Lesson Alternating current · The alternating wave
Waveforms
An AC waveform is a graph of voltage or current versus time. The sine wave is the ideal shape produced by rotating generators and assumed in most calculations—but you will also see distorted waves from electronics, VFDs, and harmonics. Learn period, frequency, amplitude, and cycle so meter readings, scope traces, and nameplate values all describe the same event.
Voltage and current change with time
In DC, a steady 12 V is a flat line on a chart. In AC, the instantaneous value rises, falls, reverses, and repeats. Plot vertical = volts (or amperes), horizontal = time. Each point on the curve is the value at that instant—what an oscilloscope shows in real time.
The sine wave as the reference shape
A sinusoidal wave follows the smooth curve of trigonometry's sine function. Utility power is designed to be nearly sinusoidal at the meter. Why it matters:
- Rotating machines produce sine waves naturally.
- Most AC theory (RMS, power, transformers) assumes sine unless noted.
- Non-sine waves can be broken into sine harmonics (advanced topic)—but the fundamental is still 60 Hz.
Peak, trough, and amplitude
Peak (maximum) is the highest positive value above the zero axis. The trough is the most negative value. Peak amplitude often means peak magnitude; peak-to-peak spans from trough to peak (twice peak for a symmetric sine). Meters in the field usually read RMS, not peak—do not confuse scope peaks with DMM numbers.
Period and frequency
One cycle is one complete pattern before it repeats. Period (T) is the time for one cycle, in seconds.
Frequency (f) = cycles per second = hertz (Hz).
T = 1 / f and f = 1 / T
At 60 Hz: T = 1/60 ≈ 0.0167 s (16.7 ms per cycle). At 50 Hz: T = 20 ms.
Alternation and zero crossings
Half a cycle from zero → positive peak → back to zero is one positive alternation. The negative half is the negative alternation. Each cycle has two zero crossings where the wave passes through zero volts. Some controls (phase-fired dimmers, certain sync circuits) trigger on zero crossings.
Other common waveforms
| Shape | Character | Where you might see it |
|---|---|---|
| Square | Jumps between two levels | Digital logic, switching supplies (idealized) |
| Triangle | Linear ramps up and down | Some oscillators, test signals |
| Sawtooth | Linear rise, sharp fall | Sweep circuits, old TV deflection (historical) |
| Distorted sine | Flattened peaks, steps | VFD output, loaded generators, harmonic-heavy loads |
Real "square" waves have finite rise time; real sine waves have slight flat-topping under heavy nonlinear load.
Phase and multiple waves
When you plot two sine waves on the same time axis—voltage and current, or two phases—they may line up (in phase) or shift (out of phase). That horizontal shift is phase angle, measured in degrees or radians of a cycle (360° = one period). Resistive loads start in phase; inductors and capacitors shift—next courses.
Reading a scope vs a meter
An oscilloscope shows instantaneous shape and peak values. A true-RMS multimeter reduces the wave to one effective heating value (next lesson). A average-responding meter calibrated on sine can lie badly on distorted waves. Always know what the instrument assumes about the wave.
Degrees, cycles, and angular velocity
One full cycle spans 360° electrically. Half a cycle is 180°; a quarter cycle is 90°. The sine wave reaches maximum at 90°, crosses zero at 180°, reaches negative peak at 270°, and completes at 360° (same as 0°).
Angular velocity: ω = 2πf radians per second. At 60 Hz, ω ≈ 377 rad/s. You will see ω in advanced formulas; for field work, degrees per cycle and time per cycle matter most when aligning scope triggers or comparing phase shifts.
Time axis skills on a scope
When you set horizontal scale to 5 ms/div on 60 Hz, one cycle (16.7 ms) spans roughly 3.3 divisions—a quick sanity check that you are on utility frequency and not harmonics or noise. Count full cycles across the screen before calling a waveform "clean."
Waveform and equipment stress
Peaks matter for insulation and clearance (peak voltage stress). RMS matters for heating and fuse sizing. Frequency matters for motors and transformers. Shape matters for harmonics and neutral current. One number rarely tells the whole story.
A motor rated for 60 Hz expects a smooth rotating field built from a sine-like wave; severe distortion increases heating and noise even when RMS voltage reads nominal.
Field case
Situation. A technician scopes a 120 V branch: the trace shows a clean sine, 60 Hz, peak about 170 V, period 16.7 ms. A helper says "the circuit is overvoltage—170 V on a 120 V system."
Explanation. 120 V is the RMS nominal value. Peak ≈ 120 × 1.414 ≈ 170 V on a sine wave—normal, not an overvoltage fault. The waveform lesson links the shape to the numbers on different tools.
Applied lesson. Match instrument type to the question: scope for shape and peaks; true-RMS meter for effective heating value.
Tip. Photograph scope settings (V/div, ms/div, coupling) when documenting "normal" waveforms for a site baseline—saves debate on the next service call.
In the field
Symptom
Scope peak much higher or lower than 1.414 × DMM reading
Where to look
Distortion, DC offset, wrong probe scale, non-sine load
Likely causes
- Harmonics, clipping, measurement on square-ish inverter output
What to measure
- Frequency, peak, RMS with appropriate meter
- capture one full cycle
What not to do
- Compare scope peak directly to RMS nameplate without conversion
Checklist
- I plot AC as value vs time and read instantaneous points
- I define period, frequency, cycle, alternation
- I use T = 1/f and f = 1/T at 60 Hz or 50 Hz
- I distinguish peak, peak-to-peak, and RMS (preview)
- I recognize sine vs common non-sine shapes
- I know 120 V nominal is RMS, not peak, on utility sine
- I can estimate one cycle width on a scope at 60 Hz