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00:03 | as promised. Here we are with part of lecture that I was not |
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00:07 | to get during class time and really we did we were talking about membrane |
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00:12 | were talking about how we go about changes in them. There are two |
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00:17 | types of membrane potential change. There's is called the action potential and what |
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00:21 | called the grated potential. And so the great next light. So what |
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00:27 | want to just kind of do you to give you the overview and we're |
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00:29 | to see how the greatest potential is . We're going first, kind of |
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00:33 | them, look a great potential. look at the axe potential, see |
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00:36 | to conduct. So the action potential our starting form. We said, |
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00:40 | is its? They change the membrane . This is actually a very large |
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00:45 | . All right, so we're looking something. It's very quick, very |
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00:49 | and very brief for rapid in terms how it moves. And we're looking |
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00:54 | something like 100 million volts change. , Miller votes are very, very |
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00:59 | , but but relative to a it's a fairly large thing. And |
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01:04 | what we're doing here is we're taking cell and what is normally negative membrane |
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01:11 | , and we're reversing. It were bringing it up to 100 mill. |
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01:15 | mean, not 100 levels, but minimal change from that starting point, |
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01:20 | least a neuron. And whenever we're at a potential remembering potential chain, |
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01:25 | , we're not talking about the entire , just going to a member of |
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01:31 | . It starts as a very, small portion remembering. All right, |
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01:36 | we're looking at whenever we see a here or even on the other |
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01:40 | we're looking at just a single point the plaza memory. And then what |
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01:45 | gonna do is we're gonna see how change occurs from that membrane from that |
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01:51 | point. And so when you're looking this graph right here, what you're |
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01:56 | at is you're looking at Miller Volts time. All right, so down |
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02:00 | the bottom, that's time. And you're looking at that single point you |
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02:04 | see here. We've got a little . We're looking at that single |
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02:07 | And what we're saying is look, is the stimulus. So our stimulus |
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02:11 | either on or it's off. So your off position. There's your own |
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02:16 | . So nothing's going on, and we turn it on their simulation. |
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02:19 | we turn off stimulation going. And what you can see here is we |
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02:24 | at a a specific charge. We're doing anything. And then when the |
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02:28 | occurs, what happens? We see rapid rise over time, and it |
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02:34 | this rapid fall that occurs there. her. Okay, so that's kind |
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02:39 | what we're looking at. Three Easy to visualize this. Which is why |
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02:44 | wish you all were in class. you could do this at home. |
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02:47 | just bear with me is I want to picture a wave. I'm not |
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02:52 | a wave like that. The I'm talking about what you do at |
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02:55 | event. All right, so you're in your chair, you're looking |
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02:58 | you have 100,000 people or 40,000 people whatever it is around view, and |
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03:02 | starts the wave and it starts moving the stadium. And so you're gonna |
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03:06 | that wave of people standing up, sitting down, it comes over to |
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03:11 | , and from where you are. you do is you basically take your |
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03:14 | from your side and you lift them and over your head and to the |
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03:18 | tough. And then you bring them again. And that's kind of the |
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03:20 | that we're looking at. We're looking at this particular action potential. We're |
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03:25 | at an individual, lifting their hands in putting their hands back down over |
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03:30 | . And that's what that rapid rises what that rapid fall is. It's |
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03:35 | the flow of ions over that period time, causing that deep polarization that's |
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03:40 | initial phase and then re polarizing back their original position. Now with an |
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03:47 | potential. What's gonna happen is, you produce it, it propagates just |
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03:51 | a wave does at a sporting So you can imagine Here is your |
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03:55 | right. You start the wave and goes around the circle and keeps going |
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04:01 | , and it just keeps going and going. In other words, it's |
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04:04 | in such a way that doesn't diminish strength. It stays the same strength |
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04:09 | entire length that that wave moves, that's what an action potential does. |
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04:14 | starts at a single point. All , so here is your neuron. |
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04:22 | your axe, Exxon. It starts a single point, and then once |
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04:26 | produced, it stays the same And it keeps going the entire |
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04:33 | All right, so you can imagine wave moving entire land. And it |
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04:37 | not diminish in strength and stays at same strength the entire length. All |
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04:43 | now, the key thing about an potential on this is important. It's |
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04:46 | all or nothing response. It either 100% or doesn't respond at all. |
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04:52 | it's very binary. It's not a , I'll kind of be in |
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04:57 | You don't kind of go up to and then come back down. It's |
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05:01 | away back down, but you have reach a certain threshold. All |
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05:06 | that's what they're showing right here is a threshold. If you can reach |
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05:10 | , you produce the big wave. you can't reach threshold, you don't |
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05:16 | the wave at all. You basically underneath that coin. All right, |
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05:22 | that's one of the key things about the action. The great potential, |
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05:30 | the other hand, is different in it is still remembering potential change, |
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05:36 | it can go in either direction. can either be a deep polarisation or |
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05:42 | . Here was the deep polarisation. the hype. Accorsi. The second |
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05:46 | about a great potential is that whatever causing the triggering event, it's gonna |
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05:51 | different magnitudes that produce that trigger of . And so the response that the |
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05:58 | potential has is equivalent to the So there are magnitude magnitude inal differences |
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06:05 | great potential in grated potentials. But means is that weaker stimuli result in |
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06:11 | responses. And that's what this is to shows like again, Here's our |
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06:15 | graph. This is a responsive It says. Look, here's the |
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06:19 | line. It says. That's a weak signal. Look, I still |
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06:23 | a membrane potential change. It's a , itsy bitsy, teeny tiny |
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06:27 | The larger the stimulus, the stronger potential right. And what you can |
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06:33 | here is I've actually turned it into action potential, which we'll get to |
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06:37 | just a moment. But look at opposite. Here appear this is |
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06:40 | hyper polarization. So this is This is causing hyper polarization, so |
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06:46 | stimulus is weak, larger, larger largest. You can see a moving |
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06:54 | and further and further down that hyper into that for a state. So |
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07:00 | we have here is a member of change that has a variety or |
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07:07 | the responses is equivalent or related to magnitude of the trigger. So in |
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07:15 | , the bigger the trigger, the the response is smaller, the period |
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07:18 | the smaller response. And this is true with regard to duration, which |
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07:22 | not really dealing with here. But , on our grasses time, the |
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07:28 | that that stimulation is there with longer , the greater potential is going to |
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07:35 | . Now again, we're looking at single point, and what we need |
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07:39 | understand is that these ions are moving that single point of stimulation. So |
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07:45 | is kind of what this draft is to show you say, Look, |
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07:47 | is where the point of stimulation probably find a different. So I guess |
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07:51 | have to use something like start purple. All right, so So |
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08:00 | we have, where the stimulation you can see the little channel. |
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08:05 | happens is is stimulation caused the opening the channel. Whatever the channel happens |
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08:09 | be, ions flow in. And are they flowing in while they're trying |
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08:13 | find their partner? And so you imagine the first place that they're going |
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08:18 | have the highest amount of ions is the point of influx, all |
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08:23 | where they're coming in. But as as they partner up, there's there's |
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08:29 | and fewer ions that are cables are to travel further and further away. |
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08:33 | so if you were to measure at and further points, what you find |
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08:38 | that the the membrane potential change is and smaller and smaller. Another would |
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08:47 | . In other words, what's happening is that the membrane potential change is |
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08:51 | out over a very, very short . So there's many reasons for |
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08:56 | One is that pairing, but they the ions are leaking back out, |
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09:00 | out whatever the case may be. this is again, this is deep |
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09:03 | . So this would be true also polarization, but your items might be |
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09:09 | brought back in. But the point this is is that what we have |
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09:14 | with the greatest potential is that that could only travel very, very short |
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09:21 | . Whereas what We're looking at the potential. It can trouble very long |
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09:26 | because of this non Decorah mental, , propagation that occurs as a result |
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09:32 | that. So action potentials are these changes, right? They leads that |
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09:41 | are large island movements that are causing very large membrane potential change. |
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09:49 | then, is a maximum membrane potential that travels. All right. The |
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09:55 | potential is kind of like a rippling you throw. You throw a rock |
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09:59 | a pond, you get ripples that of move outward. And over certain |
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10:05 | that ripple dies out. Ex You don't get that dying out. |
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10:10 | does this happen? Well, it back to those irons that we talked |
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10:13 | the sodium and potassium, All And what we have here is we |
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10:17 | channels that are going to be depended the change in the membranes state toe |
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10:22 | up. In other words, what have here is a special type of |
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10:25 | that responds to the membrane potential. called a voltage gated channels all |
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10:31 | And these have lots of charge groups them, and what they do is |
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10:34 | the membrane potential changes. It causes change in the shape of the |
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10:39 | which opens up, which allows more to flow in or out, which |
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10:43 | further changes in their shape. And that's kind of the positive feedback loop |
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10:47 | allows for the membrane potential change to . All right, And these particular |
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10:52 | are gonna be located a very specific called the Axon Hillock. Now |
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10:57 | we said, there's two different types channels. We have the voltage gated |
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11:00 | channel, all right, and this kind of a unique channel in that |
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11:03 | has two gates, all right, there's not one gate through which arms |
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11:08 | to flow. There's two of them one is called an activation gig one's |
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11:12 | inactivation. You can see here in initial state. What we have is |
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11:17 | have a closed activation gate button open gate so before stimulus ions can flow |
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11:24 | because the activation gate is closed. when you're stimulate the channel, what |
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11:30 | is that the gate opens up all , so I owns can flow |
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11:34 | but at the same time that you that that channel that the inactivation gate |
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11:40 | to close, but it takes a bit more time. And so the |
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11:44 | state is you're now back in a steak, but it's a result of |
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11:47 | second gate and then what you have do to bring yourself capable of |
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11:53 | And you have to reset yourself all way back here. You don't go |
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11:57 | this middle state. It's a than , then see, and then all |
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12:03 | way back to a There's no middle in there. Okay, so the |
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12:11 | picture here, the full city gated channel has three configurations. We call |
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12:16 | closed, capable of opening, opened then closed but incapable of opening. |
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12:22 | you have to come all the way from the inactivated state to the ready |
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12:26 | open state before anything else happens. system multi tasking channel makes more |
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12:36 | It's one that's easy to identify. has won gates, so you have |
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12:39 | states. It's either open or When the clothes tasking can't flow |
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12:44 | open tasking can flow out all And so what I want to do |
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12:48 | I want to break down this action . Alright, we're just gonna walk |
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12:52 | . So remember, we're looking at single point, and what we're asking |
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12:56 | is what is happening over this period time. At this single point, |
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13:01 | our starting point is gonna be here rest, so just follow the |
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13:04 | All right? So at rest we This is at the Axon Hillock. |
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13:09 | right, These voltage gated sodium channels bull escaped tasking channels are closed. |
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13:15 | close to know our own passes but we do have the natural flow |
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13:20 | we would get because we have the the study and potassium leak channels. |
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13:24 | have the sodium potassium, 80 Ace. So these leak channels and |
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13:31 | pump are basically maintaining that membrane potential the resting potential right here. |
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13:38 | That's what you're seeing now, at period of time, remember, we've |
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13:42 | said that there is a relative permeability between sodium and potassium, right? |
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13:50 | supersedes sodium movement by almost 50 to to one. And the reason for |
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13:56 | is because you have so many potassium . Very few, uh, sodium |
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14:04 | . Make sure I said that, . Many, many potassium channels very |
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14:07 | sodium channels. All right, so the key thing. So what's keeping |
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14:12 | at that Near that minus 70 is that that strange ratio, all |
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14:18 | but we still have these channels, they're closed. And because their |
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14:22 | that doesn't affect probability permeability right now rest permeability is a constant. So |
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14:29 | have a triggering event. When is trigger have been simply the stimulus that |
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14:33 | along and causes the opening of these ? Now we're gonna open up a |
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14:38 | bunch of different types channel We don't not talking about what the triggering event |
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14:42 | . But generally speaking, the triggering opens up a different type of |
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14:46 | usually at the at the dendrite, then causes a grated potential to be |
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14:53 | , which moves towards the acts on . It's here at the Axon |
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14:57 | where we have these voltage gated And if it's a deep polarisation |
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15:03 | what's gonna happen is you're gonna open the voltage gated sodium channels. And |
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15:06 | when that happens, more sodium comes the cell, and when you open |
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15:10 | more voltage gated sodium channels and studying , sodium is coming into the |
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15:14 | That's gonna cause further deep polarisation, causes more voltage gated sodium channels to |
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15:18 | , which causes more sodium come which causes more Holzer gated sodium channels |
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15:22 | create system positive feedback loop to the where all the voltage gated sodium channels |
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15:29 | open. And so as a what we're doing is we are moving |
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15:35 | and upward enough word, all so sodium is basically feeding back through |
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15:42 | mechanism because all the voltage gated sodium to open. So threshold is really |
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15:50 | point. Win that voltage gated All voltage Gated city and channels are |
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15:55 | So what you've done now is you the permeability, all right, so |
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16:02 | just making up a number. It's a real number, but let's say |
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16:05 | 1000 channels, right. And you start off with one's sodium Leak |
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16:11 | to 75. I'll just use It's an easier number 50 potassium leave |
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16:16 | . And then now what you've done this stimulation is you resulted opening up |
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16:23 | sodium or voltage gated sodium channel. instead of being 1 to 50 now |
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16:28 | 1000 of 50 and so it's now is that the permeability of sodium is |
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16:35 | the member and so sodium is rushing the south, and that's why you're |
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16:39 | to start seeing this massive climb. Threshold represents the point when these all |
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16:45 | channels have opened up now. So gonna keep coming in until it reaches |
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16:51 | 60 given the opportunity to do All right, that's what that's what |
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16:55 | trying to do. But something happens it ever gets there. And what's |
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17:01 | is, is that that channel? , we said it has two gates |
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17:06 | voltage gated sodium channel. It opened activation gate to allow the sudden a |
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17:10 | . But at the same time, when that voltage gated inactivation gate begins |
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17:16 | close. It's just slower. And what happens is while those gates are |
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17:22 | , you're getting sodium to come But when it closes, it ceases |
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17:25 | allow any more sodium to come and you were turned membrane potential back |
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17:29 | to its original state. All so what we've done here is basically |
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17:35 | reached the peak of flow, all , because he slammed all the doors |
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17:40 | . If nothing else were to then because leak channels in the |
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17:43 | We slowly moved back then, but don't do that. Instead, we |
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17:48 | this massive return this very quick And again, look at the relative |
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17:54 | here. We're looking at roughly a for all this to take place. |
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17:59 | right, so 11 thousands of a . That's a quick. So while |
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18:04 | sodium channels cultivated sitting shells have slammed at the same time, What we're |
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18:10 | is we're opening up the potassium Now. The easiest thing to think |
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18:16 | is that the voltage gated potassium channel being stimulated because we reached a certain |
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18:21 | way up there that's actually know what . The voltage gated potassium channel is |
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18:27 | your your ignorant friend, the one a little slow, you know, |
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18:31 | that you tell jokes to. It about a minute before they figure it |
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18:35 | . That's what's going on because the stimulus that occurred there that caused the |
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18:40 | gated sodium channel open is the exact stimulus that causes the voltage gated |
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18:46 | It just takes more time to do . It's a slow gait, and |
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18:50 | why it takes this long before it gets there, so it's almost a |
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18:55 | a millisecond before the potassium Channel But it's also the same amount of |
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19:00 | that that sodium channel closes. So two events simultaneously results in the flipping |
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19:08 | the membrane back towards re polarization. so, just to put this in |
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19:14 | , what are we doing? We the channel, which prevents more sodium |
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19:19 | coming in, and we open up vault scape. Taxing channel, which |
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19:22 | allowing the potassium to leave, which shoots it down, allows it to |
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19:29 | back down. And that's what's going as we're returning to rest now. |
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19:35 | can see in the graph here, that here's rest and we overshoot for |
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19:43 | reason. What happens well again. low, close, it's It's a |
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19:49 | opening channels, also slow closing and as a result, it takes |
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19:53 | little bit of time for those things close. So even though it should |
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19:56 | closed by this point to get us to their, we overshoot a little |
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20:00 | , and so we kind of hyper for a little bit. Before we |
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20:03 | back to normal, you can see showing a slow rise there. That's |
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20:07 | the artist, um, artists freedom do so. All right, so |
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20:14 | sodium channels, they're slow closing results a transient hyper polarization. All |
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20:22 | so we have a couple of Vince , very simple, right? We |
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20:26 | result. Me, we started rest . Rest is the stimulus that seamless |
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20:33 | up to control to get sodium positive feedback loop what we're seeing down |
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20:39 | , right? All the channels are , so we have rapid, deep |
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20:44 | . Those channels closed at the same . The voltage gated potassium channels |
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20:48 | which causes the rapid falling phase. channels closed, but they're a little |
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20:54 | . So we get this light hyper . Um, um after we've returned |
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21:00 | rest. So that is the events the resting potential. What you can |
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21:05 | to help you understand this is to at where change is occurring and ask |
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21:11 | why? Why does the graft change this point? And that's an easy |
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21:16 | to think about this. So there's couple of other ideas that I |
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21:23 | you understand for the action. All . So an action potential is simply |
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21:28 | electrical signal. Remember, traveling from cell body down the axe onto the |
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21:32 | on terminal. And what you wanted do is you want to ensure that |
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21:36 | signal is gonna be maintained in terms size, and it goes in the |
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21:41 | that you want to go into wanted go to. And so to do |
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21:45 | , what we have is what is a refractory period and the pure definition |
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21:49 | refractory. Here is that period of when something has to be reset before |
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21:56 | can be repeated, that whatever it that you're looking at, so with |
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21:59 | to an action potential, it's that of time when an action potential can |
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22:03 | produced under normal circumstances. Win that of that accident has already undergone an |
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22:10 | . And so what that means is when I produce an action potential, |
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22:13 | actress tensions to move away before I produce another one. Because there's a |
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22:19 | of time when I can't do there's actually two halves to it. |
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22:23 | the refractory period you can see here kind of demarcated as two halves. |
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22:27 | has what is referred to as an period of one is referred for the |
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22:31 | , period. All right, we're looking at a single point on |
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22:36 | Ansan, and we're asking what's happening that period of time? Well, |
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22:41 | the first part of that action potential what we would call the absolute. |
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22:47 | this is that period of time, said, is when all those sodium |
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22:50 | are open. We said, all open. And so if you've opened |
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22:55 | all the channels and all the sodium could be rushing in is rushing |
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23:01 | it doesn't matter how much you stimulate sell. You can't open with air |
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23:06 | . They're already in the open so you can't get another action potential |
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23:10 | stimulation. It's already happening. But also need to remember that these channels |
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23:16 | , go through those three stages. so once you start the stage |
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23:21 | you have to go from stage one stage two to Stage Three. Or |
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23:24 | I said earlier was ABC. So you started, you have to go |
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23:28 | that whole thing before you can even to try to stimulate that cell |
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23:34 | So the absolute refractory period is a of time when there's no responsiveness to |
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23:40 | . You've already gotten your stimulus so seem most was enough to produce the |
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23:45 | . And so what this does it that the action potential cannot occur until |
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23:51 | preceding one has moved away. So the absolute curry. The relative refractory |
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23:58 | is during that period of time when are in our re polarization and in |
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24:04 | hyper polarization re polarization stage All in those two things. So here |
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24:09 | we've done is we're article on through resetting of those sodium channels was voted |
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24:16 | get excited. They're not 100% but there's some that are so we're |
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24:23 | at, like maybe 90% of them . So what we're doing is way |
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24:27 | get 100% responsiveness because of those channels being in their clothes statement to be |
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24:34 | . All right. But the other that we have to overcome So even |
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24:38 | we have enough voltage gated sodium channels be able to overcome the threshold, |
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24:45 | still dealing with our slow friend, ? That potassium, that voltage gated |
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24:51 | channel still is in the open And so even if you've opened up |
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24:54 | channels, you saw open potassium and so you're seeing no real net |
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25:00 | , so you have to be able have a stronger, stronger responsiveness. |
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25:07 | word. Mawr voltage gated sodium channels relative to the potassium. So it |
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25:14 | possible. So let's let's just kind put this into visual, right? |
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25:19 | this is threshold, if high in , it's going to take longer form |
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25:25 | stimulus to get me up there that did when I was there. All |
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25:30 | , maybe it's a five extra Maybe it's 10 extra millet balls, |
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25:34 | I need tohave mawr of a signal order for me for that to |
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25:39 | All right, so what this It limits the frequency of when we |
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25:45 | action potential, because we have to be really, really strong to produce |
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25:50 | one in our relative period, or have the wait for the absolute period |
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25:55 | move past. And so that means a mass commemorated, which you can |
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26:00 | action. But what this also means that you can actually in code because |
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26:07 | , action potential are fairly far You can actually increase the frequency and |
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26:12 | the action potentials closer and closer and together. That's one way that the |
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26:19 | system in codes information is in the of the action. How often are |
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26:24 | being put together that encodes some of information that should produce it. Now |
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26:29 | frack, your periods have different lengths different types of neurons in different types |
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26:33 | tissues. So we can't say they look the same. They're just |
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26:37 | but they all deal with the same . It's basically a period of time |
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26:42 | you can't produce an extra potential in normal of circumstances. So this is |
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26:48 | home stretch. It was basically an 30 minutes. It looks like and |
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26:53 | over. Dealing, you know, how does it action potential conducted And |
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26:57 | you can see here what we're looking . This would be your excellent. |
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27:00 | look right here. All right, is your acts on. You can |
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27:04 | . We got a whole bunch of lined up trying to come in when |
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27:07 | open up enough of those sodium What they're gonna do is the sodium |
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27:11 | in like a great potential, and it finds its partner and said |
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27:16 | ? I found a partner, but ones that don't move forward and they |
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27:20 | moving forward, and it causes that . Potential change causes a deep |
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27:25 | which results in the opening of more gated channels because he's voltage gated, |
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27:29 | channels lying the entire length of the as good a vulture gave. And |
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27:35 | what happens is is, as the flows in it keep propagating the action |
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27:41 | . Ford. So you can imagine here that it's there and then it's |
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27:45 | , and I know that the driver great, but you can kind of |
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27:47 | the sense is the wave begins propagating the length of the action, all |
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27:54 | ? And the reason don't go backwards because, remember, we're dealing with |
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27:57 | refractory region on the backside, so only allows the action potential move in |
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28:03 | direction. Now there are two different that actually propagated Easy. One to |
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28:09 | about is what is called continuous All right, And so here we |
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28:14 | the entire axe on exposed to the cellular fluid. And so you can |
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28:19 | that I own all or not thes gated channels along the entire length, |
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28:24 | so basically I have to open and each single one of them is kind |
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28:27 | like in a continuous mode would be of like walking across the floor. |
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28:32 | hell, All right, so you're to see this whenever you have accents |
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28:37 | lack my Alan. It's a fairly process because just, like watch walking |
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28:42 | Hill while there's a distance to you have no gap between your in |
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28:47 | stride. You're basically toe to heel heel, and it's a very slow |
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28:51 | , all right, but it zey typical it's what we would think about |
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28:55 | be occurring. But the problem is that in order to get signals |
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29:01 | go faster, there's really only two to do that. All right, |
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29:06 | come back to this slide right. first way is to increase the dynamic |
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29:12 | of of the of the Axe on right, which means you have to |
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29:17 | it wider. It's kind of like . If you feel you are audio |
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29:21 | will know this. The thicker the less resistance, the better the |
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29:25 | the thinner the wire. The more you have, the harder it is |
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29:30 | get good sound out of it. of wire. And so so the |
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29:34 | here is I need big fat fibers I want to speed up the process |
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29:39 | propagation. Problem is, if I make a bigger, fatter axe |
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29:43 | it means I need a bigger If I have a bigger neuron, |
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29:45 | need a bigger space to put that got thousands upon millions of these things |
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29:50 | your body so you can imagine your would have to be bigger as a |
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29:54 | of that. And so it just probably means a further distance that up |
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29:59 | travel with me, they need a neuron in the audio, so that |
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30:03 | not a solution. It's a solution you have a same size critter or |
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30:08 | same size person. So a bigger is faster than a smaller neuron. |
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30:14 | you can't make all neurons bigger. so what the body came up with |
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30:18 | this plan that's called my Elonis all , and my l. A. |
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30:24 | is using those Schwann cells or those ago dinner sites in the central nervous |
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30:28 | to cover up a portion of that . So there's only a very, |
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30:34 | small portion of the axe on exposed the extra cellular fluid. And so |
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30:41 | is where the action potential they're gonna place the distance between one note in |
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30:46 | next and these air called the nodes Randhir. So that little space, |
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30:50 | there is a note of ranveer That's note of ranveer. That's another |
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30:54 | This is a mile in sheep. right, action, petition action potentials |
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30:59 | being produced at the nodes of All right? And so what happens |
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31:06 | , is that instead of covering the length of the axe on what we |
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31:12 | is we leap from note of Randhir note of Rand view. It's kind |
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31:17 | like a stride, and the distance these nodes is just far enough that |
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31:23 | action potential could be stimulated each All right, so there, as |
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31:28 | as they can be. So it's life. He stride once you stand |
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31:32 | right now, I don't want you walk across the room, toted hell |
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31:35 | see how long it takes you. then I want you walk across the |
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31:37 | the other direction using a regular stride see how much faster it iss all |
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31:43 | . So when my illness present, going to get salvatori, which literally |
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31:49 | to jump. All right. This is a better representation of |
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31:56 | You can see here all my channels can see I'm insulated from the |
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32:01 | So I'm opening and closing the voltage channels IOM's air flowing through, which |
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32:06 | a change in the membrane so that could get the next one and then |
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32:09 | next one. And that's why I'm from one to the neck. And |
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32:14 | allows that signal to move incredibly fast increasing the size of the fiber. |
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32:20 | you can keep your are your your I were small, The other thing |
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32:25 | does incredibly beneficial because it consumes less . And, of course, the |
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32:29 | is always looking for reasons for using energy. So our goal here to |
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32:36 | is that the action potential is going travel, um, quicker with Miles |
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32:44 | because of these little regions in between mile and called nodes of ranveer. |
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32:50 | right, That's what I wanted to to. And so that catches us |
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32:55 | . I hope you enjoy this. was 30 extra minutes. I'm |
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32:59 | I've just been talking slow all Maybe I will be caught up after |
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33:05 | unit. You can come and ask questions at office hours. That's going |
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33:09 | Thursday from 11 to noon. Or can ask questions in class. I |
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33:16 | more questions begin classes slower ago. not a reason not to ask |
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33:20 | I'm just letting you know that. thank you for tuning in |
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