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Engineering Science EAB_S_127 Electricity Chapter 4 Introduction Capacitance Energy stored in a capacitor Charging and Discharging through a resistor Time constants Capacitance Capacitors are devices which store electrical charge A capacitor consists of two plates separated by an insulator, as shown in Figure 4.1 The negative plate is connected to a low potential and the positive plate to a high potential Insulator Q - + - + - + V Negative plate Figure 4.1 Positive plate Capacitance continued The total amount of the charge stored, is denoted by Q and the voltage across the plates by V Q The capacitance then is defined as C [F ] V Where C is in Farads 1 Farad = 1 Coulomb per Volt Insulator Q - + - + - + V Negative plate Figure 4.1 Positive plate Energy Stored in a Capacitor When charged, a capacitor stores electrical energy Recall the formula for electrical energy in a circuit, which is W = VQ However, we need to be careful as the voltage between the plates in a capacitor varies from 0 to V Hence, to be more accurate we should use the average 0 Vab Vab voltage Vm W VmQ So Hence W Vab Q 2 2 2 and we know Vab 1 CVab CVab2 2 2 Q CVab Energy Stored in a Capacitor: Example Question: A capacitor is supplied with 10 V in a circuit. If its capacitance is 150µF, what is the electrical energy stored in the capacitor? Answer: W 1 1 CVab2 150 10 6 10 2 75 10 4 J 7.5mJ 2 2 Charging and Discharging a Capacitor Charging and discharging a capacitor from a DC (direct current) source is shown below V We assume that the voltage source,V, has no internal resistance If the switch was held in position 2 for a long time, then the capacitor would be completely discharged, Vc = 0V Charging a Capacitor If the switch is then moved to position 1, current will start to flow through the resistor R, thereby charging the capacitor, C The voltage across the plates of the capacitor will rise in time, until after a long time, the capacitor will have the same voltage as the supply,V V VC Discharging a Capacitor If the switch is then moved back to position 2, current will start to flow through the resistor R, thereby discharging the capacitor, C The voltage across the plates of the capacitor will fall in time, until after a long time, the capacitor will have no charge at all and again, Vc = 0V V VC Time Constant of an RC Circuit It can be shown mathematically, that the time for the voltage to fall to 37% of its original voltage, t = RC The charging and discharging curves have an exponential nature When discharging VC When charging VC RC Time Constant: Example Question: If R = 1000W and C = 0.1mF, what is the time constant of the circuit? Answer: t = RC = 1000x0.1x10-6 = 0.1 x10-3 = 100ms Hence, when discharging, the following equation can be used to calculate the voltage When charging Summary Learning Outcomes: Capacitors and capacitance Energy stored in a capacitor Charging a capacitor Time constants Exponential charging and discharging curves