DC Electronic Loads

An electronic load to test DC power supply devices up to 100W.

What do you use when you have to test a new power supply that you just built, or one that you bought and want to know if the declared specs are true?

One thing you’ll need is a passive load that you attach to the power supply output to drain a certain amount of current, both to verify that the power supply is capable of providing that amount of current, and to verify the amount of ripple that was not filtered away by the power supply itself.

rheostatA classic method for doing so is to use a rheostat, which is essentially a potentiometer capable of dissipating the amount of power produced by the power supply. The resistance of the rheostat can be changed and therefore different amount of currents can be used to test the power supply. However, rheostats are big, heavy and cumbersome.

An alternative to rheostats is to have a so-called Electronic Load. These are electronic circuits that are capable to emulate the functionality of a rheostat.

I’m proposing here two simple versions of an Electronic Load, functioning in DC, and capable of dissipating up to 100W, all of this in a very condensed space, and very light in weight.

The first version is a very simplistic one.

100W_el_load_v1

It uses a cascade of three transistors, in a configuration called Darlington. This configuration is effectively equivalent to a single transistor with a gain (hfe) that is the product of the gain of all the transistors in the configuration. This allows for a very little control current flowing into the potentiometer used to regulate the base current, and for a high current available between the collector and the emitter of the transistor Q3, in the above schematics.

This circuit does not need its own power supply, since it gets what it needs directly from the power supply under test. The resistor R1 is calculated based on the highest voltage that the circuit will be able to handle, in this case 50V. It is important to note, however, that using this load at lower voltages will prevent the possibility to use the full excursion of the potentiometer, thus limiting the sensitivity of the circuit for the control of the current.

The next circuit eliminates the sensitivity problem by providing it own power supply to control the base current of the Darlington, thus eliminating the dependency from the external power supply voltage.

100W_el_load_v2

In fact, in this case, the base current can be adjusted with the potentiometer RV1, which is polarized through the resistor R1 and the trimpot TR1, which can be adjusted to maximize the useful range of motion of the potentiometer, regardless of the voltage applied at the input terminals. This way the electronic load can have the same sensitivity for any input voltage. A digital Volt/Am-meter, powered by the same internal battery, provides a visualization of the voltage of the system under test and the current being drained from it.

I will soon publish a video on my YouTube channel that shows the Electronic Load I built for myself. Please watch for that video to come out. And, in the mean time, can you think which one of the above schematics I used? Did I use the simple one, because less expensive? O did I sacrifice a few extra bucks to gain more sensitivity on the regulation of the load?

I strongly suggest to subscribe for free to my YouTube channel, and also to click on the bell icon that appears after the subscription is done. This will allow you to automatically receive an e-mail whenever I publish a new video. This way you won’t have to go periodically to my channel to check for new posts.

Happy Experiments!

Capacitors – Part 1

A brief introduction to capacitors: what they are, how they are made, and their basic functionality.

capacitorsA capacitor is an electric device capable of storing energy in the form of electric charges (electric field).

In the most simple form, a capacitor is made of two conductive plates facing each other and an insulator in between, which is normally called a dielectric. The two plates are then attached to wires, that are used to connect the capacitor in an electric circuit.

capacitor

The schematic diagram reflects exactly the physical nature of the device:

schematic_symbol

When a capacitor is connected to a power supply, like a battery, electrons leave the plate that is connected to the positive side of the battery, while the same amount of electrons is pushed into the plate connected to the negative side of the battery. Once the difference of charges at the plates of the capacitor is enough to establish a voltage on the capacitor that is identical to the battery, electrons stop moving around the circuit and an equilibrium is reached.

capacitor_and_battery

At this point, if the connection with the battery is severed, the capacitor will retain the amount of charges on its plates: extra charges on the negative plate and defect of charges on the positive plate. If we connect a load to the capacitor, for example a resistor, charges will start moving in the circuit pushed by the voltage at the wires, called electrodes, of the capacitor. So, electrons will leave the negative plate moving toward the load, and an equal amount of electrons will move from the load into the positive plate of the capacitor. The movement of the electrons causes the voltage at the plates of the capacitor to lower until, when an equilibrium of charged is reached, the voltage will be zero and the current will stop flowing through the circuit. At this point all the energy that was stored in the capacitor has been used and the capacitor is said to be discharged.

capacitor_and_load

Both during charge and discharge, the ratio between the amount of charge stored on the capacitor and its voltage remains constant. This can be verified experimentally. We define this constant as the capacitance of the capacitor:

C = Q / V

which is measured in Farad. However, since the Farad is a very big unit, capacitors are normally measured in fractions of Farad, like microFarad (μF, 1 millionth of a Farad)), nanoFarad (nF, one billionth of a Farad), and picoFarad (pF, one trillionth of Farad).

Using the above formula, and calculating the work done to move the charges in and out of the capacitor with the help of some calculus, we can determine the energy stored in a capacitor as:

energy

And, finally, the actual capacitance can also be determined by the physical parameters of the capacitor itself. We can see experimentally that the capacitance is directly proportional to the area of the plates of the capacitor, it is inversely proportional to the distance between the plates, and depends on the type of dielectric in between the plates. The type of dielectric is identified in the formula by the Greek letter ε (epsilon). Each type of dielectric has its own value of ε (permittivity), which is the product of the vacuum permittivity and the relative permittivity of the material.

capacitance

For more information on this subject, please look also to the corresponding video on my YouTube channel.

Looking At The Future

An overview of the next subjects I will explore in my blog and my YouTube channel.

spatiul-cosmic

No, not the future of the human race! Not even the future of the space exploration!

I’m just talking about my plans for future posts on this blog and on my YouTube channel.

I observed that people tend to look mostly at short videos and, when they are too long, watchers soon give up. I attribute this to the fact that people watches YouTube videos in a different way than TV shows and, while TV shows may be long, that is not true for the majority of videos on YouTube. The expectations are just different.

So, rather than proposing long videos that exhaust a subject in all its details, and just gliding over it, it is probably better to have short videos that concentrate on a single detail of the subject. Then I could have several episodes on the same subject, each concentrating on a different detail and made in such a way that someone could watch a specific episode without the need to watch all the previous ones..

Looking back at the resistors video, it could have probably worked better if I had split the video in several pieces, one with the general information, one just for resistors in series, one for resistors in parallel, and so forth.

I could basically have several episodes on different aspects of the same subject!

Based on this assumption, I will publish in the next few weeks several episodes centered on two primary subjects: the capacitor and the inductor, to complete the overview of all the passive components used in electronics. And, maybe, in a later future, I could also provide a number of videos where I show how these components can be used together, and what kind of circuits can be created.

Please let me know what you think of this new setup of my channel by writing a comment. Should I just keep going the way I started? Or should I move on with shorter videos, centered on specific details of a subject? Would this help those people that are only interested in specific details and don’t want to listen to the whole spiel?

Before I go, I would like to finish by introducing a new subject that is very dear to me: I plan to build a functioning Theremin for myself (I play musical instruments as a hobby). It is going to be a complex project, so it wll take some time, but I plan to upload several videos on the progresses I make, until the project is completed. I will also publish the whole design of the instrument, so brave followers can try to build one for themselves too. And, maybe, I could also upload my own performance with the instrument, once completed, playing just some simple tune. Anyone interested?

theremin_in_concert

‘Till the next time…

(Watch also the video on YouTube:  https://www.youtube.com/watch?v=jXCCT2xIWcA&feature=share)