Published by Patrick Mutisya · 14 days ago
To distinguish graphically between half‑wave and full‑wave rectification.
Rectification is the process of converting an alternating‑current (AC) voltage into a unidirectional (pulsating) voltage. The most common rectifier circuits are:
The resulting pulsating voltage can be smoothed with a capacitor to obtain a near‑DC supply.
In a half‑wave rectifier the diode conducts only during the positive half‑cycle of the input sinusoid.
The input voltage can be expressed as
\$V{\text{in}} = Vm \sin(\omega t)\$
and the output voltage \$V_{\text{out}}\$ is
\$\$V_{\text{out}} =
\begin{cases}
V_m \sin(\omega t) & \text{for } \sin(\omega t) \ge 0 \\
0 & \text{for } \sin(\omega t) < 0
\end{cases}\$\$
Full‑wave rectifiers invert the negative half‑cycle so that the output voltage is always positive.
For a bridge rectifier the output voltage is
\$V{\text{out}} = |Vm \sin(\omega t)|\$
Thus both positive and negative halves of the input appear as positive pulses at the output.
The key visual differences are:
| Feature | Half‑Wave Rectifier | Full‑Wave Rectifier |
|---|---|---|
| Diodes required | 1 | 2 (centre‑tap) or 4 (bridge) |
| Output during positive half‑cycle | Yes (same polarity as input) | Yes (same polarity as input) |
| Output during negative half‑cycle | No (zero voltage) | Yes (inverted polarity, becomes positive) |
| Frequency of output ripple | \$f\$ (same as input frequency) | \$2f\$ (twice the input frequency) |
| Peak inverse voltage (PIV) on each diode | \$V_m\$ | \$Vm\$ (bridge) or \$2Vm\$ (centre‑tap) |
| Efficiency (ideal) | ≈ 40 % | ≈ 81 % |
Because a full‑wave rectifier provides a higher ripple frequency, a smoothing capacitor discharges less between peaks, giving a lower ripple voltage for the same capacitance. This makes full‑wave rectification the preferred choice for most DC power supplies.
Graphically, half‑wave rectification shows a single pulse per input cycle, whereas full‑wave rectification shows two pulses per cycle, effectively doubling the ripple frequency and improving the efficiency of subsequent smoothing. Understanding these differences is essential for designing reliable DC power supplies in A‑Level physics experiments and practical electronics.