AC Voltage Applied to a Capacitor
When an AC voltage is applied to a capacitor, unlike in a direct current (DC) circuit, the capacitor continuously charges and discharges, allowing current to oscillate. The section elaborates on how the instantaneous voltage across a capacitor relates to the charge and capacitance with the equation v = q/C.
Using Kirchhoff's loop rules, we find that the current is given by the derivative of charge, leading to the relation i = wC * v_m * cos(wt), where v_m
is the peak voltage. The current reaches its maximum value ahead of the voltage by a phase difference of π/2 radians.
In capacitive circuits, the concept of capacitive reactance (
X_c = 1/(wC)
), helps to describe the opposition a capacitor presents to AC. This reactance inversely affects the relationship between current and frequency: as frequency increases, capacitive reactance decreases, allowing greater current.
The average power consumed over a cycle remains zero in an ideal capacitor as the energy stored in the capacitor during charging is returned during discharging. This characteristic reinforces the notion of AC circuits where energy can oscillate in capacitive systems without net energy loss. This section builds a foundation for understanding more complex reactive components in AC circuits.