Let us rephrase our pemhamanan of capacitors.<\/span> Capacitors are passive circuit elements which can save energy.<\/span> Capacitors are made of two parallel conductive plates that have a large A (m2) and within each other by d (m).<\/span> With such a relationship then when it gets capacitor electric current will generate a voltage in kapasitronya, where a large value capacitor voltage is:<\/span> Where C is a constant whose value depends on the area and distance plate plate and insulation material that exists between the two plates.<\/span> Mathematically be written as follows:<\/span> Observe the following image.<\/span> A capacitor is connected to a voltage source of direct current through resistor R and is controlled by a switch S as shown below.<\/span> Up here you will want to know what happens when electric current is connected to a capacitor.<\/span> If you make the RC circuit as shown below, notice what happens to the current in the circuit and the voltage on the capacitor?<\/span> Concept<\/strong><\/span> Potential relationship when the capacitor is charged as follows:<\/span> by Vo, VR, and potential sources of VC states, potential barriers and potential on the capacitor, q is the charge which charges the capacitor, i is the current through the circuit and C is the large capacity of the capacitor.<\/span> By using equation (2) and (3), equation (1) can be completed to determine the potential capacitor while charging:<\/span> If the source is removed and linked brief RC circuit (as in the picture above), the capacitor will release its payload.<\/span> Padakondisi potential link is:<\/span> Equation (5) can be resolved into:<\/span>
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\n Where :<\/span>
\n C is called capacitance measured in Farad<\/span>
\n \u03b5 is the permittivity of the dielectric material.<\/span>
\n For air permitifitasnya value is<\/span>
\n \u03b5 = \u03b5 0<\/sub> = 8854 pF \/ m.<\/span><\/p>\n
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\n 3:41 Picture Series RC circuit<\/span><\/p>\n
\n If the direct current source is connected to a capacitor, charges from the source is supplied to the capacitor.<\/span> As a result, the plates in the capacitor, previously neutral, forming different polarity.<\/span> Through resistor R are coupled in series with the capacitor, charging obstacles.<\/span> Therefore, in addition to relying on the voltage source, charging is also dependent on the time.<\/span> The series of images shows the experimental series circuit connected to a DC source.<\/span><\/p>\n
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