Practical implications of some recent studies in electrospray ionization fundamentals
Authors: Cech Nadja B. , Enke Christie G. 
Published: July 2005

I.
Introduction
363

II.
The Mechanics of ESI‐MS
363

III.
Analyte Characteristics and Selectivity
365

A.  Charging the Analyte
366

  1. Ionization Through Charge Separation
366

  2. Adduct Formation
366

  3. Ionization Through Gas‐Phase Reactions
366

  4. Ionization Through Electrochemical Oxidation or Reduction
368

B.  Analyte Surface Activity and Its Effect on ESI Response
368

  1. Surface Activity and the Fissioning Process
369

  2. Predicting ESI Response from Other Parameters
369

C.  The Role of Analyte pKa and Solvent pH
370

D.  Improving ESI Response Through Derivatization
371

IV.
The Working Curve and Dynamic Range
373

A.  Detection Limits With ESI
373

  1. Background Interferences
373

  2. Random Noise
374

  3. Ion Transmission and Sensitivity
374

B.  Sources of Signal Saturation at High Concentrations
375

  1. Limited Amount of Excess Charge
375

  2. Limited Space on Droplet Surfaces
375

  3. Suppression and Competition at High Concentrations
376

C.  Improving the Detection Limit and Linear Dynamic Range
376

  1. Extending to Higher Concentrations
376

  2. Extending to Lower Concentrations
376

V.
Instrumental Parameters and Stability
377

A.  Current–Voltage Curves
377

B.  Effect of Instrumental Parameters on the Current–Voltage Curve
378

C.  Self‐Stabilizing Operation
379

D.  Non‐Conductive vs. Conductive Spray Capillaries
379

VI.
Solution Characteristics
380

A.  The Ideal ESI Solvent
380

B.  Solvent Choice for Analysis in the Positive Ion Mode
381

C.  Solvent Choice for Analysis in the Negative Ion Mode
381

D.  Compatibility Between ESI and Liquid Separation Techniques
382

VII.
Summary
382

VIII.
Acknowledgment
383

References
383

In accomplishing successful electrospray ionization analyses, it is imperative to have an understanding of the effects of variables such as analyte structure, instrumental parameters, and solution composition. Here, we review some fundamental studies of the ESI process that are relevant to these issues. We discuss how analyte chargeability and surface activity are related to ESI response, and how accessible parameters such as nonpolar surface area and reversed phase HPLC retention time can be used to predict relative ESI response. Also presented is a description of how derivitizing agents can be used to maximize or enable ESI response by improving the chargeability or hydrophobicity of ESI analytes. Limiting factors in the ESI calibration curve are discussed. At high concentrations, these factors include droplet surface area and excess charge concentration, whereas at low concentrations ion transmission becomes an issue, and chemical interference can also be limiting. Stable and reproducible non‐pneumatic ESI operation depends on the ability to balance a number of parameters, including applied voltage and solution surface tension, flow rate, and conductivity. We discuss how changing these parameters can shift the mode of ESI operation from stable to unstable, and how current–voltage curves can be used to characterize the mode of ESI operation. Finally, the characteristics of the ideal ESI solvent, including surface tension and conductivity requirements, are discussed. Analysis in the positive ion mode can be accomplished with acidified methanol/water solutions, but negative ion mode analysis necessitates special constituents that suppress corona discharge and facilitate the production of stable negative ions. © 2002 Wiley Periodicals, Inc., Mass Spec Rev 20: 362–387, 2001; Published online in Wiley InterScience (www.interscience.wiley.com). DOI 10.1002/mas.10008