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How are AC signals described, and how do capacitors and inductors oppose alternating current through reactance?

AC signals and reactance: peak, peak-to-peak and RMS values, frequency and period, capacitive and inductive reactance, and the phase relationship between voltage and current.

A focused answer to WJEC A-Level Electronics AC signals and reactance, covering peak, peak-to-peak and RMS values, frequency and period, capacitive and inductive reactance, how reactance varies with frequency, and the phase between voltage and current.

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  1. What this dot point is asking
  2. The answer
  3. Examples in context
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What this dot point is asking

Alternating signals behave differently from DC because capacitors and inductors oppose them in a frequency-dependent way. WJEC expects you to describe AC signals using peak, peak-to-peak and RMS values, relate frequency and period, calculate capacitive and inductive reactance, and state how each varies with frequency and the phase between voltage and current. RMS and reactance calculations underpin the whole filter topic and recur in the exam.

The answer

Describing an AC signal

The RMS value matters because it determines the power delivered: an AC supply quoted as 230 V is the RMS value, with a peak of about 325 V.

Capacitive reactance

Reactance is the AC opposition (in ohms) of a capacitor. Because XCX_C is inversely proportional to frequency, a capacitor passes high frequencies and blocks low frequencies and DC (at DC, f=0f = 0, the reactance is infinite, so no current flows once charged).

Inductive reactance

An inductor's reactance is proportional to frequency, so it blocks high frequencies and passes low frequencies and DC. This opposite behaviour to a capacitor is what lets the two be combined to select frequency bands.

Phase

Examples in context

Example 1. Smoothing a power supply
A large capacitor across a rectified supply has a low reactance to the high-frequency ripple but a high reactance to the slow DC level, so it shunts the ripple to ground while holding the DC. The frequency dependence of XCX_C is what makes the reservoir capacitor smooth the output.
Example 2. A DC-blocking coupling capacitor
Between amplifier stages, a capacitor passes the AC signal (low reactance at signal frequencies) but blocks the DC bias (infinite reactance at DC). This is why coupling capacitors couple signal without disturbing each stage's operating point.
Example 3. RMS and real power
A heater rated at 230 V AC delivers the same average power as a 230 V DC supply because the RMS value is defined to give equal heating. Using the peak (325 V) instead would overstate the power by a factor of two, which is why power calculations always use RMS.

Try this

Q1. A sine wave has an RMS voltage of 10V10\,\text{V}. Find its peak voltage. [2 marks]

  • Cue. Vpeak=Vrms×2=10×1.414=14.1VV_{peak} = V_{rms} \times \sqrt{2} = 10 \times 1.414 = 14.1\,\text{V}.

Q2. State whether a capacitor or an inductor passes DC, and explain in terms of reactance. [2 marks]

  • Cue. An inductor passes DC: at f=0f = 0, XL=2πfL=0X_L = 2\pi f L = 0. A capacitor blocks DC: at f=0f = 0, XC=12πfCX_C = \frac{1}{2\pi f C} is infinite.

Exam-style practice questions

Practice questions written in the style of WJEC exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

WJEC Eduqas 20205 marksA sinusoidal signal has a peak voltage of 8.0V8.0\,\text{V} and a frequency of 1.0kHz1.0\,\text{kHz}. Calculate its peak-to-peak voltage, its RMS voltage, and the capacitive reactance of a 100nF100\,\text{nF} capacitor at this frequency.
Show worked answer →

Peak-to-peak is twice the peak; RMS is the peak divided by root two; reactance uses the capacitor formula.

Peak-to-peak: Vpp=2×8.0=16VV_{pp} = 2 \times 8.0 = 16\,\text{V}.

RMS: Vrms=Vpeak2=8.01.414=5.7VV_{rms} = \dfrac{V_{peak}}{\sqrt{2}} = \dfrac{8.0}{1.414} = 5.7\,\text{V}.

Capacitive reactance: XC=12πfC=12π×1000×100×109=16.28×104=1,590ΩX_C = \dfrac{1}{2\pi f C} = \dfrac{1}{2\pi \times 1000 \times 100 \times 10^{-9}} = \dfrac{1}{6.28 \times 10^{-4}} = 1{,}590\,\Omega (about 1.6kΩ1.6\,\text{k}\Omega).

Markers reward the 16V16\,\text{V} peak-to-peak, the 5.7V5.7\,\text{V} RMS, and the reactance of about 1.6kΩ1.6\,\text{k}\Omega.

WJEC Eduqas 20184 marksExplain how the reactance of a capacitor and of an inductor each change as the frequency rises, and state the phase relationship between current and voltage for a capacitor.
Show worked answer →

Capacitive reactance XC=12πfCX_C = \dfrac{1}{2\pi f C} falls as the frequency rises, so a capacitor passes high frequencies more easily and blocks low frequencies and DC.

Inductive reactance XL=2πfLX_L = 2\pi f L rises as the frequency rises, so an inductor blocks high frequencies and passes low frequencies and DC.

For a pure capacitor, the current leads the voltage by 90 degrees (the current is greatest when the voltage is changing fastest, at the zero crossings).

Markers reward XCX_C falling and XLX_L rising with frequency, and the current leading the voltage by 90 degrees for a capacitor.

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