As you already know, that the electric charge generating force in the electric field, the opposite atidak jik will accelerate particles contained in the electric charge.<\/span> Let us examine Figure 1:19 (a).<\/span> What’s interesting about this phenomenon is the work done to move the charge in the electric field.<\/span> If the efforts of one joule is needed to drive the charge Q, amounting to one coulomb from position 0 to position 1 and position 1 has a potential of one volt to position 0;<\/span> then 1 V = 1 J \/ C.<\/span><\/p>\n The electric potential is able to do business because of the period (m) as shown in Figure 1:19 (b), in which the period (m) raised against the force of gravity (g) height (h) on a flat surface.<\/span> Ejergi potential (mgh) represents the ability to conduct business when the period (m) released again.<\/span> Because of the period (m) falls, the case and the acceleration potential energy is converted into kinetic energy.<\/span><\/p>\n 1:19 Effort Moving images for Electron<\/span><\/p>\n Potential differences in English voltage or often people refer to as the power supply voltage is the work done to move a charge (amounting to one coulomb) on the element or component of a terminal \/ pole to terminal \/ other poles, or at both terminals \/ poles will have potential difference if we move \/ remove a charge of one coulomb from one terminal to another terminal.<\/span><\/p>\n The linkage between the actual work done is the energy expended, can be shortened so that the above understanding that the voltage is the energy per unit charge.<\/span> Mathematically written:<\/span><\/p>\n There are two ways of analyzing the potential difference, namely: (a) the voltage drop (voltage drop), and the voltage rise (voltage rise).<\/span> For practical applications, commonly used is the second sense that the voltage drop, which when viewed from a higher potential to lower potential in this regard from the terminal A to terminal B.<\/span><\/p>\n
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