V = IZ
V = rms voltage, I = rms current, Z = total circuit impedance
The impedance Z of a device is sometimes expressed as the sum of a real and imaginary component:
Z = R + jX
R = resistance, j =
, X = reactance
The impedance of a capacitor is -j/(ωC)
ω = ac source frequency, C = capacitance
We can see that the impedance of a capacitor has no real component and has a negative imaginary component, that is to say:
Z = -jX, where we're given X = 100Ω, so Z = -j100Ω
The impedance of an inductor is jωL, ω = source frequency, L = inductance
We can see that the impedance of an inductor has no real component and has a positive imaginary component, that is to say:
Z = jX, where we're given X = 80Ω, so Z = j80Ω
The impedance of a resistor is simply R, R = resistance
WE can see that the impedance of a resistor has a positive real component and no imaginary component, that is to say:
Z = R, where we're given R = 40Ω, so Z = 40Ω
Add up the impedances to get the total impedance:
Z = 40Ω + j80Ω - j100Ω = (40-j80)Ω
To get the rms source voltage, we multiply the rms current I and the impedance Z. These two quantities will be complex numbers, and the math behind multiplying two complex numbers involves <em>multiplying their magnitudes</em>. We already have the magnitude of the rms current 2.2A, so let's calculate the magnitude of the impedance:
|Z| = √(40²+(-80)²)Ω = 89.44Ω
Now let's calculate the rms source voltage V = IZ:
V = 2.2A(89.44Ω)
V = 197V