The form factor of an AC waveform is the ratio of its RMS value to its average value. For a perfect sine wave, the form factor is approximately 1.11 (RMS value/Average Value = 1.11). This factor indicates how closely a waveform resembles a pure sine wave; a form factor closer to 1.11 suggests a waveform that is more sinusoidal.
Supply voltage, $$V_{rms} = 110\ V$$
Diode internal resistance, $$R_D = 20\ \Omega$$
Load resistance, $$R_L = 1000\ \Omega$$
The total resistance in the conducting circuit is:
$$R_T = R_D + R_L$$
$$R_T = 20 + 1000 = 1020\ \Omega$$
(i) Peak Load Current
The peak value of the supply voltage is:
$$V_{peak} = \sqrt{2}\,V_{rms}$$
$$V_{peak} = 1.414 \times 110 = 155.56\ V$$
Therefore, the peak load current is:
$$I_{peak} = \frac{V_{peak}}{R_T}$$
$$I_{peak} = \frac{155.56}{1020} = 0.1525\ A$$
Peak load current:
$$I_{peak}\approx0.153\ A=153\ mA$$
(ii) DC Load Current
For a half-wave rectifier, the average or DC value of current is:
$$I_{DC} = \frac{I_{peak}}{\pi}$$
$$I_{DC} = \frac{0.1525}{3.142} = 0.0485\ A$$
DC load current:
$$I_{DC}\approx0.0485\ A=48.5\ mA$$
(iii) AC Load Current
For a half-wave rectified current, the RMS load current is:
$$I_{RMS} = \frac{I_{peak}}{2}$$
$$I_{RMS} = \frac{0.1525}{2} = 0.07625\ A$$
The AC component of the load current is:
$$I_{AC} = \sqrt{I_{RMS}^{2}-I_{DC}^{2}}$$
$$I_{AC} = \sqrt{(0.07625)^2-(0.0485)^2}$$
$$I_{AC} \approx 0.0588\ A$$