Description
An increasing number of appliances draw a very small current from the
power supply. If you need to design a mains powered device, you could
generally choose between a linear and a switch-mode power supply.
However, what if the appliance’s total power consumption is very small?
Transformer-based power supplies are bulky, while the switchers are
generally made to provide greater current output, with a significant
increase in complexity, problems involving PCB layout and, inherently,
reduced reliability.
Is it possible to create a simple, minimum part-count mains (230 VAC
primary) power supply, without transformers or coils, capable of
delivering about 100 mA at, say, 5 V A general approach could be to
employ a highly inefficient stabilizer that would rectify AC and,
utilizing a zener diode to provide a 5.1 V output, dissipate all the
excess from 5.1 V to (230×v2) volts in a resistor. Even if the load
would require only about 10 mA, the loss would be approximately 3 watts,
so a significant heat dissipation would occur even for such a small
power consumption.
At 100 mA, the useless dissipation would go over 30 W, making this
scheme completely unacceptable. Power conversion efficiency is not a
major consideration here; instead, the basic problem is how to reduce
heavy dissipation and protect the components from burning out. The
circuit shown here is one of the simplest ways to achieve the above
goals in practice. A JVR varistor is used for overvoltage/surge
protection. Voltage divider R1-R2 follows the rectified 230 V and, when
it is high enough, T1 turns on and T3 cannot conduct.
Circuit diagram:
When the rectified voltage drops, T1 turns off and T3 starts to
conduct current into the reservoir capacitor C1. The interception point
(the moment when T1 turns off) is set by P1 (usually set to about 3k3),
which controls the total output current capacity of the power supply:
reducing P1 makes T1 react later, stopping T3 later, so more current is
supplied, but with increased heat dissipation. Components T2, R3 and C2
form a typical ‘soft start’ circuit to reduce current spikes this is
necessary in order to limit C1’s charging current when the power supply
is initially turned on. At a given setting of P1, the output current
through R5 is constant.
Thus, load R4 takes as much current as it requires, while the rest
goes through a zener diode, D5. Knowing the maximum current drawn by the
load allows adjusting P1 to such a value as to provide a total current
through R5 just 5 to 6 mA over the maximum required by the load. In this
way, unnecessary dissipation is much reduced, with zener stabilization
function preserved. Zener diode D5 also protects C1 from over voltages,
thus enabling te use of low-cost 16 V electrolytics.
The current flow through R5 and D5, even when the load is
disconnected, prevents T3’s gate-source voltage from rising too much and
causing damage to device. In addition, T1 need not be a high-voltage
transistor, but its current gain should exceed 120 (e.g. BC546B, or even
BC547C can be used).
CAUTION!
The circuit is not galvanically isolated from the mains. Touching any
part of the circuit (or any circuitry it supplies power to) while in
operation, is dangerous and can result in an electric shock! This
circuit should not be built or used by individuals without proper
knowledge of mains voltage procedures.
Copyright: Elektor Electronics Magazine
Author: Srdjan Jankovic & Branko Milovanovic
Author: Srdjan Jankovic & Branko Milovanovic