Operation of the half-wave rectifier with resistive-capacitive load
Conditions: α=0, ra=0, Ld=0, 0 < C < 
Figure 1.7
The equations describing electric processes in the circuit are

Let's designate:
λ - a pulse thyristor current duration,
φ – a delay angle of the thyristor switching on is fixed concerning a point of natural switching on.
Let's consider intervals:
1) 
The thyristor is on-state:
UT=0;
Let's find IT.

2) -
The thyristor is off-state:
.
According to second Kirchhoff’s law

Characteristic equation is
.
Root of this equation is
.
Then a voltage across the condenser is
.
Current through the load is
.
Current of the condenser is
.
Voltage across the thyristor is
.
Constant A we could be defound from the condition:
At

Then
.
Let's define 
At


Figure 1.7
According to the diagram of changing the function tg(u)
limits by
.
For active load: 
for the capacitive load: ,
From the condition of the no interrupted process, i.e. periodicity of electromagnetic processes in the circuit, we could find φ:

This transcendental equation can be solved graphically or by numerical methods by computer.
Fig. 1.8 – The diagram of electric processes in a single-phase half-wave circuit of the rectifier with resistive-capacitive load.
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