Wednesday, February 28, 2024

Simple 12V, 1A SMPS

AshvinI Vishvakarma and Atanu Dasgupta

Most electronics enthusiasts require DC power supplies to operate various devices and accessories. The most popular and common supply is a 12V DC supply that can be easily derived from the household AC supply with transformation, rectification, filtering and stabilisation. These power supplies have a bulky steel- or iron-laminated transformer that provides a safety barrier for the low-voltage output from the AC input, and reduces the input from typically 230V AC to a much lower voltage. The low-voltage AC output from the transformer is then rectified by two or four diodes and smoothed into low-voltage DC by large electrolytic capacitors. Presented here is a 1A, 12V SMPS that can help.

Fig. 1: Author’s prototype of the 12V SMPS
Fig. 1: Author’s prototype of the 12V SMPS

A switched mode power supply (SMPS) offers the same end results at a lower cost and higher efficiency. For a given output power, an SMPS is lighter and smaller. This is because, if the frequency of operation is increased, one can get away with using a smaller core cross-sectional area. Besides, an iron-core transformer works only up to about 10 kHz, and if we need something in 50-100kHz range, we need a ferrite core.


Circuit and working

E47_Table-2Fig. 2 shows the circuit of a simple 1A, 12V SMPS. The circuit is built around a low-power offline switcher TNY266 (IC1), photo-transistor photo-coupler EL817 (IC2), a flyback transformer (X1) and some other easily-available components.

Low-power offline switcher (TNY266). The SMPS here has been designed using a TNY266 chip, which is affectionately called the ‘555’ of SMPS. This device has a 700V power MOSFET, an oscillator, a high-voltage switched current source, a current limiting and thermal shutdown circuitry integrated onto a monolithic device. The start-up and operating power is derived directly from the voltage on the drain (pin 5), eliminating the need for a bias winding and associated circuitry. In addition, the device incorporates auto-restart, line under-voltage sense, and frequency jittering.

- Advertisement -

The drain-source breakdown voltage of the MOSFET in TNY266 is important. During the ‘off’ period, the MOSFET sees rectified 317V DC approximately. Additionally, it sees the reflected voltage of the secondary, which is about 130V AC. It also encounters the ringing voltage from the leakage inductance, and the drain-source capacitance of the MOSFET. Therefore a MOSFET with a Vdss of 650V DC is expected to keep the necessary safe operating margin. Fortunately, a MOSFET with these properties is included in TNY266.

The 230V AC input is connected at CON1, which is rectified by diode D1. The neon lamp (NL1) glows when the input supply is present. Resistor R1 limits the current through the lamp. The rectified output goes to the first terminal (A) of coil L1 and the second terminal (B) is connected to the drain of the inbuilt MOSFET in IC1. Diodes D2 and D3 are essentially the snubbers, and are used to protect the MOSFET from going above 600V.


  1. Dear Sir,
    i have try this circuit at home but i didn’t get its out put. i check its AC &DC voltage across snubber circuit (Diode across primary side of transformer)& capacitor , it shown 696 V & 295V respectively.

    i have design its ferrite core E20 transformer my self using you tube videos , but i didnt get its secondary side voltage . here i am using schottky diode SB560 insist of SB 160.
    Kindly guide what is a fault in the circuit.

    vipin pandey
    [email protected]

  2. Good day Sir,
    Please, I need your help. I have tried building the circuit using your schematic diagram and it work, but the output I’m getting is 3V at the secondary side and it’s the highest I could get even when I increase the number of turns.
    please I need 12V output, what must I do to be able to get this?
    Thank you.


Electronics News

Truly Innovative Tech

MOst Popular Videos

Electronics Components