ELECTRICAL TERMINOLOGYBasic Electrical TheoryVoltageThe basic unit of measure for potential difference is the volt (symbol V), and, because the voltunit is used, potential difference is called voltage. An object’s electrical charge is determinedby the number of electrons that the object has gained or lost. Because such a large number ofelectrons move, a unit called the "coulomb" is used to indicate the charge. One coulomb is equalto 6.28 x 1018 (billion, billion) electrons. For example, if an object gains one coulomb ofnegative charge, it has gained 6,280,000,000,000,000,000 extra electrons. A volt is defined asa difference of potential causing one coulomb of current to do one joule of work. A volt is alsodefined as that amount of force required to force one ampere of current through one ohm ofresistance. The latter is the definition with which we will be most concerned in this module.CurrentThe density of the atoms in copper wire is such that the valence orbits of the individual atomsoverlap, causing the electrons to move easily from one atom to the next. Free electrons can driftfrom one orbit to another in a random direction. When a potential difference is applied, thedirection of their movement is controlled. The strength of the potential difference applied at eachend of the wire determines how many electrons change from a random motion to a moredirectional path through the wire. The movement or flow of these electrons is called electroncurrent flow or just current.To produce current, the electrons must be moved by a potential difference. The symbol forcurrent is (I). The basic measurement for current is the ampere (A). One ampere of current isdefined as the movement of one coulomb of charge past any given point of a conductor duringone second of time.If a copper wire is placed between two charged objects that have a potential difference, all of thenegatively-charged free electrons will feel a force pushing them from the negative charge to thepositive charge. This force opposite to the conventional direction of the electrostatic lines offorce is shown in Figure 9.ES-01 Page 10 Rev. 0
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