or chaotropic salts, protein filtration, LLE, and SPE. Typically not a very high degree of protein removal is achieved. The increasing demand for highthroughput causes a unique situation of balancing cost versus analysis speed as each sample preparation technique offers unique advantages. Sample preparation with PPT is widely used in bioanalysis of plasma samples. The method has been extended to quantitation of drug and metabolites from whole blood. A sensitive and specific LC–MS/MS method for the simultaneous determination of cyclosporine A and its three main metabolites (AM1, AM4N, and AM9) in human blood have been developed (Koseki et al., 2006). Overall, PPT offers a generic and fast sample preparation technique that can be easily automated. However, when analyzing supernatant from a plasma sample using PPT, salts and endogenous material are still present and cause ion suppression or enhancement that will lead to higher variation from sample to sample. Solvent extraction and SPE typically result in very clean extracts; ion-suppression effects due to residual matrix components are reduced with solvent extraction and SPE compared to mere PPT (Annesley, 2003; Taylor, 2005). While LLE is predominantly based on differential polarity, a variety of different extraction surfaces is available for SPE such as carbohydrates (C2, C8 and C18), ion exchange materials (De Jong et al., 2007; De Jong et al., 2010a), phenylic groups, amino groups, co-polymer mixed mode materials (Dunér et al., 2007), immobilized on particles packed in cartridges. SPE materials can have added particular functions, as removing of phospholipids. Both LLE and SPE allow up to ten-fold concentration of analytes; however, these methods are technically far more demanding compared to PPT. The optimum choice of one of the four main principles of sample preparation is specific for the respective