## Inductors Basics

Describing basic functionality of the inductors and how they are treated when connected in series or in parallel.

What is an inductor? How does it work? And how we handle inductors when they are connected in series or in parallel? Here are the answers.

An inductor is an electric device capable of storing energy in the form of a magnetic or electromagnetic field.

In its basic form, an inductor can be made of a single loop of wire, or several loops (solenoid). These loops can be arranged in air or on a ferromagnetic core.

When an inductor is connected to a battery, a current starts flowing in the circuit. The current that flows inside the inductor generates a magnetic field, like the one that would be generated by an actual magnet. This field stores an amount of energy, the same way an electric field does.

If the battery is suddenly disconnected, the energy that was accumulated in the inductor must be somehow released. but the energy cannot be released instantaneously, it needs to be released a little bit at a time. And since the energy depends on the current flowing in the inductor, the inductor tries to keep the it running, even if the battery is no more connected. To do so, it uses the energy stored into the magnetic field to generate a voltage at its terminals to keep the current going.

However, since the inductor is now connected nowhere, current cannot flow, unless the voltage is so high that the current can flow in the thin air. And that is exactly what happens: the voltage increases so much that there is a sudden discharge of current through the air, in the form of a spark, that dissipates all the energy that was stored in the inductor. This spark is the one you may sometimes notice when opening a switch that is powering a lamp or a motor, or when you pull the plug from a device that was working using a considerable amount of current.

Similarly to the case where the current is suddenly removed, an inductor generates a voltage also when the current is just changed in intensity. In this case, the voltage is created to react to the change in current, trying to keep it to the same value, so the energy can be conserved.

In both cases, the amount of voltage is proportional to the change in current (ΔI) and inversely proportional to the amount of time in which the current changes (Δt). In other words, the faster the current change, the higher is the voltage.

For a specific inductor, the ratio between the change of current and the interval in which that happens equals the voltage generated by the inductor divided by a constant that depends on the physics dimensions of the inductor. Such constant is called inductance, represented with the letter L, and can be calculated with the following experimental formula: where:

μ = permeability of the material inside the coil

N = number of turns making the coil

A = area of the cross section of the coil

l = length of the coil

L is measured in Henry.

μ is the product of the permeability of the void (or air) and the relative permeability of the material: The voltage at the terminals of the inductor is therefore calculated as: We can now calculate the energy stored in the magnetic field of an inductor as the integral of the power, which is obtained multiplying the voltage at the inductor and the current that flows through it: which, considering the value of the voltage previously calculated, can be solved as follows: where I is the current flowing through the inductor at the time the energy is calculated.

When choosing an inductor for a circuit, the following parameters must be considered:

• the value of the inductance in Henry

• the max current the inductor can sustain; failure to specify that could cause the inductor to overheat, since the wire could be too thin to deal with the required current;

• the max voltage that can be applied to the inductor; an excessive voltage on the inductor could cause sparks due to insufficient insulation of the wire.

## Inductors In Series

Let’s consider a series of inductors of different inductance values and let’s calculate the equivalent inductance. All the inductors, being in series, are traversed by the same current. And since each inductor has its own inductance value, each one will store a different amount of energy: The total energy stored in the inductors is therefore: So, the equivalent inductance is clearly: which we can generalize as: ## Inductors In Parallel

In the case of inductors in parallel, they are all subject to the same voltage and are traversed by a different current:  From these equations we can find the currents by integration: The total amount of current is therefore: So we can say that the equivalent inductance of a parallel of inductors can be determined through the formula: or, more in general: All the formulas presented here are very general and can be applied to both DC and AC circuits. Note, however, that since AC circuits have a variable voltage and current, the application of the formulas in AC is a little more challenging then in DC. But this is a story for another time.

## Looking At The Future

An overview of the next subjects I will explore in my blog and my YouTube channel. 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? ‘Till the next time…