The hardest electrical-principles items are rarely formula hunts. They test whether you preserve three distinctions while calculating: series versus parallel, positive versus negative reactance, and stored energy versus dissipated energy. Write those labels before inserting numbers.
Reduce the circuit before calculating
| Model | Working rule |
|---|---|
| Resonance | Inductive and capacitive reactance cancel. A series circuit then looks resistive and carries maximum line current; a parallel circuit draws minimum input current while large currents circulate between L and C |
| Q and bandwidth | Half-power bandwidth is resonant frequency divided by Q. Raising Q narrows the response and raises internal reactive voltage in a series resonant circuit |
| Complex form | Use Z = R + jX, with inductive X positive and capacitive X negative. Polar form carries magnitude and phase angle |
| Admittance | Y = 1/Z. In polar form, invert the magnitude and negate the angle; susceptance is Y's imaginary part |
| Power | Only resistance consumes average real power, using I²R. Ideal L and C return their stored field energy instead of dissipating it |
For a series phase-angle problem, calculate net reactance as XL − XC, then use the sign before the magnitude: positive is inductive and voltage leads current; negative is capacitive and voltage lags current. For a reciprocal, do not separately guess how each rectangular component changes when polar form already gives the clean operation.
At RF, the schematic symbol is only the intended term. Leads contribute inductance whose reactance rises with frequency; at microwave wavelengths their propagation delay also creates phase shift. Rolled foil gives an electrolytic capacitor appreciable series inductance, while adjacent turns give an inductor distributed capacitance. A real component self-resonates where its nominal and opposite parasitic reactances match in magnitude.
The traps
- Giving series and parallel resonance the same input behavior. Cancellation makes both resistive, but series input current is high; parallel input current is low even while branch current is high.
- Reading higher Q as wider bandwidth or gentler internal stress. The response narrows, and reactive voltage in a series resonant circuit grows. At parallel resonance, large opposing branch currents can coexist with minimum input current.
- Changing only a sign when taking a reciprocal. Reactance-to-susceptance conversion inverts magnitude as well as reversing the reactive sign; admittance is not merely inverse reactance.
- Losing the lead-lag direction after finding the angle. Capacitive current leads its voltage; inductive voltage leads its current. The sign of XL − XC decides which statement fits a mixed series circuit.
- Swapping rectangular axes or reactive signs. Resistance is the real horizontal component, inductive reactance is positive imaginary, and capacitive reactance is negative imaginary; magnitude and angle describe polar form instead.
- Blaming every RF departure on one parasitic. Short VHF leads address inductive reactance, short microwave connections address phase shift, capacitor construction can add inductance, and coil turns can add capacitance.
Try it
What is the half-power bandwidth of a resonant circuit that has a resonant frequency of 7.1 MHz and a Q of 150?
- 157.8 Hz
- 315.6 Hz
- 47.3 kHz
- 23.67 kHz
What is the half-power bandwidth of a resonant circuit that has a resonant frequency of 3.7 MHz and a Q of 118?
- 436.6 kHz
- 218.3 kHz
- 31.4 kHz
- 15.7 kHz
How much real power is consumed in a circuit consisting of a 100-ohm resistor in series with a 100-ohm inductive reactance drawing 1 ampere?
- 70.7 watts
- 100 watts
- 141.4 watts
- 200 watts