This topic mixes definitions with short calculations: reactance and resonance, sine-wave voltage forms, power, transformers, and series or parallel components. Most wrong answers come from using a valid relationship in the wrong family, so write the family first and substitute numbers only afterward.
Four families, four decision rules
| Family | Relationship to write first | Direction check |
|---|---|---|
| AC opposition | Z = E / I; reactance is the inductive or capacitive part of opposition to AC | Inductive XL rises with frequency; capacitive XC falls; signal amplitude does not set either reactance |
| Sine-wave voltage | Epeak = ERMS × √2; Ep-p = 2 × Epeak | RMS is smaller than peak, and peak is half the full peak-to-peak swing |
| Transformer | Es / Ep = Ns / Np; Zs / Zp = (Ns / Np)2 | Voltage uses the turns ratio; impedance matching requires its square root |
| Component networks | R and L add in series; C adds in parallel; the opposite connection uses reciprocals | A parallel resistance or inductance is below the smallest branch; a series capacitance is below the smallest capacitor |
Reactance belongs to alternating current. An inductor's changing current creates an opposing voltage, so increasing frequency increases XL. A capacitor has less time to build opposing charge at higher frequency, so increasing frequency decreases XC. At resonance the two reactances are equal in magnitude and opposite in sign, so they cancel. What remains depends on the circuit arrangement: in a series LC circuit only the small series resistance remains and impedance is low; resistance itself has not disappeared.
For sine-wave and power questions, make a conversion chain rather than jumping from the given voltage straight into a power formula. Move from peak-to-peak to peak by halving, from peak to RMS by dividing by √2, and then use the RMS voltage in P = E2 / R. Reverse those steps when RMS is given and the full swing is wanted. RMS is the AC value that produces the same heating in a resistor as the same numerical DC voltage.
Transformer problems have two ratios that look alike but are not interchangeable. Voltage changes in direct proportion to turns, and the transformer works in either direction: driving the winding that was the low-voltage side reverses step-down into step-up. Impedance changes as the square of the turns ratio, so matching two impedances requires taking the square root of their ratio. The low-voltage winding carries the higher current for approximately equal power, which is why it normally needs heavier wire.
Finally, use a magnitude check on component combinations. Series resistors and inductors add, so their total exceeds the largest part. Parallel resistors and inductors use reciprocals, so their total is below the smallest branch. Capacitors reverse that pattern: parallel values add, while series capacitance falls below the smallest capacitor. Convert all metric prefixes to the same unit before applying either rule.
Where the answers are lost
- Swapping the inductor and capacitor directions, or a series resonance result with the parallel case. Options reverse how frequency changes reactance, make signal amplitude control it, make series impedance very high, average component values, cancel resistance, or turn resonance into radiation. Track frequency first, then inspect the remaining circuit path after opposite reactances cancel.
- Inverting an electrical definition. Options turn current divided by voltage into impedance, multiply voltage and current when a ratio is requested, or choose conductance, susceptance, or reluctance as the inverse of the whole AC opposition. Keep Z = E / I and Y = 1 / Z together; P = E × I belongs to power.
- Putting the wrong voltage form into the power law. Options square peak-to-peak or peak voltage as though it were RMS, or halve a peak value instead of dividing by √2. Label every intermediate value before carrying it into the next step.
- Using one transformer relationship for every property. Options divide when the turn count calls for multiplication, keep the input unchanged, add protective resistors merely because the drive direction reversed, or explain heavier low-voltage wire through coupling, parasitic oscillation, or equal winding volume. Voltage follows turns directly; impedance follows turns squared; current moves oppositely for nearly equal power.
- Applying one connection rule to every component. Options average branch currents or make total current fall as branches are added, add parallel resistors, leave a reciprocal sum uninverted, add series capacitors, or report a parallel inductor in henrys when the inputs were millihenrys. Use the magnitude check after the calculation and preserve the unit.
- Losing a metric prefix inside otherwise correct arithmetic. Options treat milliamperes as amperes, mix picofarads with nanofarads, or change millihenrys into henrys without the factor of one thousand. Normalize units before squaring, adding, or taking reciprocals.
Try it
How many watts of electrical power are consumed if 400 VDC is supplied to an 800-ohm load?
- 0.5 watts
- 200 watts
- 400 watts
- 3200 watts
What is the peak-to-peak voltage of a sine wave with an RMS voltage of 120 volts?
- 84.8 volts
- 169.7 volts
- 240.0 volts
- 339.4 volts
What transformer turns ratio matches an antenna’s 600-ohm feed point impedance to a 50-ohm coaxial cable?
- 3.5 to 1
- 12 to 1
- 24 to 1
- 144 to 1