A brief note on AC Voltage and Simple AC Circuits . Read it before a test. Try each question at the end before you open its answer.
The alternating voltage The equation: v = V m sin ω t v = V_m \sin \omega t v = V m sin ω t , with ω = 2 π f \omega = 2\pi f ω = 2 π f and T = 1 f T = \dfrac{1}{f} T = f 1 . The rms value: V r m s = V m 2 = 0.707 V m V_{rms} = \dfrac{V_m}{\sqrt{2}} = 0.707\, V_m V r m s = 2 V m = 0.707 V m , and I r m s = I m 2 I_{rms} = \dfrac{I_m}{\sqrt{2}} I r m s = 2 I m . Meters and ratings give rms values. Its meaning: the steady current that heats a resistor as much. For any wave, square, take the mean, take the root. The mean: zero over a full cycle, and 2 π I m \dfrac{2}{\pi}\, I_m π 2 I m over half a cycle. One part at a time Resistor: I m = V m R I_m = \dfrac{V_m}{R} I m = R V m . The current is in phase with the voltage. P = V r m s I r m s = V r m s 2 R P = V_{rms} I_{rms} = \dfrac{V_{rms}^2}{R} P = V r m s I r m s = R V r m s 2 . Coil: X L = ω L = 2 π f L X_L = \omega L = 2\pi f L X L = ω L = 2 π f L . The current lags by 90 ∘ 90^\circ 9 0 ∘ . It passes direct current and holds back fast changes. Capacitor: X C = 1 ω C = 1 2 π f C X_C = \dfrac{1}{\omega C} = \dfrac{1}{2\pi f C} X C = ω C 1 = 2 π f C 1 . The current leads by 90 ∘ 90^\circ 9 0 ∘ . It blocks direct current and passes fast changes. Both reactances: the unit is the ohm, I r m s = V r m s X I_{rms} = \dfrac{V_{rms}}{X} I r m s = X V r m s , and the average power is zero. Memory aid: ELI the ICE man. In L the voltage (E) comes before the current (I). In C the current comes before the voltage. Phasors A phasor is an arrow that turns at ω \omega ω . Its length is the peak value and its vertical part is the value now. The angle between two phasors is the phase difference φ \varphi φ . A phase is a delay Δ t = φ 360 ∘ T \Delta t = \dfrac{\varphi}{360^\circ}\, T Δ t = 36 0 ∘ φ T . Voltages in series add as arrows, tip to tail, not as numbers. A worked example A pure coil of 0.12 0.12 0.12 H and a pure capacitor of 47 μ 47\ \mu 47 μ F are joined, one at a time, to a source of 18 18 18 V rms and 60 60 60 Hz. Find each current.
The coil. X L = 2 π × 60 Hz × 0.12 H = 45.2 Ω X_L = 2\pi \times 60\ \text{Hz} \times 0.12\ \text{H} = 45.2\ \Omega X L = 2 π × 60 Hz × 0.12 H = 45.2 Ω . So I r m s = 18 V 45.2 Ω = 0.398 I_{rms} = \dfrac{18\ \text{V}}{45.2\ \Omega} = 0.398 I r m s = 45.2 Ω 18 V = 0.398 A, lagging the voltage. The capacitor. X C = 1 2 π × 60 Hz × 47 × 10 − 6 F = 56.4 Ω X_C = \dfrac{1}{2\pi \times 60\ \text{Hz} \times 47 \times 10^{-6}\ \text{F}} = 56.4\ \Omega X C = 2 π × 60 Hz × 47 × 1 0 − 6 F 1 = 56.4 Ω . So I r m s = 18 V 56.4 Ω = 0.319 I_{rms} = \dfrac{18\ \text{V}}{56.4\ \Omega} = 0.319 I r m s = 56.4 Ω 18 V = 0.319 A, leading the voltage. Practise with new numbers
Check yourself A voltmeter on an AC supply reads 12 12 12 V. What is the peak voltage? Why does the meter not read the average? Stuck? Show a hint Show the answerThe frequency of a source is made 4 4 4 times larger. What happens to the reactance of a coil and of a capacitor? Stuck? Show a hint Show the answerAt 50 50 50 Hz, the current peak of a pure part comes 5 5 5 ms before the voltage peak. Which part is it? Stuck? Show a hint (1 of 2) Show the answer