The ESD Control Program Handbook. Jeremy M. Smallwood

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photographs and other material, and for writing the Foreword, as well as for many enlightening discussions over the years. Dave performed the extraordinary feat of reading and commenting on almost all the draft Chapters at least once. This helped enormously in picking up my mistakes and typographic errors, adding or clarifying important points and generally improving my work.

      Several other friends and colleagues have also very kindly read and commented on Chapters of this book and encouraged me in this work. Special thanks are due to Rainer Pfeifle, Charvakka Duvvury and Christian Hinz who each reviewed and commented on various Chapters in detail. Bob Willis also contributed comments, and Charles Cawthorne kindly provided me some photographs from his own ESD training materials. Lloyd Lawrenson kindly allowed me to use Kaisertech facilities for some of my photography. I'm indebted to Lisa Pimpinella of the ESD Association for arranging permission for me to include figures from the 2016 ESD Association Electrostatic Discharge (ESD) Technology Roadmap.

      Last, but definitely not least, I would like to thank my wife Jan for her good‐natured tolerance of my absent mindedness and lack of communication when engrossed in my work, and my daughter Alia for helping improve some of my photographs in preparation for publication in this book.

      Sometimes a range of meanings is common in different industries. For example, the terms conductive, static dissipative, insulative or insulating, and antistatic can mean many different things to different people from different industry areas or in the context of different standards or electrostatic discharge (ESD) control product types. In most cases, only the meaning common in ESD control, and in particular in the context of the IEC 61340‐5‐1 and ANSI/ESD S20.20 and related standards, is emphasized here.

      The task of supervising an ESD control program is often given to personnel from many technical and educational backgrounds. For this reason, the minimum of prior technical knowledge is assumed in this book.

      Despite this, some of the terms used in this document are defined with basic mathematical relationships given where appropriate. This is because simple mathematics often helps to clarify the subject and, in some cases, may be essential to helping the user understand how to specify aspects of an ESD control program. In many cases, these aspects, and their practical importance and application, are discussed further in Chapter 2.

      In electrostatics and ESD work, we often have to deal with very large or very small numbers. For example, the resistance of a material may be measured to be 10 000 000 000 Ω. For convenience and clarity, we use scientific notation and SI unit prefixes as shorthand for numbers (http://physics.nist.gov/cuu/Units/prefixes.html).

Value Scientific notation SI prefix
150 Ω 1.5 × 102 Ω 150 Ω
22 000 Ω 2.2 × 104 Ω 22 kΩ
35 000 000 Ω 3.5 × 107 Ω 35 MΩ
1 000 000 000 Ω 1.0 × 109 Ω or 109 Ω 1 GΩ
1 000 000 000 000 Ω 1.0 × 1012 Ω or 1012 Ω 1 TΩ
0.000 022 F 2.2 × 10−5 F 22 μF
0.000 000 001 F 1.0 × 10−9 F or 10−9 Ω 1 nF
0.000 000 000 15 F 1.5 × 10−10 F 150 pF
0.000 000 000 001 F 1.0 × 10−12 F 1 pF

      1.2.1 Charge

      When talking of static electricity, it is often said that charge is “generated” in certain circumstances. That is not so – all that happens is that a small number of negative charges become separated from their positive companions in a material and end up in a different place. For every negative charge appearing somewhere, there must be a positive charge appearing somewhere else. An object is described as charged if it has a net imbalance of the number of positive and negative charges that it contains. The electrical effects of the charges are no longer balanced, and a net static electrical charge exists at that location. It is this net charge imbalance that we are referring to when we talk about the charge on an object or material.

      The unit of charge is the coulomb (C). In practice, the coulomb is a rather large amount of charge and microcoulombs (μC, 10−6C), nanocoulomb (nC, 10−9C), or even picocoulombs (pC, 10−12C) are more usual. A single electron or proton has a charge of 1.6 × 10−19C. So, an object having even 1nC of net charge has a large number, 6.2 × 109, of unneutralized electrons or protons.

      1.2.2 Ions

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