WEBVTT - TechStuff Classic: The Basic Components of Electronics

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<v Speaker 1>Welcome to tex Stuff, a production from I Heart Radio.

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<v Speaker 1>Hey there, and welcome to tech Stuff. I'm your host

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<v Speaker 1>job and Strickland. I'mond executive producer with I Heart Radio

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<v Speaker 1>and how the tech area. It is time for a

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<v Speaker 1>classic episode of tech Stuff. This episode originally published on

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<v Speaker 1>June two thousand fifteen. It is titled The Basic Components

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<v Speaker 1>of Electronics. I bet you'll never guess what it's about.

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<v Speaker 1>Don't be alarmed. I'm going in medias race. This is

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<v Speaker 1>the middle of the email here or really the end. Lastly,

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<v Speaker 1>I was hoping in the future to see topics covered

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<v Speaker 1>like how electronics work, transistors, capascitors, chips, etcetera. I worked

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<v Speaker 1>at Radio Shack for five years and got really interested

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<v Speaker 1>in electronic components, but found them pretty confusing. That is

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<v Speaker 1>perfectly understandable. I still have to look up the various

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<v Speaker 1>components and remind myself what each one does, because I

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<v Speaker 1>don't tend to work with electronic circuits that frequently, and

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<v Speaker 1>I know in general what needs to happen, but sometimes

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<v Speaker 1>I forget the specifics because there's a lot of stuff there,

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<v Speaker 1>and if you aren't familiar, if you're not always working

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<v Speaker 1>in that world, it can very easily slip away from you.

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<v Speaker 1>And we are talking about lots of different components that

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<v Speaker 1>you measure using different units, And after a while you

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<v Speaker 1>just start to you know, if you again, if you're

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<v Speaker 1>not just naturally inclined to this kind of stuff, you

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<v Speaker 1>start to pull your hair out. Except in my case

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<v Speaker 1>that's already been done for me, so I just kind

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<v Speaker 1>of rubbed my head. So let's start with the basics.

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<v Speaker 1>And I know this is going to sound incredibly basic,

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<v Speaker 1>but we have to build a foundation before we can

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<v Speaker 1>start talking about the components. So electronics are all about

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<v Speaker 1>leveraging electricity. Not a big surprise, you're you're leveraging electricity

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<v Speaker 1>in order to do something to accomplis something like a

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<v Speaker 1>radio is meant to receive and amplify radio signals and

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<v Speaker 1>and convert them into acoustic signals so that you can

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<v Speaker 1>actually hear them. That that's a simple example. A flashlight

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<v Speaker 1>is meant to channel electricity to end up powering a

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<v Speaker 1>light bulb, which is essentially a resistor. We will talk

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<v Speaker 1>about those that heats up. We're talking about a basic

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<v Speaker 1>incandescent light bulb here um and gives off light as

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<v Speaker 1>a result. That's your basic use of that kind of electronics.

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<v Speaker 1>So we're gonna talk about how electronics control electricity. These

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<v Speaker 1>basic components are all used to do that so that

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<v Speaker 1>you can accomplish whatever the goal of your electronic device is. Now,

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<v Speaker 1>most electronic devices have lots and lots of different components

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<v Speaker 1>to them, sometimes worked in various configurations, whether they're in

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<v Speaker 1>series or in parallel. I'm not going to get into

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<v Speaker 1>all of that because that's be on what I really

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<v Speaker 1>wanted to focus on in this episode. Instead, in this episode,

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<v Speaker 1>I want to talk about the very basic components and

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<v Speaker 1>what they are intended to do. These are the things

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<v Speaker 1>that make up the circuits that you would see in

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<v Speaker 1>physical circuitry. So if you ever have, uh, you know,

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<v Speaker 1>an old electronic device and you were to take it

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<v Speaker 1>apart and you saw all these little weird do dads

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<v Speaker 1>on a circuit board, I'm gonna tell you what those

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<v Speaker 1>do dads do. Dad. Alright, So first we describe an

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<v Speaker 1>electronics materials is having electrons that fall into certain energy

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<v Speaker 1>bands or electronic bands. Now, the two important ones that

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<v Speaker 1>to talk about are the valence band and the conduction band.

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<v Speaker 1>Electrons and the conduction band are able to move freely

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<v Speaker 1>through the material in question. Assuming the conduction band isn't

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<v Speaker 1>totally full, you can think of it kind of like

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<v Speaker 1>a think of it like a nightclub. It's a nightclub

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<v Speaker 1>that's maybe you know, full, so you can still move

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<v Speaker 1>through it freely. Now that nightclubs packed, you're not going anywhere,

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<v Speaker 1>so there has to be you know, almost but not

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<v Speaker 1>quite full for you to be able to move around.

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<v Speaker 1>That's the conduction band. That's the basics of electrical conductivity. UH.

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<v Speaker 1>Whereas the valance band is kind of this um this

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<v Speaker 1>this basic energy level, and there is a gap between

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<v Speaker 1>the valence band and the conduction band. UH. It is

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<v Speaker 1>called the band gap. And depending upon the material, that

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<v Speaker 1>band gap will be of a certain size, and in

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<v Speaker 1>some cases the gap is insurmountable. You cannot get electrons

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<v Speaker 1>from the valence band into the conductance band, and you

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<v Speaker 1>cannot get them to flow, at least not under normal

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<v Speaker 1>operating circumstances. So in that sense, think of you've got

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<v Speaker 1>a like a holding room before you can get into

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<v Speaker 1>the nightclub, and the the doorway going into the nightclub

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<v Speaker 1>has got a big old bouncer, and that big old

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<v Speaker 1>bouncers not letting anyone through that's your band gap. You

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<v Speaker 1>cannot there's no one even collectively, all of you working together,

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<v Speaker 1>you're not gonna be able to budge that bouncer. That

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<v Speaker 1>would be as if you were in a non conducting

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<v Speaker 1>material and I'll get into more of that later. Whereas

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<v Speaker 1>if you're in a room where there's a wide open

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<v Speaker 1>door and you're allowed to go through as long as

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<v Speaker 1>someone else is coming in, that would mean that you

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<v Speaker 1>could flow through properly. You've got you got electrical electrical

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<v Speaker 1>conductivity going on there, and I'll talk more about that

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<v Speaker 1>in a second. I realized this analogy isn't perfect, but

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<v Speaker 1>I'm just trying to simplify things for those who haven't

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<v Speaker 1>really taken this kind of class in physics. So a

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<v Speaker 1>large gap would represent a great deal of energy needed

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<v Speaker 1>to move electrons from the valence band to the conductance band,

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<v Speaker 1>and sometimes that gap is so large as to be

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<v Speaker 1>impossible to cross again under normal operating conditions. So let's

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<v Speaker 1>look at the basic materials that we talk about in electronics, conductors, insulators,

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<v Speaker 1>and semiconductors. Pretty simple to understand. Conductors have high electrical conductivity.

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<v Speaker 1>That means they facilitate the flow of electrons uh. They

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<v Speaker 1>have a nearly full but not completely full conduction band.

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<v Speaker 1>Electrons can move freely through this material in response to

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<v Speaker 1>an electric field applied to that material. So you apply

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<v Speaker 1>an electrical field to this material, it will then allow

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<v Speaker 1>electrons to flow through freely. This is the stuff that

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<v Speaker 1>moves electrons from point A to point B. You apply

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<v Speaker 1>a voltage across it, you get electrons to flow. That's current,

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<v Speaker 1>Although technically current flows from positive to negative as opposed

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<v Speaker 1>to the flow of electrons, which is from negative to positive.

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<v Speaker 1>We can thank lots of early thinkers for that confusion.

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<v Speaker 1>So current flow and electron flow are in opposite directions,

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<v Speaker 1>Thank you, Benjamin Franklin. Uh. Alright, So then you've got insulators.

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<v Speaker 1>These do not have electrons within the conduction band, or

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<v Speaker 1>they have a full conduction band, so again no room

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<v Speaker 1>for electrons to move around, so there are no free electrons.

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<v Speaker 1>They impede the flow of electrons through that material, and

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<v Speaker 1>most solids fall into this category. Metals are uh an exception,

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<v Speaker 1>but most solids are insulators. So at normal operating parameters,

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<v Speaker 1>you wouldn't be able to apply a strong enough electric

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<v Speaker 1>field to make them conduct electricity. So you could apply

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<v Speaker 1>an electric field to these things, but it wouldn't be

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<v Speaker 1>able to jump that gap between the valence band and

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<v Speaker 1>the conductance band, so it would just stop. You wouldn't

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<v Speaker 1>have any electrical flow through that at all. So we

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<v Speaker 1>use insulators for things like insulation on wires where we

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<v Speaker 1>wrapped the wires in that to help prevent leakage or interference, because,

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<v Speaker 1>as we've talked about many times on this show, the

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<v Speaker 1>flow of electricity is also very closely related to magnetism

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<v Speaker 1>and vice versa. So you have to be able to

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<v Speaker 1>limit interference between different wires if you don't want there

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<v Speaker 1>to be that interaction obviously, otherwise you can end up

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<v Speaker 1>causing shorts, which is when you have an unintended connection

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<v Speaker 1>between two different elements of a circuit and it allows

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<v Speaker 1>electricity to pass from one to the other, almost like

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<v Speaker 1>you think of it like a short cut, you know,

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<v Speaker 1>when we say an electrical short and it means that

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<v Speaker 1>the device itself will not work properly because the electricity

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<v Speaker 1>is not flowing through the pathway you had intended it

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<v Speaker 1>to go in. All right, then we've got semiconductors, and

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<v Speaker 1>we'll talk more about them a little bit later, but

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<v Speaker 1>in general, semi conductors have an almost empty conduction band

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<v Speaker 1>and an almost full valence band, and the band gap

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<v Speaker 1>is relatively narrow, so if you don't apply a strong

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<v Speaker 1>enough electric field, it acts as an insulator. But when

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<v Speaker 1>you apply the right amount of energy and electric field,

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<v Speaker 1>it will allow electrons jump from the valence band to

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<v Speaker 1>the conductor band and move freely within the material. You

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<v Speaker 1>do this by doping the material, which is when you

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<v Speaker 1>insert impurities into the semiconductor on purpose. Doping a semiconductor,

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<v Speaker 1>which is all about introducing impurities specifically at at predetermined levels,

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<v Speaker 1>will determine the energy levels required to do this, and

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<v Speaker 1>that's the basis for solid state electronics. We'll get into

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<v Speaker 1>more about semiconductors towards the end of this. And we

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<v Speaker 1>also have to remember voltage and current, something that I

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<v Speaker 1>always have trouble remembering. So voltage is a lot like

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<v Speaker 1>water pressure, all right. That's that's the the amount of

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<v Speaker 1>electrical pressure being applied, and the higher the voltage, the

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<v Speaker 1>more electrons want to move from the concentration of electrons

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<v Speaker 1>to the more positive side. Now, the actual flow of

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<v Speaker 1>electricity is the current, so they are related but not

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<v Speaker 1>the same thing. So voltage and current, and then you

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<v Speaker 1>multiply those two de patent together and you get the power.

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<v Speaker 1>So voltage times current equals power. Alright, So those are

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<v Speaker 1>your basics. Now we're gonna go through and talk about

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<v Speaker 1>the very individual components and what they do. So first

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<v Speaker 1>we have resistors. Resistor does pretty much what it sounds like.

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<v Speaker 1>It does. It resists but does not halt the flow

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<v Speaker 1>of electricity. I'm gonna talk a lot about electricity in

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<v Speaker 1>terms of water because it is a useful analogy, and

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<v Speaker 1>it's also very common to talk about the similarities between

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<v Speaker 1>electricity flowing and water flowing when you're discussing these components.

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<v Speaker 1>So let's say that you have two different pipes. You've

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<v Speaker 1>got a brand spanking new pipe. It's shiny and beautiful

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<v Speaker 1>and free from any any irregularities, and it allows water

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<v Speaker 1>to flow through the minimum of resistance. That water is

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<v Speaker 1>just flowing right through easily. You've got a second, old,

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<v Speaker 1>gnarly pipe, and this one's got calcium build up in it.

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<v Speaker 1>They're all these bumps and stuff on the inside. So

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<v Speaker 1>water actually encounters resistance friction if you will, as it's

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<v Speaker 1>flowing through, and it does not flow through as easily.

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<v Speaker 1>Resistors are like that old gnarly pipe, and they are

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<v Speaker 1>invented on purpose for specific reasons. So why would you

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<v Speaker 1>want to have an electronic component that actually slows down

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<v Speaker 1>or impedes the flow of electricity for some reason. Well,

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<v Speaker 1>sometimes you have to limit the amount of electricity that

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<v Speaker 1>can flow through part of a circuit within a given

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<v Speaker 1>amount of time, sort of like how a faucet going

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<v Speaker 1>back to water, how fauce it can limit how much

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<v Speaker 1>water it can flow through your water pipes into your sink.

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<v Speaker 1>So you wouldn't want just an on off switch for

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<v Speaker 1>the water coming into your home. That water is at

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<v Speaker 1>a much higher pressure, know it's it's a higher pressure

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<v Speaker 1>to deliver the water to your house. And if all

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<v Speaker 1>you had wasn't on off switch and you flipped it,

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<v Speaker 1>you would have water blasting through the pipe according to

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<v Speaker 1>the amount of pressure that was built up behind it.

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<v Speaker 1>That'd be a little bit nerving, especially if you just

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<v Speaker 1>wanted to have a nice, frusty glass water. So you

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<v Speaker 1>want to have some sort of limiter on that to

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<v Speaker 1>control the amount of water that's or the pressure of

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<v Speaker 1>the water that's coming in. So resistors reduced the amount

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<v Speaker 1>of voltage placed on other electronic components within a circuit

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<v Speaker 1>by restricting the amount of current that can flow through

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<v Speaker 1>the resistor. The reason why this is important is that

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<v Speaker 1>we cannot create a battery for every single type of

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<v Speaker 1>electronic device that's out there. It's not practical. So batteries

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<v Speaker 1>different batteries. Different types of batteries have different voltages. So

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<v Speaker 1>you could, in theory, develop a battery specifically for a

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<v Speaker 1>particular type of electronic device that would not require resistors

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<v Speaker 1>because the battery is providing exactly the voltage needed for

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<v Speaker 1>whatever electronic components are in net. But it's not practical

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<v Speaker 1>to do that for everything. We want standardized batteries, and

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<v Speaker 1>then we use things like resistors to help control the

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<v Speaker 1>voltage in those electronic components so that the right amount

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<v Speaker 1>of voltage is applied to those specific parts of the

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<v Speaker 1>electronic circuit, rather than having to have a billion different

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<v Speaker 1>types of batteries. That would not be practical. So there

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<v Speaker 1>are many different types of resistors designed to work on

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<v Speaker 1>specific amounts of electrical power. Now, some have changeable resistor

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<v Speaker 1>values dependent upon the amount of voltage placed across them.

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<v Speaker 1>They're called nonlinear or voltage dependent resistors. Resistor values can

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<v Speaker 1>also change when the temperature of the resistor changes UH.

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<v Speaker 1>Different types of resistors do this. Some can also be

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<v Speaker 1>mechanically adjusted. So it all depends upon what you need

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<v Speaker 1>the resistor form. Why what you needed to do, that's

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<v Speaker 1>what would determine which type of resistor you would use.

0:14:11.000 --> 0:14:13.600
<v Speaker 1>The unit of measurement for a resistor is the ohm

0:14:14.440 --> 0:14:18.400
<v Speaker 1>oh h M. Resistor values are ten percent apart from

0:14:18.440 --> 0:14:22.080
<v Speaker 1>each other, and resistors are color coded with bands of

0:14:22.120 --> 0:14:24.880
<v Speaker 1>color or or rings of color. So the first ring

0:14:24.960 --> 0:14:28.440
<v Speaker 1>represents the first digit of the resistors value. So what

0:14:28.560 --> 0:14:30.160
<v Speaker 1>you would do is you would look at the first ring,

0:14:30.240 --> 0:14:33.040
<v Speaker 1>whatever color it was, you would cross reference that with

0:14:33.640 --> 0:14:38.000
<v Speaker 1>the with a color UH index, and we'll tell you

0:14:38.040 --> 0:14:41.080
<v Speaker 1>what the value of the resistor is for the first digit.

0:14:42.000 --> 0:14:44.640
<v Speaker 1>The second ring tells you the value of the second digit.

0:14:45.120 --> 0:14:48.000
<v Speaker 1>So then you've got the two the two digits that

0:14:48.040 --> 0:14:50.120
<v Speaker 1>are involved. The third tells you the power of ten

0:14:50.200 --> 0:14:54.960
<v Speaker 1>to multiply by, so it might be ten thousand, and

0:14:55.000 --> 0:14:58.200
<v Speaker 1>then you would multiply. Let's say that your first two

0:14:58.200 --> 0:15:00.960
<v Speaker 1>digits are a twenty two and seven, and you would

0:15:01.000 --> 0:15:03.440
<v Speaker 1>multiply that by ten thousand. You have twenty seven thousand homes.

0:15:03.480 --> 0:15:07.000
<v Speaker 1>There and the fourth ring would tell you the tolerance

0:15:07.080 --> 0:15:11.520
<v Speaker 1>of the resistor plus or minus whatever percentage. Uh. So

0:15:11.600 --> 0:15:14.000
<v Speaker 1>the physical size the resistor and the amount of power

0:15:14.040 --> 0:15:16.360
<v Speaker 1>it can handle tends to be proportional. So in other words,

0:15:16.400 --> 0:15:20.080
<v Speaker 1>the larger the resistor, the more power it can handle.

0:15:20.400 --> 0:15:24.920
<v Speaker 1>In general, So those are resistors covers that basic component.

0:15:25.200 --> 0:15:30.280
<v Speaker 1>Now let's move on to capacitors. Alright, So capacitors are

0:15:30.680 --> 0:15:33.760
<v Speaker 1>similar to batteries and that it's a means of storing

0:15:33.920 --> 0:15:40.080
<v Speaker 1>electrical energy, but unlike batteries, instead of creating an a uh,

0:15:40.400 --> 0:15:44.200
<v Speaker 1>electrical flow through a chemical reaction that is steady the

0:15:44.400 --> 0:15:48.960
<v Speaker 1>entire time, it is designed to release a it's it's

0:15:49.160 --> 0:15:55.600
<v Speaker 1>entire stored electrical charge all at once. So let's say

0:15:55.640 --> 0:15:58.680
<v Speaker 1>they've got two leads of a capacitor. You have a

0:15:58.720 --> 0:16:01.680
<v Speaker 1>difference in voltage across us these two leads. That's when

0:16:01.720 --> 0:16:05.240
<v Speaker 1>a capacitor is charged, So one lead has a greater

0:16:05.320 --> 0:16:09.160
<v Speaker 1>build up of electrons than the other lead does. Uh. Now,

0:16:09.200 --> 0:16:12.040
<v Speaker 1>if you were to connect the leads together, you would

0:16:12.040 --> 0:16:15.920
<v Speaker 1>short them. You would have a discharge of that capacitor,

0:16:16.080 --> 0:16:19.200
<v Speaker 1>and the voltage would equalize across the two, so you

0:16:19.240 --> 0:16:22.040
<v Speaker 1>get a release of a quick burst of electricity, so

0:16:22.120 --> 0:16:26.560
<v Speaker 1>capacitors can pass alternating current freely. A C current will

0:16:26.600 --> 0:16:28.880
<v Speaker 1>just pass through a capacitor as if it were not

0:16:29.040 --> 0:16:32.800
<v Speaker 1>really there. Direct current, however, will charge a capacitor. It

0:16:32.800 --> 0:16:36.800
<v Speaker 1>will have that build up of electrons on one side

0:16:37.200 --> 0:16:40.000
<v Speaker 1>while the other side doesn't get that build up of electrons,

0:16:40.040 --> 0:16:43.600
<v Speaker 1>and then you have that difference in voltage. Alternating current

0:16:43.640 --> 0:16:48.640
<v Speaker 1>just will pass back and forth through it without any problems.

0:16:48.640 --> 0:16:52.400
<v Speaker 1>So capacitors contain the same fundamental parts. You have at

0:16:52.480 --> 0:16:57.040
<v Speaker 1>least two conductive plates separated by a non conductive material

0:16:57.120 --> 0:17:00.680
<v Speaker 1>that's the dielectric. The amount of charge held a capacitor

0:17:00.760 --> 0:17:04.000
<v Speaker 1>is measured in units called faret's. But a faret is

0:17:04.119 --> 0:17:08.520
<v Speaker 1>a large amount of capacitance, so large that you don't

0:17:08.600 --> 0:17:12.119
<v Speaker 1>really talk about a ferret. Instead we end up talking

0:17:12.160 --> 0:17:16.000
<v Speaker 1>about micro ferrets, which are about a well, which are

0:17:16.160 --> 0:17:20.639
<v Speaker 1>one million of a ferret, so much smaller. Ferret, by

0:17:20.640 --> 0:17:25.720
<v Speaker 1>the way, not ferret, two different things. Nice Marmot capacitance

0:17:26.000 --> 0:17:29.919
<v Speaker 1>is dependent upon surface area, so it's directly proportional to

0:17:29.960 --> 0:17:33.119
<v Speaker 1>the surface area of those leads, those those capacity plates.

0:17:33.640 --> 0:17:38.040
<v Speaker 1>Um it is indirectly proportional to the distance between the

0:17:38.119 --> 0:17:41.119
<v Speaker 1>plates so the greater the distance between the plates, the

0:17:41.200 --> 0:17:46.760
<v Speaker 1>lower the capacitance. Uh. It's also uh dependent upon the

0:17:46.880 --> 0:17:51.760
<v Speaker 1>dielectric constant of the insulating material. And they are used

0:17:51.800 --> 0:17:54.479
<v Speaker 1>for things that need a quick release of electricity rather

0:17:54.560 --> 0:17:59.000
<v Speaker 1>than a steady flow. So for example, a traditional flash

0:17:59.119 --> 0:18:01.960
<v Speaker 1>on a camera. So you've got an old camera and

0:18:01.960 --> 0:18:05.160
<v Speaker 1>you've got the the the flash, Uh, you know it

0:18:05.200 --> 0:18:07.560
<v Speaker 1>bursts in this quick burst of light. Will It needs

0:18:07.640 --> 0:18:10.560
<v Speaker 1>that quick It needs access to a quick burst of

0:18:10.720 --> 0:18:14.240
<v Speaker 1>electricity in order to do that, and that's what capacitors

0:18:14.240 --> 0:18:16.440
<v Speaker 1>are good for. And it takes some time for the

0:18:16.480 --> 0:18:18.719
<v Speaker 1>capacitors to build up the charge again so it can

0:18:18.760 --> 0:18:21.080
<v Speaker 1>do it another time. That's sort of you know, if

0:18:21.119 --> 0:18:25.000
<v Speaker 1>you're using the old ones, you hear that noise. It's

0:18:25.040 --> 0:18:28.800
<v Speaker 1>the the discharge and then charging of the capacitors that

0:18:29.000 --> 0:18:32.600
<v Speaker 1>require you to take a moment between taking pictures with

0:18:32.680 --> 0:18:38.159
<v Speaker 1>those old style camera flashes. Now, obviously newer ones use

0:18:38.240 --> 0:18:41.760
<v Speaker 1>different a different approach, but you often have capacitors that

0:18:41.840 --> 0:18:46.159
<v Speaker 1>actually provide the electricity for those Now, the voltage of

0:18:46.160 --> 0:18:51.359
<v Speaker 1>a capacitor cannot change instantly, it's important to remember, and

0:18:51.560 --> 0:18:56.720
<v Speaker 1>quick voltage changes in a capacitor produced large current changes.

0:18:57.080 --> 0:19:01.200
<v Speaker 1>Capacitor store energy in an electric field. The reason I

0:19:01.240 --> 0:19:03.600
<v Speaker 1>mentioned all that is because we're now going to talk

0:19:03.880 --> 0:19:09.760
<v Speaker 1>about inductors, and inductors are kind of, um, the opposite

0:19:10.200 --> 0:19:12.919
<v Speaker 1>of capacitors, or really maybe not even opposite is the

0:19:13.000 --> 0:19:15.880
<v Speaker 1>right way of saying it. In many ways that they

0:19:15.920 --> 0:19:19.000
<v Speaker 1>behave in opposite ways than capacitors do. But we'll get

0:19:19.040 --> 0:19:22.120
<v Speaker 1>to that. We'll be back with more of this classic

0:19:22.160 --> 0:19:36.879
<v Speaker 1>episode of tech stuff after this quick break. So basically,

0:19:36.920 --> 0:19:40.639
<v Speaker 1>an inductor at its most basic level is a coil

0:19:40.680 --> 0:19:43.159
<v Speaker 1>of wires, so sometimes we just call them coils and

0:19:43.280 --> 0:19:48.119
<v Speaker 1>not inductors. Uh. They deal with what is the electrical

0:19:48.200 --> 0:19:54.119
<v Speaker 1>equivalent of momentum. So if you're familiar with momentum, essentially,

0:19:54.240 --> 0:19:56.919
<v Speaker 1>this is that idea that you get a you know,

0:19:57.000 --> 0:19:59.400
<v Speaker 1>objects in motion tend to stay in motion. So let's

0:19:59.440 --> 0:20:04.320
<v Speaker 1>say you've got a large mass moving at a particular velocity.

0:20:04.440 --> 0:20:06.800
<v Speaker 1>It has a certain amount of momentum and you have

0:20:06.840 --> 0:20:10.879
<v Speaker 1>to overcome that momentum to slow down and stop that uh,

0:20:10.880 --> 0:20:14.040
<v Speaker 1>that that mass. So it's the same type of thing

0:20:14.119 --> 0:20:17.920
<v Speaker 1>with inductors, except we're talking about the electrical equivalent of momentum.

0:20:17.920 --> 0:20:22.040
<v Speaker 1>We're talking about the flow of electricity. So again going

0:20:22.040 --> 0:20:25.240
<v Speaker 1>back to the water analogy, Let's say that you've got

0:20:25.280 --> 0:20:28.840
<v Speaker 1>a water hose, a really long one, several hundred feet long,

0:20:29.000 --> 0:20:32.400
<v Speaker 1>and you've coiled it up so it's in a nice

0:20:32.480 --> 0:20:36.280
<v Speaker 1>long coil and it's filled with water. There are gallons

0:20:36.480 --> 0:20:39.560
<v Speaker 1>of water inside this hose, and the end of the

0:20:39.600 --> 0:20:41.680
<v Speaker 1>hose is tilted at such an angle so the water

0:20:41.760 --> 0:20:44.440
<v Speaker 1>is not just flowing right out. You put a plunger

0:20:44.480 --> 0:20:47.679
<v Speaker 1>into the other end and you start to press on

0:20:47.760 --> 0:20:51.000
<v Speaker 1>the plunger to push the water out. Now, all of

0:20:51.000 --> 0:20:54.000
<v Speaker 1>that water is not just going to simultaneously start to

0:20:54.119 --> 0:20:56.800
<v Speaker 1>move together. It actually is going to take some time

0:20:57.440 --> 0:21:01.080
<v Speaker 1>for the pressure you are applying to exert enough force

0:21:01.200 --> 0:21:05.240
<v Speaker 1>to push the water out to overcome the inertia within

0:21:05.480 --> 0:21:09.159
<v Speaker 1>that coil of water hose. And once you get that

0:21:09.200 --> 0:21:12.040
<v Speaker 1>water coming out at the speed at which it can

0:21:12.160 --> 0:21:13.920
<v Speaker 1>come out and you let go of the plunger, the

0:21:13.920 --> 0:21:17.840
<v Speaker 1>plunger is going to continue going down that tube because

0:21:17.920 --> 0:21:21.080
<v Speaker 1>of inertia. That's the same sort of thing with inductors,

0:21:21.080 --> 0:21:24.680
<v Speaker 1>except instead of water, we're talking about electricity. So coils

0:21:24.720 --> 0:21:28.199
<v Speaker 1>of wire will pass D C current but will block

0:21:28.520 --> 0:21:31.160
<v Speaker 1>a C current. So in other words, direct current can

0:21:31.240 --> 0:21:36.160
<v Speaker 1>flow through an inductor, but alternating current would be blocked

0:21:36.200 --> 0:21:39.080
<v Speaker 1>because it cannot flow the opposite way through the coil.

0:21:39.800 --> 0:21:43.760
<v Speaker 1>So that makes it the opposite of capacitors. Remember, capacitors

0:21:43.760 --> 0:21:47.240
<v Speaker 1>would pass alternating current that can flow straight through, but

0:21:47.320 --> 0:21:50.480
<v Speaker 1>would block direct current. Direct current would charge a capacitor

0:21:50.520 --> 0:21:52.960
<v Speaker 1>a capacitor, but could not just flow through the capacitor.

0:21:53.320 --> 0:21:56.600
<v Speaker 1>In this case, direct current can flow through an inductor,

0:21:56.680 --> 0:22:00.719
<v Speaker 1>but a c altering current would be blocked. The standard

0:22:00.840 --> 0:22:05.520
<v Speaker 1>unit of inductance is the henry. I wish I could

0:22:05.520 --> 0:22:08.120
<v Speaker 1>tell you why, but I honestly don't know. I'm sure

0:22:08.160 --> 0:22:11.280
<v Speaker 1>some of you out there, you electricians, are very familiar

0:22:11.280 --> 0:22:14.040
<v Speaker 1>with the reason why and could tell me and feel

0:22:14.080 --> 0:22:17.200
<v Speaker 1>free to I I honestly do not off hand. No,

0:22:17.920 --> 0:22:21.240
<v Speaker 1>the inductance of a coil is indirectly proportional to the

0:22:21.359 --> 0:22:25.080
<v Speaker 1>length of the coil, but directly proportional to the cross

0:22:25.200 --> 0:22:29.000
<v Speaker 1>sectional area of the wire, So, in other words, the

0:22:29.040 --> 0:22:32.040
<v Speaker 1>gauge of the wire is important here. It's also proportional

0:22:32.080 --> 0:22:35.000
<v Speaker 1>to the square of the number of turns in the coil,

0:22:35.480 --> 0:22:39.320
<v Speaker 1>and it's directly proportional to the permeability of the core material. Now,

0:22:39.320 --> 0:22:42.560
<v Speaker 1>the core is whatever this coil is wrapped around. Now

0:22:42.560 --> 0:22:44.840
<v Speaker 1>it could be wrapped around air, or it could be

0:22:44.840 --> 0:22:48.760
<v Speaker 1>wrapped around something like iron, which is incredibly effective. So

0:22:49.200 --> 0:22:51.320
<v Speaker 1>those are that's what we're talking about with the cords,

0:22:51.400 --> 0:22:56.399
<v Speaker 1>whatever the wire or is coiled around. So when current

0:22:56.520 --> 0:22:59.560
<v Speaker 1>first starts flowing into the coil, the coil wants to

0:22:59.600 --> 0:23:03.280
<v Speaker 1>build up a magnetic field. We talked about this again

0:23:03.320 --> 0:23:08.439
<v Speaker 1>and again that you start running electricity through a coil

0:23:08.520 --> 0:23:12.439
<v Speaker 1>of wire that's coiled around like an iron core, like

0:23:12.480 --> 0:23:16.800
<v Speaker 1>a nail, and you start to you create an electro magnet. Well,

0:23:16.880 --> 0:23:20.320
<v Speaker 1>once that field is built. While while the magnetic field

0:23:20.359 --> 0:23:22.840
<v Speaker 1>is building, the coil inhibits the flow of current through

0:23:23.040 --> 0:23:26.440
<v Speaker 1>the wire, But once the field is built, current can

0:23:26.480 --> 0:23:30.280
<v Speaker 1>flow normally through the wire. So if you were to

0:23:30.720 --> 0:23:34.360
<v Speaker 1>have an inductor hooked up to a light bulb, let's

0:23:34.359 --> 0:23:37.840
<v Speaker 1>say and you flip a switch so that you know,

0:23:37.920 --> 0:23:40.720
<v Speaker 1>technically in an electronics we'd say that you close the switch,

0:23:40.760 --> 0:23:43.440
<v Speaker 1>so you have created a closed path so electrons can

0:23:43.440 --> 0:23:46.760
<v Speaker 1>flow through. The electrons would flow through the inductor, which

0:23:46.800 --> 0:23:49.560
<v Speaker 1>would start to build up a magnetic field. So at

0:23:49.600 --> 0:23:52.320
<v Speaker 1>first you would get the light bulb coming on. Then

0:23:52.320 --> 0:23:54.520
<v Speaker 1>it would start to dim a bit because as that

0:23:54.600 --> 0:23:58.720
<v Speaker 1>magnetic field is getting built up the lightbulb, you know,

0:23:58.760 --> 0:24:01.080
<v Speaker 1>the electricity would be it did to the light bulb,

0:24:01.080 --> 0:24:03.720
<v Speaker 1>it would actually act as sort of a resistor, and

0:24:03.760 --> 0:24:06.120
<v Speaker 1>the light bul would start to get dimmer. But then

0:24:06.160 --> 0:24:09.360
<v Speaker 1>eventually that that magnetic field would get charged up as

0:24:09.440 --> 0:24:12.919
<v Speaker 1>much as it can because it's direct current, not alternating current,

0:24:13.600 --> 0:24:16.560
<v Speaker 1>and you would reach a level where it was stabilized.

0:24:16.680 --> 0:24:20.439
<v Speaker 1>Current would flow fine. At that point, you could actually

0:24:20.480 --> 0:24:25.639
<v Speaker 1>turn off the switch, you can open it. In other words,

0:24:26.160 --> 0:24:29.440
<v Speaker 1>the magnetic field around the coil would keep current flowing

0:24:29.480 --> 0:24:33.240
<v Speaker 1>through the coil until that magnetic field collapsed. So even

0:24:33.240 --> 0:24:36.560
<v Speaker 1>though you turn the switch to off, because you have

0:24:36.600 --> 0:24:40.280
<v Speaker 1>an inductor, that light bulb would stay lit until the

0:24:40.280 --> 0:24:43.359
<v Speaker 1>magnetic field and the inductor collapsed, in which case it

0:24:43.400 --> 0:24:46.840
<v Speaker 1>would stop inducing current to flow through and the light

0:24:46.840 --> 0:24:50.760
<v Speaker 1>bulb would go off. So the experience you would have

0:24:50.960 --> 0:24:54.520
<v Speaker 1>is turn the switch on, light bulb comes on, light

0:24:54.560 --> 0:24:57.840
<v Speaker 1>bulb starts to get dim, light bulb gets bright again,

0:24:58.080 --> 0:25:00.439
<v Speaker 1>You turn the switch off, light bulb stays lit for

0:25:00.480 --> 0:25:02.960
<v Speaker 1>a while, and then turns off. That's what it would

0:25:03.000 --> 0:25:08.159
<v Speaker 1>look like to you, So pretty interesting to me now. So,

0:25:08.200 --> 0:25:11.679
<v Speaker 1>an inductor stores energy in its magnetic field, and it

0:25:11.720 --> 0:25:14.440
<v Speaker 1>tends to resist any change in the amount of current

0:25:14.640 --> 0:25:18.480
<v Speaker 1>flowing through it, thus making it different from capacitors. Because

0:25:18.480 --> 0:25:23.520
<v Speaker 1>capacitors store things an electric field, inductor store things energy,

0:25:23.800 --> 0:25:27.040
<v Speaker 1>not just things. Capacitor store energy and electric fields, and

0:25:27.240 --> 0:25:32.560
<v Speaker 1>inductor store energy and magnetic fields. And capacitors resist changes

0:25:32.680 --> 0:25:37.720
<v Speaker 1>to voltage, whereas inductors resist changes to current. So really

0:25:37.760 --> 0:25:41.639
<v Speaker 1>interesting about that. We've got more to say in this

0:25:41.800 --> 0:25:52.879
<v Speaker 1>classic episode of tech stuff after these quick messages. So

0:25:52.960 --> 0:25:57.440
<v Speaker 1>because of this relationship between inductors and capacitors, these two

0:25:57.520 --> 0:26:02.119
<v Speaker 1>different components are sometimes referred together as duel components because

0:26:02.119 --> 0:26:06.320
<v Speaker 1>they they are opposites that complement one another. The current

0:26:06.400 --> 0:26:09.479
<v Speaker 1>in an inductor cannot change instantly the quick current changes

0:26:09.520 --> 0:26:12.560
<v Speaker 1>produced the large voltage, and inductors store their energy in

0:26:12.560 --> 0:26:16.400
<v Speaker 1>those magnetic fields. That's what sets them opposite of capacitors,

0:26:16.400 --> 0:26:19.600
<v Speaker 1>because they are all the opposite of those things. And

0:26:19.640 --> 0:26:21.760
<v Speaker 1>you might wonder, well, what are inductors used for. I mean,

0:26:21.760 --> 0:26:25.280
<v Speaker 1>that light bulb example seems kind of crazy. Well, they're

0:26:25.600 --> 0:26:27.400
<v Speaker 1>used for lots of stuff. For example, if you've ever

0:26:27.440 --> 0:26:31.280
<v Speaker 1>gone to uh, like traffic lights, that are the respond

0:26:31.320 --> 0:26:35.040
<v Speaker 1>to the presence of vehicles. Most of those are using inductors.

0:26:35.080 --> 0:26:38.719
<v Speaker 1>So underneath the pavement where you're driving on top of

0:26:39.000 --> 0:26:43.800
<v Speaker 1>you know, there are giant coils of wire, and when

0:26:43.880 --> 0:26:47.240
<v Speaker 1>you stop your car at a stoplight that has one

0:26:47.240 --> 0:26:50.640
<v Speaker 1>of these systems, your car starts to act as the

0:26:50.680 --> 0:26:53.679
<v Speaker 1>core for that inductor loop. You've got this massive amount

0:26:53.680 --> 0:26:58.119
<v Speaker 1>of steel that's right there that affects the inductance of

0:26:58.160 --> 0:27:01.159
<v Speaker 1>the that cable. You of a meter attached to the

0:27:01.160 --> 0:27:05.000
<v Speaker 1>cable that measures the inductance. So when it measures a

0:27:05.160 --> 0:27:09.640
<v Speaker 1>change in inductance, that meter knows there's a vehicle at

0:27:09.680 --> 0:27:13.960
<v Speaker 1>that location and sends that information to the control unit

0:27:14.040 --> 0:27:17.919
<v Speaker 1>for the traffic system and thus changes the traffic cycle

0:27:18.040 --> 0:27:20.919
<v Speaker 1>so that you get a green light faster. So if

0:27:20.960 --> 0:27:24.639
<v Speaker 1>you're ever at one of those intersections where the the

0:27:24.760 --> 0:27:28.200
<v Speaker 1>light cycles depend heavily upon whether or not their cars

0:27:28.280 --> 0:27:33.040
<v Speaker 1>present at the intersection, that's generally speaking, what is happening.

0:27:33.040 --> 0:27:36.159
<v Speaker 1>You've got these inductors. The inductance changes, sends the message

0:27:36.160 --> 0:27:39.320
<v Speaker 1>to the meter, or rather the meter detects the inductor

0:27:39.320 --> 0:27:42.080
<v Speaker 1>the change in inductance and then sends that onto the

0:27:42.119 --> 0:27:46.200
<v Speaker 1>traffic control system. That will then, at least in theory,

0:27:46.600 --> 0:27:50.439
<v Speaker 1>gets you on your way a little faster. So that's inductors.

0:27:52.080 --> 0:27:56.120
<v Speaker 1>Now let's take a look at transformers, which are more

0:27:56.160 --> 0:27:59.320
<v Speaker 1>than meets the eye. So I'm not talking about autobots

0:27:59.359 --> 0:28:02.160
<v Speaker 1>in Decepticon, as much as I would love to do that,

0:28:02.359 --> 0:28:06.040
<v Speaker 1>instead of talking about the basic electronic component. So let's

0:28:06.080 --> 0:28:10.000
<v Speaker 1>say you've got a single core, like like that iron nail.

0:28:10.280 --> 0:28:15.120
<v Speaker 1>Let's say and you put multiple coils of wire over

0:28:15.160 --> 0:28:18.639
<v Speaker 1>this same iron core, and then you force a DC

0:28:18.800 --> 0:28:21.880
<v Speaker 1>current through one of those coils of wire, not all

0:28:21.920 --> 0:28:25.399
<v Speaker 1>of them, just one. Now, as that current charges, it

0:28:25.440 --> 0:28:28.479
<v Speaker 1>will induce current to flow through the other coils wrapped

0:28:28.480 --> 0:28:32.639
<v Speaker 1>around that same core, and constantly changing the voltage of

0:28:32.680 --> 0:28:35.879
<v Speaker 1>that primary coil. The one that you've got attached to

0:28:35.920 --> 0:28:40.000
<v Speaker 1>some sort of voltage generator, will cause currents that change

0:28:40.040 --> 0:28:43.600
<v Speaker 1>in a similar fashion in the other coils. Now, if

0:28:43.640 --> 0:28:46.400
<v Speaker 1>the other coils have more loops than the primary coil,

0:28:46.720 --> 0:28:50.240
<v Speaker 1>the voltage will be greater, but the current will be lower.

0:28:50.360 --> 0:28:52.240
<v Speaker 1>I'll explain that in a second. So let's say we've

0:28:52.280 --> 0:28:54.760
<v Speaker 1>got we'll make it really simple. We'll just do two coils.

0:28:55.560 --> 0:28:58.160
<v Speaker 1>Let say we've got an iron core and we've got

0:28:58.240 --> 0:29:02.200
<v Speaker 1>a primary wire coiled a fund it ten times, and

0:29:02.240 --> 0:29:04.920
<v Speaker 1>we have a second wire coiled in the same direction

0:29:05.000 --> 0:29:08.560
<v Speaker 1>around that iron core, but it is coiled twenty times,

0:29:09.120 --> 0:29:12.760
<v Speaker 1>and we apply a varying voltage across the primary wire.

0:29:13.240 --> 0:29:15.560
<v Speaker 1>The voltage across the second wire will be twice as

0:29:15.640 --> 0:29:19.160
<v Speaker 1>much because there are twice as many coils, but the

0:29:19.240 --> 0:29:21.840
<v Speaker 1>current will be half as much as that in the

0:29:21.880 --> 0:29:25.680
<v Speaker 1>primary coil. And that's because you have to conserve power.

0:29:26.200 --> 0:29:29.120
<v Speaker 1>You cannot create or destroy power. You have to conserve it.

0:29:29.440 --> 0:29:32.600
<v Speaker 1>And power, like I said earlier, is equal to voltage

0:29:32.600 --> 0:29:36.480
<v Speaker 1>times current. So if we double the voltage, but ultimately

0:29:36.520 --> 0:29:38.800
<v Speaker 1>the power in the secondary coil has to be the

0:29:38.840 --> 0:29:41.680
<v Speaker 1>same as the primary coil, and the only way to

0:29:42.080 --> 0:29:46.520
<v Speaker 1>address that is to have the current. So that's you know,

0:29:46.600 --> 0:29:50.680
<v Speaker 1>that's what happens. So if the second coil is coiled

0:29:50.680 --> 0:29:52.720
<v Speaker 1>in the same direction as the primary, like I was

0:29:52.760 --> 0:29:56.520
<v Speaker 1>saying before, the voltage is in the same polarity as

0:29:56.560 --> 0:30:00.720
<v Speaker 1>that of the generator the primary coil. If second coil

0:30:00.840 --> 0:30:04.120
<v Speaker 1>is coiled in the opposite direction of the primary coil,

0:30:04.680 --> 0:30:08.000
<v Speaker 1>then the voltage is in the opposite polarity from the

0:30:08.040 --> 0:30:12.080
<v Speaker 1>primary coil. Polarity is really important, but also pretty complicated,

0:30:12.200 --> 0:30:17.040
<v Speaker 1>So I'll probably spend another episode to explain that concept

0:30:17.200 --> 0:30:20.760
<v Speaker 1>because it's really a bit much to go into right now.

0:30:21.720 --> 0:30:26.280
<v Speaker 1>But anyway, this is the basics for power transmission using

0:30:26.320 --> 0:30:31.240
<v Speaker 1>alternating current. It's the reason why we have alternating current

0:30:31.240 --> 0:30:34.200
<v Speaker 1>distributing our power instead of direct current. So then that

0:30:34.320 --> 0:30:39.480
<v Speaker 1>old Tesla versus Edison argument, really i should say Westinghouse

0:30:39.720 --> 0:30:43.760
<v Speaker 1>versus Edison argument, where Edison was saying direct current was

0:30:43.840 --> 0:30:47.320
<v Speaker 1>best and westing Us was saying no alternating current was best.

0:30:48.040 --> 0:30:51.320
<v Speaker 1>The things that let alternating current win out over direct

0:30:51.360 --> 0:30:56.200
<v Speaker 1>current where that using transformers you could boost the voltage

0:30:56.280 --> 0:31:01.160
<v Speaker 1>to huge high voltage numbers, which were great for power transmission.

0:31:01.440 --> 0:31:06.440
<v Speaker 1>You could transmit over vast distances using high voltage wires,

0:31:06.520 --> 0:31:09.200
<v Speaker 1>and then you would use other transformers on the opposite

0:31:09.320 --> 0:31:12.840
<v Speaker 1>end to step down the voltage until you reach the

0:31:12.920 --> 0:31:15.040
<v Speaker 1>level that was safe for homes, which in the United

0:31:15.040 --> 0:31:18.680
<v Speaker 1>States is two forty volts. Uh. Now, keep in mind

0:31:18.680 --> 0:31:21.360
<v Speaker 1>that when you're talking about transmission voltages, it could be

0:31:21.400 --> 0:31:24.120
<v Speaker 1>anywhere between a hundred fifty five thousand to seven d

0:31:24.200 --> 0:31:28.760
<v Speaker 1>sixty thousand volts, So we're talking huge differences here, and

0:31:28.800 --> 0:31:32.440
<v Speaker 1>it's all because you can use this basic element of

0:31:32.480 --> 0:31:36.880
<v Speaker 1>electronics with these transformers to step up or step down

0:31:36.880 --> 0:31:41.160
<v Speaker 1>the voltage simply by using different coils along a core.

0:31:42.240 --> 0:31:46.240
<v Speaker 1>So that was incredibly useful. You could end up transmitting

0:31:46.240 --> 0:31:49.600
<v Speaker 1>power over great distances. Direct current, however, is very different.

0:31:50.000 --> 0:31:52.760
<v Speaker 1>It is most efficient if it is close to whatever

0:31:52.840 --> 0:31:56.680
<v Speaker 1>the load is on the line. So the load is

0:31:56.720 --> 0:31:59.800
<v Speaker 1>whatever the electricity is meant to power. So in the

0:31:59.840 --> 0:32:02.880
<v Speaker 1>case of homes, you would want the power plant to

0:32:02.920 --> 0:32:06.800
<v Speaker 1>be relatively close to the homes that are receiving electricity.

0:32:06.880 --> 0:32:10.560
<v Speaker 1>If you were using direct current, um this is you know,

0:32:10.840 --> 0:32:14.600
<v Speaker 1>it would be incredibly useful to have direct current powering

0:32:14.600 --> 0:32:18.080
<v Speaker 1>our homes because most of the stuff we have relies

0:32:18.280 --> 0:32:23.000
<v Speaker 1>on direct current. It actually has to convert the alternating

0:32:23.040 --> 0:32:26.120
<v Speaker 1>current that comes to the house into direct current. You

0:32:26.160 --> 0:32:29.840
<v Speaker 1>have these converters that are part of the electronics that

0:32:29.920 --> 0:32:32.240
<v Speaker 1>allow it to do that. If you had direct current

0:32:32.320 --> 0:32:36.200
<v Speaker 1>being uh supplied directly to your house, you wouldn't need

0:32:36.240 --> 0:32:40.160
<v Speaker 1>the conversion part of those devices. However, you wouldn't be

0:32:40.160 --> 0:32:42.800
<v Speaker 1>able to transmit it over great distances like you can

0:32:42.880 --> 0:32:46.800
<v Speaker 1>with alternating current. So in case you're wondering about the

0:32:46.840 --> 0:32:49.720
<v Speaker 1>power grids in the United States. We I mentioned that

0:32:49.800 --> 0:32:52.800
<v Speaker 1>you have those those high voltage lines that are carrying

0:32:52.800 --> 0:32:57.360
<v Speaker 1>between a d to center sixty volts. When you get

0:32:57.400 --> 0:33:01.960
<v Speaker 1>to distribution levels, you step down that voltage to less

0:33:01.960 --> 0:33:04.600
<v Speaker 1>than ten thousand volts typically, and then you get to

0:33:04.680 --> 0:33:08.120
<v Speaker 1>distribution busses that have transformers that reduce it further to

0:33:08.360 --> 0:33:11.120
<v Speaker 1>seven thousand, two hundred volts or less. And then you

0:33:11.200 --> 0:33:13.560
<v Speaker 1>have the homes that are connected to a final transformer

0:33:13.640 --> 0:33:16.400
<v Speaker 1>that step it down again to the voltage of volts

0:33:16.480 --> 0:33:24.920
<v Speaker 1>or so. So incredibly useful and here at how stuff works. Recently,

0:33:25.160 --> 0:33:27.680
<v Speaker 1>as of the recording of this podcast, we had a

0:33:27.800 --> 0:33:32.320
<v Speaker 1>lovely transformer fire right next to the building we work in,

0:33:32.440 --> 0:33:35.160
<v Speaker 1>which cut power to our part of the building for

0:33:35.240 --> 0:33:38.360
<v Speaker 1>some time. So if you've ever been near a transformer

0:33:38.400 --> 0:33:41.800
<v Speaker 1>when it's blown, it's a pretty spectacular thing. It's usually

0:33:41.920 --> 0:33:45.040
<v Speaker 1>lots of sparks and a really loud bang and often

0:33:45.120 --> 0:33:50.200
<v Speaker 1>requires the work of dedicated personnel to repair. And it

0:33:50.280 --> 0:33:53.520
<v Speaker 1>does also typically mean that you have a loss of

0:33:53.600 --> 0:33:59.000
<v Speaker 1>power for at least a localized area. Pretty impressive when

0:33:59.040 --> 0:34:02.000
<v Speaker 1>it happens. Luckily, it doesn't happen all that frequently the

0:34:02.120 --> 0:34:06.160
<v Speaker 1>electrical storms and areas of or times of great use

0:34:06.800 --> 0:34:11.160
<v Speaker 1>can make the more vulnerable. Now let's move on to

0:34:11.719 --> 0:34:15.439
<v Speaker 1>semiconductors and how they are used in electronics. So we've

0:34:15.480 --> 0:34:18.000
<v Speaker 1>got lots of different uses for semiconductors. I'm going to

0:34:18.120 --> 0:34:21.839
<v Speaker 1>talk about two specific ones. There are diodes. Diodes are

0:34:21.840 --> 0:34:24.960
<v Speaker 1>really useful. They allow current to flow in only one direction,

0:34:25.000 --> 0:34:27.840
<v Speaker 1>so it's like a one way channel or a valve.

0:34:28.200 --> 0:34:30.760
<v Speaker 1>So electricity flowing one way is fine, but it cannot

0:34:30.800 --> 0:34:34.799
<v Speaker 1>flow back the other way, and semiconductor doping allows for

0:34:34.840 --> 0:34:37.839
<v Speaker 1>this to happen. Remember I mentioned earlier. Doping is when

0:34:37.880 --> 0:34:41.719
<v Speaker 1>you have introduced impurities into the semiconductor material to give

0:34:41.760 --> 0:34:46.200
<v Speaker 1>its specific UH features. So there are two different types

0:34:46.800 --> 0:34:49.680
<v Speaker 1>that we're going to talk about. There's IN type layers

0:34:49.760 --> 0:34:52.000
<v Speaker 1>of semiconductors, so you can think of that as an

0:34:52.040 --> 0:34:56.239
<v Speaker 1>excess of electrons. It has lots of negative electrons that

0:34:56.280 --> 0:34:59.560
<v Speaker 1>are just ready to flow out of there. And then

0:34:59.600 --> 0:35:03.880
<v Speaker 1>you have of P type layers, and these have electron

0:35:03.960 --> 0:35:06.000
<v Speaker 1>holes or at least you know, in other words, of

0:35:06.000 --> 0:35:10.040
<v Speaker 1>the capacity to take on electrons. So if you pair

0:35:10.080 --> 0:35:13.560
<v Speaker 1>this together, you get what's called a P N diode,

0:35:13.600 --> 0:35:16.280
<v Speaker 1>which all only allows electricity to flow in one direction.

0:35:16.480 --> 0:35:20.000
<v Speaker 1>It can the electrons can come through UH and flow

0:35:20.120 --> 0:35:24.200
<v Speaker 1>to the holes, but they can't go the other way,

0:35:24.280 --> 0:35:28.040
<v Speaker 1>so very useful and electronic components where you need to

0:35:28.080 --> 0:35:31.000
<v Speaker 1>direct the flow of electricity along a particular path and

0:35:31.040 --> 0:35:35.839
<v Speaker 1>prevent it from coming back through that pathway. Transistors are

0:35:35.880 --> 0:35:38.960
<v Speaker 1>another type of semiconductor that use a small amount of

0:35:38.960 --> 0:35:43.000
<v Speaker 1>current to control a large amount of current. So while

0:35:43.040 --> 0:35:47.400
<v Speaker 1>a diode is p n, transistors are either P n

0:35:47.560 --> 0:35:51.719
<v Speaker 1>P or N p n, and if you apply an

0:35:51.719 --> 0:35:54.520
<v Speaker 1>electrical current to the center layer, which is also known

0:35:54.560 --> 0:35:57.480
<v Speaker 1>as the base, electrons will move from the N type

0:35:57.520 --> 0:36:00.319
<v Speaker 1>side to the P type side, and that initial small

0:36:00.360 --> 0:36:02.719
<v Speaker 1>current allows for much larger current to flow through the

0:36:02.719 --> 0:36:07.920
<v Speaker 1>material at that point. So transistors act as switches or amplifiers.

0:36:08.520 --> 0:36:12.720
<v Speaker 1>Incredibly useful. So when we talk about transistors in solid

0:36:12.760 --> 0:36:16.279
<v Speaker 1>state electronics, these are the things that allow us to

0:36:17.120 --> 0:36:21.799
<v Speaker 1>build logic circuits. And it's because we can allow electrons

0:36:21.840 --> 0:36:25.400
<v Speaker 1>to either flow or prevent them from flowing. It's also

0:36:25.520 --> 0:36:28.840
<v Speaker 1>why things like electron tunneling can be such a problem.

0:36:29.520 --> 0:36:33.080
<v Speaker 1>Electron tunneling is a quantum effect, so you can think

0:36:33.080 --> 0:36:36.319
<v Speaker 1>of an electron as not really existing in a specific

0:36:36.640 --> 0:36:40.400
<v Speaker 1>point in space at any given time, but rather having

0:36:40.440 --> 0:36:44.560
<v Speaker 1>the potential to exist in an area of space at

0:36:44.600 --> 0:36:47.279
<v Speaker 1>any point in time. So think of it like a

0:36:47.280 --> 0:36:52.200
<v Speaker 1>cloud where an electron could be, and that cloud covers

0:36:52.239 --> 0:36:54.759
<v Speaker 1>all the potential places the electron could be, and there's

0:36:54.840 --> 0:36:58.600
<v Speaker 1>different probability for different parts of the cloud. If your

0:36:58.760 --> 0:37:03.040
<v Speaker 1>transistor gates are so small, so narrow, so thin, I

0:37:03.080 --> 0:37:06.600
<v Speaker 1>guess I should say not narrow, that the cloud of

0:37:06.680 --> 0:37:11.160
<v Speaker 1>potential can overlap the transistor gate. That means there is

0:37:11.200 --> 0:37:15.240
<v Speaker 1>the possibility that at some point the electron could exist

0:37:15.320 --> 0:37:17.719
<v Speaker 1>on the other side of the transistor gate, even if

0:37:17.719 --> 0:37:21.840
<v Speaker 1>the gate never opened. And if there's a possibility, that

0:37:21.880 --> 0:37:24.480
<v Speaker 1>means sometimes it does appear on the other side of

0:37:24.480 --> 0:37:27.480
<v Speaker 1>the gate. We call it electron tunneling. It's not really tunneling.

0:37:27.600 --> 0:37:30.279
<v Speaker 1>It's just if there is the possibility they could be

0:37:30.320 --> 0:37:33.120
<v Speaker 1>on the other side, sometimes it is on the other side,

0:37:33.760 --> 0:37:37.000
<v Speaker 1>which means that you cannot actually control the flow of electrons.

0:37:37.080 --> 0:37:40.120
<v Speaker 1>In that case, it would mean that your transistors would

0:37:40.120 --> 0:37:42.160
<v Speaker 1>be ineffective in doing what they're supposed to do. They

0:37:42.160 --> 0:37:44.920
<v Speaker 1>wouldn't really be able to act to switches reliably and

0:37:44.920 --> 0:37:49.120
<v Speaker 1>you would get errors in your computations. I might work

0:37:49.480 --> 0:37:51.719
<v Speaker 1>most of the time and then only some of the

0:37:51.760 --> 0:37:54.600
<v Speaker 1>time not work, but even then that's problematic, which is

0:37:54.640 --> 0:37:59.120
<v Speaker 1>one of the engineering challenges that transistor designers and multi

0:37:59.640 --> 0:38:02.960
<v Speaker 1>around their microprocessor designers encounter all the time, you know.

0:38:03.080 --> 0:38:08.320
<v Speaker 1>Finding new materials that are better at acting as transistors

0:38:08.320 --> 0:38:12.120
<v Speaker 1>switches it's a big part of it. And coming up

0:38:12.160 --> 0:38:15.919
<v Speaker 1>with different architectures to really take advantage of electron flow

0:38:16.000 --> 0:38:19.040
<v Speaker 1>is another big part of it, all right. So those

0:38:19.080 --> 0:38:22.920
<v Speaker 1>are the basics the basic electronic components that you can

0:38:22.960 --> 0:38:26.080
<v Speaker 1>talk about with, you know, if you're looking at it

0:38:26.120 --> 0:38:28.719
<v Speaker 1>from a very high level. Obviously there's tons of other

0:38:28.760 --> 0:38:31.040
<v Speaker 1>stuff that I didn't get into, and some of it

0:38:31.080 --> 0:38:36.080
<v Speaker 1>just requires you to pair up or otherwise put into

0:38:36.120 --> 0:38:38.759
<v Speaker 1>series or parallels some of the components I've mentioned to

0:38:39.120 --> 0:38:43.040
<v Speaker 1>to get whatever effects you want. I hope you enjoyed

0:38:43.080 --> 0:38:45.600
<v Speaker 1>that classic episode of tech Stuff as we covered the

0:38:45.640 --> 0:38:49.040
<v Speaker 1>basic components of electronics. It's probably something I'll end up

0:38:49.080 --> 0:38:53.239
<v Speaker 1>covering again in various Tech Stuff tidbits episodes where I

0:38:53.320 --> 0:38:58.319
<v Speaker 1>really focus on specific components and their place in electronics

0:38:58.360 --> 0:39:02.080
<v Speaker 1>and their purpose. Because us you can always do a

0:39:02.080 --> 0:39:05.319
<v Speaker 1>better job, right. I mean, I'm always proud of the

0:39:05.320 --> 0:39:08.880
<v Speaker 1>work I do, but I also recognize when I could

0:39:08.920 --> 0:39:11.839
<v Speaker 1>do it even better, and I think it's about time

0:39:11.880 --> 0:39:14.239
<v Speaker 1>I try and do that. If you have suggestions for

0:39:14.280 --> 0:39:16.480
<v Speaker 1>topics I should cover in future episodes of tech Stuff,

0:39:16.520 --> 0:39:18.600
<v Speaker 1>reach out to me on Twitter to handle for the

0:39:18.600 --> 0:39:21.799
<v Speaker 1>show is tech Stuff hs W, and I'll talk to

0:39:21.800 --> 0:39:30.399
<v Speaker 1>you again really soon. Text Stuff is an I Heart

0:39:30.480 --> 0:39:34.239
<v Speaker 1>Radio production. For more podcasts from I Heart Radio, visit

0:39:34.280 --> 0:39:37.319
<v Speaker 1>the I Heart Radio app, Apple Podcasts, or wherever you

0:39:37.440 --> 0:39:38.760
<v Speaker 1>listen to your favorite shows.