Back to Basics: Planar Transformers

Planar Transformers

Anyone remotely associated with electrical systems would have seen a transformer. These tend to stick out as big rectangular-shaped units in your circuit and are called wire wound transformers. Most of you would have seen this in use in step or step-down voltage use cases for low frequencies(50Hz) AC power signals. They are built by wrapping enameled wire over a plastic part(bobbin) for both primary and secondary wires. Whenever there is a current change in the primary, there will be an induced current in the secondary. There are different types of ways by which you wind a transformer, but all of it is just to ensure that coupling is high between 2 sides and leakage is low.

Now coming to high-frequency transformers, which are used in SMPSs, where the frequency of switching is several times larger. As freq is higher, you can use thinner wires(Skin effect, refer to older posts) This will help reduce the size of transformers. Now an even better way to reduce spacing(and increase coupling) is to ditch circular wires altogether and get them printed in PCB tracks. That’s exactly what planar transformers are. It’s a stack of PCBs with multiple layers with both primary and secondary current coils printed on them and connected in a certain way. Insulation is provided by the PCB dielectric and you can have more areas for better coupling. This ensures that the height of the unit is drastically reduced. Since these are PCBs, it has better heat dissipation ensuring that the transformers remain cooler. Manufacturability also goes up as it’s repeatable to make PCBs that are SMD mountable with machines than the older wire wounding semi-manual process. You can even create slots on the PCBs to mount your ferrite cores directly in it.

This is one of the key reasons for the size reduction in your phone chargers(refer to older posts). To learn more about the design and state of art of this tech, I would suggest watching a few videos on YouTube on the international workshop conducted by IISc this year. Search IWPMT 2023 for a series of talks on the same.

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Back to Basics: Oscilloscope Part 9: Current Probes

Oscilloscope Current Probes

We can’t close this series on scopes till we discuss the current probes. For measuring current waveforms there are two main methods, one is adding a small resistor in series in the current path and measuring the voltage diff across the resistor with a differential probe as we discussed last week. This method is cumbersome and you can’t always cut up a cable/track to add the resistor.

Internals of a Clamp of a Current Probe

The other way is via Current Probes. A current probe consists of a magnetic core and/or a Hall effect sensor positioned within a clamp. Probe jaws are placed around the conductor you want to measure. Whenever there is a current flow, it induces a voltage in the magnetic core inside the probe. This voltage is directly proportional to the rate of change or derivative of the current enclosed by the loop formed by the probe jaws. To measure DC, you need a hall effect sensor on the core. Hence you see a split core design with it. The induced voltage is fed to an instrumentation amplifier/signal conditioner and fed to the input of the oscilloscope. The probes mention a voltage/Ampere rating with which you will be able to determine the current value on the scope. Select a probe with the appropriate sensitivity for your specific application to measure low signals accurately.

Personally, I use these clamps to measure coil currents in motors clamping around to fine-tune motor currents. It’s a lifesaver for me there.

Pro Tip: To increase sensitivity when measuring small currents, wrap multiple turns through the primary of a current probe.

Concluding the oscilloscope series! It’s been a journey. If you enjoy long post-series like this, drop a comment. Next week, we dive into a new topic!

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