Low push-pull transformer output voltage often appears only after the load is connected. An isolated rail may look close to its target on the bench, then drop when a communication board, sensor or other secondary-side circuit starts drawing current. A higher turns ratio can help in some designs, but not in all of them. The useful question is where the voltage is being lost: before the transformer, after rectification, or across a regulator that no longer has enough headroom.
VOOHU offers push-pull transformers with a range of turns ratios and inductances. For low-voltage supplies built around 3.3 V or 5 V inputs, considering minimum input voltage and maximum load together is more useful than dividing nominal voltages. The discussion below applies to a common open-loop push-pull driver with center-tapped windings and capacitor-input rectification. Designs with an output inductor, closed-loop regulation or a voltage doubler need the equations for their particular topology.
A supply may indicate 3.3 V while the driver and primary center tap receive less. Cables, connectors, protection circuitry and narrow PCB traces all introduce voltage drops that become more visible as the load increases. Measure close to the actual supply pins, using the local ground on that side of the isolation barrier. If this voltage falls with the load, improve the supply path and decoupling first. Increasing the turns ratio alone can increase the input-current demand.
Compare the voltage across the rectifier reservoir capacitor with the LDO input and output. If the rectified rail is already close to or below the target output, investigate turns ratio, driver voltage drop and winding losses. If there is adequate voltage at the reservoir but the LDO output falls, check dropout, current limiting, temperature and the traces before and after the regulator. Separate a startup dip from a steady-load problem: charging the output capacitor is a different load condition.
For a circuit with symmetrical center taps on both windings, define n as secondary half-winding turns divided by primary half-winding turns. The ratio is unchanged if both sides are expressed using their complete windings. Mixing a complete winding on one side with a half winding on the other creates a factor-of-two error. Identify the center taps and polarity dots before using a quoted ratio in the circuit calculation.
A useful starting point for a push-pull output-voltage calculation is that the ideal secondary pulse amplitude is approximately n times the effective primary voltage during conduction. Rectification, winding resistance and interconnect losses reduce the voltage available to the reservoir capacitor. Load current also lowers the ripple trough. This is a headroom calculation, not a promise of a fixed DC output from the turns ratio alone.
With an LDO after the rectifier, the important condition is: minimum LDO input-voltage trough ≥ required output voltage + dropout at the relevant load and temperature. Input voltage has tolerances, and rectifier drop and regulator dropout change with operating conditions. Start with minimum input, maximum load and the operating-temperature range, then allow for ripple and component variation. A 1:1 ratio does not make 5 V in become a guaranteed regulated 5 V out.
For a worked example, assume a nominal 3.3 V input, a 3.0 V minimum input and a required 5.0 V output. Also assume the LDO needs at least 0.25 V of dropout at the intended load.
At 3.3 V, a 1:1.7 ratio gives an ideal secondary amplitude of 5.61 V, which appears to exceed the 5 V target. At 3.0 V input, however, it gives only 5.10 V. The LDO alone requires at least 5.25 V, before rectifier, winding and driver losses are included. There is therefore insufficient headroom under these assumptions. A near-5 V no-load reading does not establish that the supply will maintain 5 V at full load and minimum input.
At the same 3.0 V input, a 1:2 ratio gives an ideal amplitude of 6.0 V and more headroom to work with. Subtract the actual losses, check the ripple trough, and confirm that driver current, transformer volt-second capability and temperature rise remain suitable. A larger turns ratio changes the voltage relationship; it does not automatically increase the power available from the complete supply.
The following products span near-unity isolation and designs needing additional step-up headroom. First match the voltage relationship to the supply requirement, then consider drive frequency, winding resistance, package and temperature conditions.
| Supply requirement | VOOHU product | Specifications and selection points |
|---|---|---|
| Near-unity isolated voltage conversion | WHST06001A0 | 1:1 turns ratio; 538 μH inductance. Check the voltage after rectification and allow additional headroom if regulation is required. |
| A low-voltage isolated supply needing step-up headroom | WHST06010A0 | 1:1.7 turns ratio; 538 μH inductance. A step-up option whose usable headroom depends on minimum input and loaded losses. |
| A supply requiring a higher ratio than 1:1.7 | WHST06K02A0 | 1:2 turns ratio; 340 μH inductance. More ideal ratio headroom, with light-load voltage, drive current and regulator heating to consider. |
The inductances are not identical, so a change also calls for checking drive frequency and magnetizing current. Neither higher inductance nor a larger ratio translates directly into greater usable power. Match the schematic, PCB pin assignments and mounting orientation to the chosen product rather than assuming that similar-looking packages are interchangeable.
High no-load voltage in an isolated supply can result from open-loop operation and lower losses as current decreases. In the same 1:2 example, a 3.6 V maximum input gives an ideal secondary amplitude of 7.2 V. The regulator and reservoir capacitor must accommodate the highest normal operating voltage, with startup overshoot and ringing considered as well. Their ratings should not be chosen close to 5 V simply because the final output is 5 V.
The main LDO loss is approximately input-to-output voltage difference multiplied by load current. For example, if its actual input is measured at 6.4 V, with 5.0 V output and 100 mA load, that contribution is about 0.14 W. It rises as load current increases. Select enough transformer headroom, not the largest ratio available. Persistent regulator overheating may call for a different regulation approach or improved heat removal.
When an isolated supply drops under load, examine the rectified-voltage trough as well as its average. Capacitance, equivalent series resistance, switching frequency and pulsed loads all affect the trough. The average can look adequate while repeated dips below the LDO input requirement produce output ripple or brief voltage drops. More capacitance can help some ripple problems, but it cannot restore sustained headroom that the turns ratio does not provide. Excessive capacitance can also increase the startup charging burden.
If voltage dips only when a load is switched on and then recovers, focus on the load step, local energy storage and supply loop. If the steady-state voltage continues to fall as the load increases, investigate conduction losses and driver-current capability. Use differential or isolated measurement equipment with suitable common-mode and voltage ratings when measuring across an isolation barrier. An earth-referenced probe connection can unintentionally bridge the two sides.
No. Input-path voltage drop, insufficient turns-ratio headroom, LDO dropout and current limiting can all reduce the output. Compare the driver supply, rectified rail and regulated output before deciding whether the transformer needs to change.
Nominal voltages alone cannot answer that. Multiplying 3.3 V by 1.7 gives 5.61 V, but at 3.0 V input the ideal value is only 5.10 V. Suitability depends on minimum input, rectifier losses, ripple and regulator dropout.
Work out the minimum headroom at low input and maximum load, then check the highest voltage at high input and light load, along with regulator dissipation. Once both ends of the operating range are acceptable, compare transformer losses, size and drive requirements.
Inductance is not the DC voltage-conversion ratio; turns ratio directly affects the ideal secondary amplitude. However, at the same applied voltage and conduction time, a different inductance changes magnetizing current. Driver losses or current limiting can then affect actual output, so consider operating frequency too.
No. It may improve ripple or a brief load transition, but it cannot remove a sustained lack of headroom or replace adequate drive capability. Distinguish a steady-state loss from a transient dip before changing capacitance or the current path.
Include the input-voltage range, target output, maximum and pulsed load current, drive frequency, rectification and regulation arrangement, space constraints and isolation requirements. If a voltage drop already occurs, include no-load and loaded readings and waveforms at the rectified rail and output.
A suitable push-pull supply maintains enough loaded voltage at minimum input without excessive light-load voltage or heating at maximum input. Locate the drop before changing turns ratio; that is often more effective than repeatedly choosing a larger specification. To discuss which of these products fits your supply, contact VOOHU technical support with your operating conditions and application requirements.