4Current and Voltage Relationship Q=CV (at t=t1) (Current is 0)If you increase voltage by ∆V, then more charges will be shoved to the capacitor. (Q+ ∆Q)Here is what we have. Q+ ∆Q=C(V+ ∆V)Charges can not be moved instantaneously. The accumulation of charges will take place between t1 and t1+ ∆tWe are interested only in the incremental change of charges. ∆Q/ ∆t=C ∆V/ ∆t=i
5Current and Voltage Relationship i=C ∆V/ ∆t∆V/ ∆t represent the rate of change of voltage across a capacitor.The faster the rate of change, the greater the current.∆V/ ∆t is the slope VC vs time plot.
6The rate of change of a sine wave Determine the slope by putting a ball on the curve.
9Capacitive Impedance as a function of frequency IC=C ∆V/ ∆tThe faster the voltage changes, the higher the frequency,the greater the current, and hence lower the Impedance.So ZC, the Impedance, is inversely proportional to f.
10Impedance as a function of Capacitor i=C ∆V/ ∆tAssume that ∆V/ ∆t is constant, the larger the C, the greater the current.In other words, ∆V/ ∆t represent changes in the voltage across the capacitor. The changes in VC can not happen without the changes in Q. A larger the capacitance will require more charges for the same ∆V/ ∆t. So it will require more current.Reactance is inversely proportional to capacitance.
11Similarity to resistance ADD impedance of series capacitorsZTC=ZC1+ZC2+ZC3Calculate Impedance of parallel capacitors like parallel resistors.ZTC=ZC1ZC2/(ZC1+ZC2)
15Capacitive Voltage Divider Vx=(XCx/Xc,tot) VsThis is similar to the formula for voltage divider
16Power in a capacitorInstantaneous PowerTrue PowerReactive Power
17Power curveInstantaneous power fluctuates as twice the frequency of voltage and current.Ideally all the energy stored by a capacitor during the positive power cycleis returned to the source during the negative portionNote that the average power is 0.
21Understanding ZL IC=VC [-j/(ωL)] An inductor has a natural tendency to resist change in current. Therefore, as the frequency of VC increases, it will not be able to keep up with changes.At sufficiently high frequencies, the current will cease to track the voltage, and begins to behave as an open circuit.
22Inductive reactance formula In general:XL=2ΩfL=ωLFor series inductors:XLT=XL1+XL2+XL3….For parallel inductors:1/XLT=1/XL1+1/XL2+1/XL3