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Charge Redistribution

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Charge Redistribution

Because a spark is an electrostatic effect, and does not conduct a DC current, a return DC path to the source is not needed to support it. See Exhibit 1a.

Exhibit 1: Charge Redistribution

Suppose a voltage V made by charge Q exists on capacitor C1, and capacitor C2 is initially uncharged. There is no energy stored in capacitor C2, so the total energy of the two capacitors is the energy stored in capacitor C1, or QV/2. If the switch is closed, the charge originally present on C1 is redistributed between C1 and C2. Because Q = CV is conserved, and the capacitance is now doubled to 2C, the voltage on the capacitors is now halved, to V/2. The total energy stored in the two capacitors is now Q(V/2)/2 = QV/4. Where did the energy go? The "missing" energy, QV/4, was dissipated in the spark jumping the switch terminals as it closed.

The interesting point in this thought experiment is one that is rarely mentioned; it is not necessary for the "bottom" plates of the capacitors to be connected together, or to anything else, to see this effect, because it is an electrostatic effect — a physical manifestation of charge redistribution. No return path is needed because no direct return current exists—only the displacement current associated with the capacitance between the two capacitors. This is clear to those performing helicopter rescues on ships at sea; triboelectric charging associated with the helicopter moving through the air can result in a significant ESD event when the helicopter lowers its rescue basket to the deck of a ship, especially in dry, fair weather. Sailors are told to let the basket touch the deck first, before they touch it.

Perhaps a more intuitive (and in some ways, more physically correct) view is to remove the ground completely as illustrated in Exhibit 1b, and consider the ESD event to be the discharge of a single capacitance between two objects, one of which is neutral and one of which has a mobile charge Q placed on it. (Because charge is conserved, an object with a charge Q on it exists somewhere in the universe, but this object will be ignored.) Without loss of generality, one may assume the neutral device as a reference; it is clear then that the only currents involved in the ESD event are the current through the discharge itself, and the displacement current through the electric field of the discharging capacitance.

[4]Ajith Amerasekera and Charvaka Duvvury, ESD in Silicon Integrated Circuits. 2nd ed. Chichester, West Sussex, England: John Wiley & Sons. 2002.

[5]The arc has another interesting property — negative resistance. Once it is formed, an increase in current across the arc makes the arc thicker, resulting in a lowering of the voltage drop across the arc. This phenomenon was used to make continuous wave radio transmitters of up to 1 MW of output power by 1918, before the advent of short waves (and the vacuum tube) rendered them obsolete.

[6]This distinction also holds for the arc transmitter, which is not to be confused with the spark transmitter, popular at about the same time but which transmitted damped, instead of continuous, waves.

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