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00:02 | this is Lecture five of neuroscience and finished talking about neurons and some of |
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00:08 | properties of neurons. And we started about neuron subtypes and we said how |
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00:15 | you distinguish these different subtypes of We can distinguish it based on |
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00:21 | We can distinguish based on excitability, versus inhibitory. We can distinguish based |
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00:28 | projection whether they are projecting into the networks. In this case the parameter |
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00:33 | of the hippocampus parameter cells of the york cortex will be excited to your |
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00:38 | sells this circuit that we looked There's a lot of things in the |
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00:44 | that will be replicated in different parts the brain. But we presented that |
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00:48 | a somewhat simple circuit. Three layer as opposed to neo cortical circuit which |
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00:53 | will study in the third section of course that has six layers and has |
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00:58 | lot more complex anatomy and connectivity. this is just an introduction to how |
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01:04 | circuits work. And in general you these excitatory projection cells and the activity |
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01:10 | these projections cells is going to be to interconnected regions. In this case |
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01:15 | the hippocampus there flanked by these much diverse and different subtypes of inhibitory into |
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01:25 | and inhibitory interneuron that will all be Gaba but there will also be |
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01:30 | They'll be different based on their morphology on the synopsis and what parts of |
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01:36 | excitatory cells they target and also distinguished unique and for cellular markers that they |
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01:43 | be expressing and as we discussed they also have distinct membrane produced. So |
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01:55 | modern electrophysiology, I thought somebody was on zoom. But it was just |
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02:01 | . Uh So these cells apart from these different morphological and cellular markers as |
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02:09 | may and live in different locations and different aspects of the parameter cells. |
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02:16 | also have a different dialect. And dialect is the active in this case |
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02:22 | pattern of action potentials, that active properties. And we will be getting |
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02:26 | a lot more of what happens for action potential to take place. What |
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02:32 | happens at the biophysical level at the of the member in the next couple |
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02:36 | lectures. So what questions may you from the slide? We spend |
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02:43 | maybe half an hour, 20 minutes the slide. You can expect |
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02:47 | Are there 21 subtypes of tyrannical excitatory ? What are they inhibit? Their |
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02:53 | nerds and hippocampus release glutamate or Are they excited to parameter cells, |
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03:01 | cells or their local inter neurons. of these are great questions. Uh |
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03:08 | uh as I said some of the that we study will get more and |
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03:12 | complex with time. So we talked the dialect of neurons. Yes, |
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03:22 | . Or let's see I'm a schematic . The little yellow triangles are axons |
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03:39 | and and synapses onto the parameter So these are the selma's in red |
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03:45 | an orange, you have dendrites and little yellow cups, I mentioned it |
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03:50 | the past. But these little yellow and thanks for asking that again are |
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03:54 | axons and their synapses And this shows that some of them will target these |
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04:00 | regions of parameter cells. Because if recall 90% of the parameter cells, |
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04:06 | are going to be found in this intermodal region. So some of them |
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04:11 | cells will target the Selma's and others target the ethical dem rights and yet |
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04:18 | will target the basil dendrites and even axons of these parameter cells. So |
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04:25 | can think of these inhibitory cells. not only have these different dialects and |
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04:30 | frequencies by which they control the output the hippocampus, but they can also |
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04:36 | the integrative properties by targeting dendrites and . Because Selma integrates all of the |
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04:44 | and they can also modulate the output targeting the axon. So there's almost |
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04:50 | three levels of control anatomically dendrite axons or inputs, integration and outputs |
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04:59 | those four regions that we discussed in therefore functional domains and regions uh and |
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05:06 | have all of these different patterns that can do that all of these three |
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05:10 | levels and that's what makes the output comes out of the parameter cells which |
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05:15 | just speak one dialect. Now they're controlled how they speak when they |
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05:20 | when they can you know, really a lot. And when they get |
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05:26 | and their activity is sequestered into the circuits. Is there some significance where |
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05:33 | amygdala and the programmable cells are coming with it. It's it's it's it's |
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05:42 | schematic illustration of some of the projections connectivity. I wouldn't worry about |
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05:46 | The take home message is the parameter would project out of it. But |
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05:51 | do recall somebody else had a really question about the circuit. So does |
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05:57 | mean that parameter cells and inhibitory cells some common input? And the answer |
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06:05 | yes. So these projection cells parameter when they're gonna project into another |
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06:11 | they're gonna contact excitatory cells in the circuit and they're gonna contact inhibitory |
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06:19 | Everything is interconnected. Excitatory cells can inhibitory cells, inhibitory cells can target |
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06:25 | cells. Excitatory cells can target excitatory inhibitory cells. Target inhibitory cells. |
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06:32 | So these circuits or this circuit will a common input from another part of |
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06:38 | hippocampus that will excite parameter cells and will be excited but they will also |
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06:45 | inhibitory cells. And the inhibitory cells in turn can control those already excited |
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06:53 | parameter cells and they can control what of information they're gonna be able to |
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06:59 | of that circuit. Does that Okay cool. So we moved pretty |
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07:09 | well and we talked about the different of the inhibitory cells and how you |
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07:14 | perform these types of experiments and then discussed leo cells, we discussed a |
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07:21 | of de milo Nation diseases actual with conditions. We talked about uh |
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07:30 | We talked about sharks but mary to and periphery. And we talked about |
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07:35 | multiple sclerosis and C. N. . Condition that has to do with |
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07:39 | Myelin Nation. This uh image summarized well all of the cells that we |
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07:46 | about and I think maybe at this I may jump into uh this here |
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07:58 | big review. This image summarized a about glial south and what we think |
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08:06 | and what we know about glial And so this is a great image |
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08:11 | label stuff. If you have it on your note or digitally write down |
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08:16 | a strong side does blood brain Um Synopsis micro glia next to michael |
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08:24 | you can you know activated with You know just notes that we've talked |
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08:30 | the likud undersides, Myelin C. . S. And next to it |
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08:34 | put Swanson smile and P. S. So you know you can |
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08:38 | your notes like this for for studying in some of these slides um you |
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08:44 | see my slides are not worthy. don't like to ride down 20 sentences |
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08:49 | for you to think that which ones these 20 are important to really remember |
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08:53 | the exam but rather to listen and realize what concepts are important. Some |
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08:59 | that we repeat obviously and more important others. Sounds a little bit like |
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09:03 | animal farm. But um okay so is the blood brain barrier that we |
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09:11 | and we discussed it in the light positive control and positive checkpoints that basically |
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09:20 | what enters from the blood into the . The substances that are meant to |
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09:26 | the substance substances that have transporters and there are substances that are unwelcome in |
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09:32 | brain and there are substances that we that get into bloodstream that are |
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09:37 | And we also want to this blood barrier potentially prevent the toxicity in the |
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09:44 | not just the blood. Uh so have the main players and the filial |
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09:48 | with tight junctions the parasites the astra recall that during covid infections if you |
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09:55 | significant inflammation and heavy viral load in blood you will potentially cause breaches and |
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10:04 | brain barrier and will make the blood barrier more susceptible for allowing the virus |
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10:11 | virus to enter. And virus has stew receptors that it can hang on |
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10:18 | and once it enters into the brain it can target glial cells and neurons |
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10:25 | . Okay so we also talked about fact that blood brain barrier is a |
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10:32 | when you're talking about the drugs and if you watch commercials on tv a |
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10:36 | of times somebody is taking an antidepressant it's a commercial for an antidepressant drug |
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10:43 | PTSD and you're hearing that you're gonna diarrhea, you're gonna have abdominal |
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10:50 | you may have abdominal bleeding, you start suffocating uh you may have all |
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10:57 | these side effects and that's because you're trying to get the drugs to treat |
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11:02 | brain. And as I explained, of the drugs we consume are pills |
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11:07 | get broken down through the digestive digestive tract, absorbed into the |
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11:13 | a fraction of what was entered into mouth and smaller fraction getting into the |
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11:19 | . And so what I said is what we want. And thinking about |
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11:25 | drugs and the future of neuro drugs they're small molecules that they're easily crossing |
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11:31 | blood brain barrier that there potentially like so that they can cross through the |
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11:36 | membranes and maybe their self specific to circuit specific. That would be the |
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11:42 | . You know, we know if apply for example, nicotine will bind |
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11:48 | nicotine acetylcholine receptors in the brain and will bind to all of the nicotine |
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11:54 | receptors it can find in the periphery in the brain because it enters into |
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12:01 | blood. But wouldn't it be nice you could actually not only have a |
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12:05 | subtype of the cell but have a receptor and still have the ability to |
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12:11 | that receptor only in sub population of . Okay, because different populations of |
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12:19 | will express different overlapping protein channels receptors such. So that's that's where we're |
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12:27 | with this. So it's impeding you have side effects. So thinking of |
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12:31 | future this is what we have to about designing Really smart um drugs. |
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12:39 | we will talk about neuronal membrane potential . And as we talk about neuronal |
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12:45 | potential, the first thing to realize neurons is that if you take this |
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12:51 | electors that I was telling you about glass micro electors and you say that |
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12:56 | outside of the cell is zero. of also neutral environment. Charge neutral |
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13:03 | you say is grounded zero. And you pluck this electorate from this outside |
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13:10 | that zero through the plasma membrane or a plasma membrane, the number in |
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13:18 | on on the volt meter will show sudden change to about 100 minus 65 |
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13:26 | volts. So the reason why is inside of the plasma membrane is negatively |
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13:35 | and the positive charges accumulated on the of the plasma membrane. Either than |
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13:41 | the fluids further away from the member outside are charge neutral. And actually |
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13:46 | inner core of the side of plasma the cells are also charged neutral. |
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13:51 | the charge is actually accumulated. This separation is accumulated along the phosphor lipid |
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14:02 | . Now we have this charge and also talked about how actions with tom |
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14:08 | is a very fast discharge which is a very fast membrane potential. About |
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14:15 | million volts to sell over one or milliseconds. So you learn what happens |
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14:21 | this to happen for this action potential be generated. But before we learn |
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14:27 | the dynamics and the kinetics of the involved in generating the action potential, |
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14:33 | will review resting membrane potential. Before review resting membrane potential. Let's talk |
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14:41 | the seconds and also take really good . And I'll tell you why because |
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14:46 | gonna involve some of our favorite And if I talk about things two |
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14:50 | three times, that's probably gonna be exam question. Okay, so why |
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14:56 | we need the charge and why do need the discharge and the action |
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15:01 | We need excitable tissues, It's muscle nerve. Why do we need |
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15:07 | We need to react? We need integrate the stimuli. Think very |
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15:12 | But we also have reflexive behaviors just the cart said that the child that |
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15:17 | never seen the fire is gonna extends the fire and withdraw it immediately. |
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15:21 | reflexive. That doesn't take intellect. debate whether this fire is hot, |
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15:26 | gonna burn your skin or not. in this circuit which you have is |
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15:32 | very simple circuit and the spinal So we're going to come back to |
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15:36 | . And we're also going to understand differences between the synapses that are called |
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15:42 | junctions that happened between motor neurons and and also the synapses that are present |
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15:50 | the in the cns. So that's be the second section and we'll come |
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15:54 | to talk about the some of the graded potentials that you're seeing there. |
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15:59 | in general will also discuss this briefly too. Now the circuit that we're |
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16:06 | about is the reflex arch. It's simplest kind of reflex pathway is also |
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16:12 | jerk or patellar tendon reflex. And what is depicted in this image is |
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16:19 | you go for sometimes you and check if your primary doctor is good, |
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16:25 | will do this kind of thing or you complain about something in your mobility |
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16:32 | back or something like that, they send you to a neurologist and neurologist |
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16:36 | perform a simple test. It's a and it's a tap with a little |
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16:42 | . Okay. And it's a tap this patella tendon here. And basically |
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16:49 | response after that tap should be a which of the leg up. |
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16:54 | Should be basically this circuit activated So the cap is the stimulus for |
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17:02 | input that gets picked up by the spindle. These are sensory neurons so |
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17:08 | will pick up that predation and sensory will pick up the mechanical stimulus in |
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17:14 | case. Okay. And they will this information up. And these cells |
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17:19 | dorsal root ganglion cells or DRG Yes. So if your reflex isn't |
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17:28 | then it could be like in this there could be a problem in any |
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17:32 | of those things. Yes, let get to that in just a |
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17:36 | It's a great question. So the neuron will pick up this information and |
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17:41 | sensor in Iran is excitatory and it's to release glutamate it's gonna release glutamate |
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17:52 | it's gonna project. So this is peripheral axon. Remember this is a |
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17:59 | unipolar style. These are great juicy because we talked about bipolar, pseudo |
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18:06 | unipolar salsa. These are pseudo unit house. They have the peripheral axon |
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18:12 | then they have the central axis in central axon. Remember the selma's of |
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18:17 | roots are outside the spinal cord proper this bundle. That's why it's referred |
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18:24 | as a route that looks like a . Ok, It's part of the |
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18:27 | sitting there dorsal root, ganglion, DRG cells and the central axon will |
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18:35 | stimulate or excite with mermaids the cells live in the spinal cord problem. |
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18:44 | just by exciting one motor neuron just exciting one motor neuron here it |
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18:55 | now tell this motor neuron to produce action potential. Okay, so the |
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19:01 | fan goes in information processing happens you this motor neuron now contracting the quadriceps |
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19:10 | extensive muscle. This motor neuron is to the motor neuron. It's in |
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19:16 | neuro muscular junction and the neurotransmitter that uses is acetylcholine. Okay and the |
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19:27 | of the salad is morphological e this self. So now if you have |
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19:36 | contraction of the quadriceps extensive muscle, basically assuring that this reflex is just |
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19:43 | know synaptic 11 single synapse or mono synaptic single synapse involved. Then you |
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19:50 | contraction of the muscle but we all that whenever you contract the muscles the |
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19:56 | you have an opposing muscle and opposing triceps. When you contract the biceps |
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20:01 | triceps is relaxed and vice versa. you contract the triceps the biceps is |
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20:07 | extended. Okay so you have the muscles which is going to extend the |
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20:15 | . That's your quads and you have the hamstrings that are gonna bring the |
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20:21 | back in. Okay. Control how of the knee is allowed to go |
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20:26 | to. All right. So when motor neuron activates this this squadrons of |
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20:32 | contracts but that's not the only thing happens. In fact in order to |
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20:37 | this reflex effective and fully functional. also need to relax the hamstring. |
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20:45 | the hamstring needs to be relaxed in for this to contract and move your |
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20:49 | fast. So this circuit goes at some sensory neurons apart from contacting the |
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20:58 | motor neurons here they also contacted inhibitory neurons and they inhibit the inter neurons |
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21:05 | the spinal part are also multipolar cells the neurotransmitter that they release everybody don't |
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21:13 | gaba it's glycerine and that's an exception the C. N. S. |
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21:19 | the spinal cord and the C. . S. Neurons release Yabba Castle |
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21:27 | the spinal cord into neurons release glycerine a major inhibitory neurotransmitter difference and you |
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21:36 | know this difference. So now when inhibitor into neurons are activated. So |
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21:42 | this sensor neuron excites inhibitor interneuron, inhibitor interneuron is going to release glycerine |
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21:50 | this girl I seen instead of exciting flexor motor neuron inhibits the flex of |
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21:56 | neuron and by inhibiting the flux of neuron it allows for this muscle to |
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22:03 | . So there's no contraction there, inhibited and it's relaxed. It allows |
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22:09 | for the quadriceps muscle to effectively pick the lag and perform this patella tendon |
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22:16 | arch reflex. So you have the sensor information. The parent information is |
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22:23 | the spinal cord into the periphery. that's your parent neurons apparent versus another |
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22:34 | . Mama synaptic a single synapses enough contract this muscle. But policy synoptic |
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22:42 | or more three is really necessary for circuit to function properly completely and for |
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22:49 | reflex to function properly completely. Getting to your question, what if there |
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22:55 | a problem and the patient is sitting and the doctor has to bring like |
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23:01 | sledgehammer and the leg is still not . What is the problem? So |
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23:06 | start guessing what the problem is? know what if what if light tap |
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23:11 | do it but heart attack doesn't. heart attack may indicate well maybe there's |
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23:16 | dysfunction and sensory neurons it's one thing maybe there's too much inhibition. So |
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23:23 | there was too much inhibition then this be always relaxed. Always relaxed. |
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23:28 | you can start looking at is it always relaxed. There is some deductive |
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23:35 | can be done by observing this but after not seeing a normal reflex, |
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23:43 | would have a look at it and you know they may start looking a |
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23:48 | bit deeper into the spinal cord or like that. It could be associated |
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23:52 | the pain that could be associated with nerve and the leg and and it |
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23:58 | be associated with the circuit and which of the circuit. Yeah but it |
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24:03 | give you a clue. It does you a clue. And and like |
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24:07 | said good doctors even uh um primary physicians often do this and there's something |
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24:15 | often do it for Children too because need to check their you know the |
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24:18 | of the eyes and legs and feet all of that. So okay so |
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24:23 | three types of cells in here. their neurotransmitters whether their projection cells or |
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24:28 | they're into neurons. And how the between mono synaptic policy synaptic service. |
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24:35 | neurotransmitters. So the sensory neuron synapses the extensive and that's where just released |
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24:45 | good in it will be released on neurons. It will excite them and |
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24:49 | into neurons that will excite them But those into neurons instead of releasing |
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24:56 | on the opposing muscles release glycerine which inhibit and relax this muscle. The |
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25:03 | basically means it just stays still. not contracting. It's relaxed and |
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25:13 | One has no stimulation of the Yeah, but it's still this one |
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25:18 | expresses and will release acetylcholine. Because you also need to do a |
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25:24 | of this, you need to put leg back you know and relax |
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25:29 | So this is just one direction. if you need to extend it will |
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25:35 | in this way. But if you to flex this will get inhibited and |
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25:39 | will get excited. And of course all of it is we're not talking |
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25:46 | reflex. There's no reflex to check back circuit. Is your head giving |
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25:51 | motor command and the ability for you do these things. But when we're |
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25:55 | about the reflexes just to kick up it would be the same neuron, |
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26:00 | would just have a different somewhere They're not. Or would it be |
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26:06 | different neurons and probably different neurons and synapses. Yeah, good questions. |
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26:16 | always most of the policy synaptic grief , we have to involve inhibitor synopsis |
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26:25 | kerosene policy synaptic excited to uh I'm not certain if there are excitatory |
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26:33 | synaptic reflex. And this when you about reflexes, like other complex reflexes |
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26:42 | you're mentioning like for example gagging reflex a complex reflex but it's a |
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26:47 | Something is toxic and pleasant. You and it activates you know, many |
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26:52 | synapses. So that's like complex, know complex really complex reflexes. Uh |
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26:59 | it's just by definition because its policy africa is complex so but it's not |
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27:04 | complex. So I was excited to um in code analysis we also |
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27:18 | Hmm. So yeah, if I'm your question correctly, so if for |
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27:27 | , if you want to stimulate the with the light, you're gonna go |
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27:32 | red land to thalamus once announce, actually you're gonna go through about three |
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27:39 | in Radnor 1 to 3rd and they're and some of them will be inhibitor |
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27:45 | the excitatory goes out of the retina going to go to thalamus from thalamus |
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27:50 | gonna go through the primary cortex. it's already you're talking about for |
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28:00 | yes, if you want to send long ranges you're gonna have all the |
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28:04 | excited three circuits or networks that are processing and sending that information from one |
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28:12 | to another from one place of the and another. Alright, so let's |
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28:20 | for the reflex that is mediated for by the autonomic nervous system, is |
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28:27 | the amount of while this is a of sensory nervous, this is mediated |
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28:34 | the circuit by the peripheral, you , you're gonna involve the conscious perception |
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28:42 | us but you won't be able to to stop it. Maybe you can |
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28:49 | stop that. Like if you're sitting , somebody started because you're gonna be |
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28:53 | by keeping this tight. So it's could obviously have a conscious control and |
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29:00 | have a conscious perception of this with fact of the matter is a lot |
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29:03 | things can happen at the level of spinal cord, Oh, reflexively or |
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29:12 | inhibited neuron bundle, I guess they're many synapses in the or summer inhibitory |
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29:19 | excitatory. And it's like a spatial of whether it's uh well, one |
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29:31 | about the circuit is a very reliable . Maybe we should re examine that |
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29:36 | . We talk about the cortical it's going to be more applicable. |
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29:40 | is really more kind of a triangle the class, understand that there's a |
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29:44 | circuit with one or few synapses. hang on to that thought and hang |
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29:49 | to that question. Now, of they'll have multiple synapses. And is |
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29:53 | an inhibitory driven inhibition? Probably to small extent. But the reason why |
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30:00 | circuits is our reliable and why they're is the output is gonna be |
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30:05 | It's gonna be a huge graded potential inflate potential in your muscular junction that |
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30:12 | generated. We'll talk about it again the next section. So, hang |
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30:15 | to some of these thoughts because you'll maybe understand it a little bit better |
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30:20 | the next few lectures to uh so very reliable and a action potential in |
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30:29 | motor neuron means of twitch of a . So this neuro muscular junction, |
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30:35 | synapse here is a very reliable, fidelity. 1 to 1 I called |
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30:40 | , okay, not so in the but we'll talk about it in a |
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30:45 | of lectures. So let's a little talk about what's in the brain. |
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30:48 | in general it's water, water And then some towns don't have |
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30:55 | Oxygen attracts extra electrons and has negative . Hydrogen has net net positive |
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31:03 | It's held by Covalin bonds. It's polar molecules like ions souls, it |
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31:11 | dissolve ions are atoms or molecules that a net charge, positive net charge |
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31:19 | one. The difference in the number protons and electrons, its ion valances |
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31:25 | plus one is a positive charge or on minus one is negative charge or |
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31:32 | ion plus two is a positive Also kati on but it's di vale |
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31:39 | cat eye on. So you can minus one -2 to plus. |
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31:45 | so this is for example, sodium which is surrounding the cells. And |
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31:50 | basically surrounded by water. And you the plasma membrane. The plasma membrane |
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31:58 | we talk, is consisting of the lipid bi layer and ions that are |
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32:03 | the side of plasma. And ions are on the outside of the cells |
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32:07 | freely pass through the phosphor lipid bi . So they need to have channels |
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32:14 | these channels will control how much of major ions are going to be sequestered |
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32:20 | the inside of the membrane versus the of the membrane. The main players |
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32:25 | the resting membrane potential. And you'll learn an action potential but in the |
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32:31 | membrane potential. the sodium potassium and very small extent chloride, the fourth |
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32:42 | important ion that is shown here is . And it's not shown because it |
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32:48 | much to the resting membrane potential. it is shown because these four ionic |
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32:53 | are the most important for resting membrane or action potential and also for activation |
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33:00 | some intracellular processes by calcium. Because is not only an ion inside the |
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33:07 | , it's also a secondary messenger and can have downstream down inside the cells |
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33:16 | processes that can activate other highnesses and associated with calcium that can even alter |
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33:25 | transcription mechanisms and transcription outputs of the . So, calcium is also very |
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33:33 | ion. And finally we have here potassium pump And with this shows actually |
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33:42 | come back to this in a What this shows is that there is |
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33:47 | distribution of these ions on the outside the cell versus the inside of the |
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33:53 | . And so if you drop this again on the inside of the cell |
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33:57 | measure the difference between the outside of cell to the inside of the |
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34:01 | you will see approximately minus 60 to 75 million volt resting membrane potential. |
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34:10 | when we start talking about these dynamics memory potential action potential. I also |
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34:16 | some drawings that I've done myself. add these slides are already on the |
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34:22 | notes. A lot of these slides I talk about things. But quite |
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34:29 | there's a question to wrestling. So is wrestling member in paternity -60? |
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34:34 | is it -75? Or is it in between? The answer is |
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34:41 | Everything in between. Why? Why 60 to minus 75? In fact |
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34:48 | 55 to minus 90. Why? , fluctuate over time? Well, |
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34:57 | a wrestling member and potential. but there's species of cells it's fluctuating |
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35:02 | there are species of cells that will around -75 and others around -60. |
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35:09 | that's because yeah, good thinking. not exactly. It's because they will |
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35:21 | have a different composition of the ion of the possible number and expresses and |
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35:28 | charge of the inside versus the outside dependent on the permeability through these ion |
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35:34 | . And these ion channels could be different splice variants and different subtypes of |
|
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35:39 | . And so the kinetics might be and they'll let in more ions and |
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35:44 | instances less ions. Some cells can more d polarized wrestling number and potential |
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35:50 | 55 minus 60. And other cells have more hyper polarized numbering potentials minus |
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35:57 | minus 80. That's for neurons and wrestling member and potential is minus 90 |
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36:04 | gallons. And you understand that in next two lectures so don't uh don't |
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36:09 | ahead of yourself and thinking well how that happen? But the important thing |
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36:13 | not to get hung up On the range I'm gonna be lost. Because |
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36:20 | will talk about reversal potentials but we'll about certain values and the values that |
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36:24 | gonna ask you to know are the that I'm going to present you in |
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36:28 | slide because in some textbooks will say number of potential is -65 and give |
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36:35 | the same formula for calculating it. others will say it's -70 -75. |
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36:41 | cellular environment is slightly different to in instances there might be slightly higher concentration |
|
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36:47 | sodium chloride in some instances potassium but general everything is under home a static |
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|
36:54 | . And glia are really good at some of these inequalities in in in |
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37:04 | concentrations which is ultimately means charge or in the neurotransmitter concentrations, fluctuations of |
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|
37:12 | concentrations. What you were saying is different cell types, right? Is |
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37:18 | also a range within one cell type on inhibition or excitation. So wrestling |
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37:24 | of potential is not a set it fluctuates it's like a random walk |
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37:29 | it doesn't deviate too far beyond like mill levels. If it deviates to |
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37:34 | , it will produce some action potential it does have to do with inputs |
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|
37:38 | in some constant excitatory inputs not constant some inhibitory input, some stronger inhibitory |
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37:45 | and stronger excitatory inputs. Yeah, a constant, it's a constant flux |
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37:49 | activation of difference and access. And if you reach the pressure will produce |
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37:54 | action potential. But that wrestling number potential will never be one value. |
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|
37:58 | know when you see a flatline in , bad news. You don't want |
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38:05 | see it on anybody's monitor flat you don't want to see a |
|
|
38:08 | there's nothing that's bio thermal biological, no flat line. So the temperature |
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|
38:15 | fluctuate around 76 but it will not always 76.0 77 78 80 goes down |
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|
38:25 | body temperature same physiological. 36 37. You got a little |
|
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38:32 | you know, 37 a half, know fever, 39 Celsius. So |
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38:37 | it's a number of potential is also . It's what we call a random |
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38:43 | will come back to that concept to affecting expression of the affecting the |
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|
38:59 | Does that change expression? Um but then you were talking about like |
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39:09 | pathology, everything is fairly balanced and this home in a static control and |
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|
39:15 | we are most of us, you like emotionally contained smart but we you |
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39:23 | have deviations and such. You we have geniuses and savants and you |
|
|
39:31 | pathologies too. So it's a little . Let's review the major building blocks |
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|
39:40 | the cells. Me no assets. that? You need some of them |
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|
39:46 | ones. You need to eat them get in your body and then you |
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|
39:53 | some others. And this amino They form these bonds here and they |
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|
40:01 | themselves together as the primary structure of amino acids. And they banned themselves |
|
|
40:07 | into these polyps peptide structures that in structures can become like helix is like |
|
|
40:16 | corkscrew girl and secondary structures that can the sheets a lot of times. |
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|
40:21 | hear beta sheets and the proteins that laid okay tertiary structures and there's coils |
|
|
40:27 | their sheets could be placed in this sub unit structure and then a protein |
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|
40:37 | for example or even a trance membrane coupled receptor protein will be comprised of |
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40:46 | subunits. So then you have the ordinary structure and you will form these |
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40:54 | channels for each ion that we talked the sodium and the potassium ions and |
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|
41:00 | will be selective. So what are of the features of the ionic |
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|
41:06 | First of all, some of them very reliable and can conduct. A |
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41:13 | of ions can allow the passage of lot of ions such as in the |
|
|
41:19 | junction with acetylcholine receptors. Some of processes and styles are slower. So |
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|
41:26 | you talk about N. A. . Or sodium potassium 80 P pump |
|
|
41:31 | . T. P A. They're slower. We won't conduct or |
|
|
41:35 | will not allow for the transport of and potassium only about 100 iles per |
|
|
41:42 | . So they're slower. So again have some fast processes and channels that |
|
|
41:49 | capable of conducting a lot and large and you have some channels that are |
|
|
41:54 | and they are not capable of conducting much. And they also have their |
|
|
41:59 | . So channels are selective filters and one of these species, sodium potassium |
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|
42:09 | chloride have their specific channels. So do you when it's surrounded by |
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|
42:16 | Some hydration on the outside of the will enter into the south and it |
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|
42:22 | get stripped of the waters in an of getting stripped off the waters inside |
|
|
42:28 | sodium selective channel there is a negatively amino acid residue. We just talked |
|
|
42:36 | amino acids building blocks. Some of will have positively, some of them |
|
|
42:40 | have negatively charged amino acid residues. a very microsecond interactions. Now the |
|
|
42:48 | interactions with this charged polar group. this interaction allows for the sodium to |
|
|
42:57 | of stick to the wall of the and then get propelled into the inside |
|
|
43:04 | immediately gets rehydrated. Again. Now the cytoplasmic environment. So sodium is |
|
|
43:13 | off the waters my amino acid residues enters inside with larger diameter, potassium |
|
|
43:21 | strapped and sent back out so larger cell doesn't fit through the innermost channel |
|
|
43:33 | tries to commend but this interaction and size stops it. So does that |
|
|
43:41 | then potassium channel is gonna have to a bigger opening. Gas. Does |
|
|
43:46 | mean that smaller islands can pass. just a bigger opening. The question |
|
|
43:52 | , how selective are they based on and they're quite selective because if you |
|
|
44:00 | smaller ions will have a stronger attraction water. So they will actually be |
|
|
44:07 | by bigger clouds of these waters of . Number one, then there is |
|
|
44:12 | cell activity as it is specifically, know, related to these amino acid |
|
|
44:19 | . Number two. Number three. rules can be broken. Which means |
|
|
44:25 | at some point, yes, if is some pathological condition, if there |
|
|
44:31 | over excitability, even if it's transient a lot of excitability, there might |
|
|
44:38 | a breach of selectivity and everything maybe everything as long as the size |
|
|
44:46 | Mhm. But in general, the physiological conditions, These selective ion channels |
|
|
44:55 | sodium will patrol sodium potassium will patrol chloride will patrol chloride and it |
|
|
45:01 | instead of having a negatively charged amino residue and chloride channel chloride as a |
|
|
45:08 | and ion chloride -1, it will a positively charged amino acid residue. |
|
|
45:14 | may have the amino acid residue in different locations. Which also will influence |
|
|
45:22 | much ions or the kinetics of that , how much ions can flow through |
|
|
45:26 | channel or how long it can be , for example. So, we |
|
|
45:29 | the selectivity. It's like molecular It's not purely based on size, |
|
|
45:35 | size of this. It but it's it's it's dependent on science. For |
|
|
45:42 | . So now let's review some of basic things that you've learned a while |
|
|
45:48 | um swan d equals Ir where Is voltage and vaults and relevant scale |
|
|
45:57 | neurons. Miller vault so minus 65 volts 100 million volts neurons. This |
|
|
46:05 | the scales for neurons I is current amperes and from neurons irrelevant scales or |
|
|
46:12 | amperes and PICO amperes, resistance is is our arms. And because neurons |
|
|
46:21 | very small, just 10 microns in in general they have high resistance and |
|
|
46:27 | relevant scales and mega arms or neurons , conductance is the inverse of resistance |
|
|
46:37 | over r and conductance and cements the scales for neurons is PICO and nano |
|
|
46:46 | . And that relates to the conductivity single channels. Or overall conductivity through |
|
|
46:52 | whole south as a sum of all these single channels. Easy stuff. |
|
|
47:00 | good questions also. And also don't this very simple switcheroo here because it |
|
|
47:09 | keep coming up when we talk about concept of the driving force a little |
|
|
47:14 | later, probably next lecture now. here let's remind ourselves it's like we |
|
|
47:20 | this possible lipid bi layer here and we have sodium and chloride on one |
|
|
47:26 | and we have no channels and sodium chloride will just stay on that |
|
|
47:29 | So for it to to start flexing the sodium and chloride to start flexing |
|
|
47:35 | have to have a sodium channel. like the sodium chloride chloride channel and |
|
|
47:40 | will start flexing until through simple diffusion was just based on the concentration, |
|
|
47:47 | will reach equal concentrations on on both . So it was just purely based |
|
|
47:56 | the concentration, it would do that and flora, but it is not |
|
|
48:05 | based on the concentration, it's also on the electricity and the electrical |
|
|
48:10 | Its voltage, voltage and differences and in voltage is what's gonna drive ions |
|
|
48:19 | plasma membrane inside or outside. And you look at it, you have |
|
|
48:25 | battery. The negative end is a and cat ions are gonna be attracted |
|
|
48:32 | cathode and chloride which is an ion going to be attracted to positive and |
|
|
48:39 | ode. So you have apart from concentration gradient, you have electrical potentials |
|
|
48:47 | ions have charged plus 1 -1 to and so on. So separation of |
|
|
48:55 | across the plasma membrane here that we're negative charge accumulated on the inside is |
|
|
49:01 | difference between the voltage on the inside the outside is the membrane. A |
|
|
49:07 | of times you'll see abbreviation D. . VM addressed -65 million balls. |
|
|
49:13 | means membrane potential address -65 million bowls is the same as inside the current |
|
|
49:22 | . Just by definition is in the of the net movement of the positive |
|
|
49:26 | . So and ions move opposite because negatively charged and catan moved in the |
|
|
49:35 | same direction If you reduce the charge plasma membrane, that means that the |
|
|
49:42 | of the membrane is becoming more positive -40, maybe zero. That is |
|
|
49:48 | deep polarization. Your d polarizing the of the number. If you make |
|
|
49:54 | plasma membrane on the inside more you accumulate more negative charge on the |
|
|
50:00 | here, you're causing hyper polarization and arresting number. And potential from minus |
|
|
50:05 | can slide down to minus 70. does happen because of the synaptic activity |
|
|
50:13 | that does happen because of the thermodynamics local micro thermodynamic fluctuations. The warmer |
|
|
50:21 | stuff the faster things move. Okay and if you have a slight difference |
|
|
50:27 | the in the temperature across brain circuits this could be a small effect on |
|
|
50:33 | on the speed. So now when talking about ions because I am so |
|
|
50:44 | ions have what is called an equilibrium I think maybe it's hidden underneath |
|
|
50:51 | The equilibrium potential for e. Ionic E stands for equilibrium or an |
|
|
50:58 | Each ion potassium sodium fluoride calcium will its own equilibrium potential. Now that |
|
|
51:07 | potential best explained, is with this . So we have the potassium and |
|
|
51:14 | have some negatively charged sodium and we a potassium channel. So potassium can |
|
|
51:22 | from this inside of the south to outside of the cell. But this |
|
|
51:27 | is trapped there and it's keeping a bit of negative charge from the inside |
|
|
51:31 | the cell. So potassium from its concentration. The large K. Plus |
|
|
51:37 | means a lot of potassium concentration but lot of positive charge two on the |
|
|
51:42 | side K plus starts flowing its concentration that's driving to flow to the opposite |
|
|
51:49 | through this open potassium channel. this concentration doesn't equal out on both |
|
|
51:58 | because as potassium ion starts leading the and accumulating on the outside of the |
|
|
52:06 | membrane, the positive charge of already potassium will start turning away more potassium |
|
|
52:15 | that it will never reach equal molar of both sides because this positive charge |
|
|
52:22 | start repelling its own positively charged Which is basically the moment at which |
|
|
52:33 | difference at the plasma membrane is diffusion forces which is concentration forces and electrical |
|
|
52:43 | are equal to each other. The will forces still have more concentration of |
|
|
52:49 | saying go go to the other go, but the electrical charge selling |
|
|
52:56 | I have too much of positive I put resistance to you and at |
|
|
53:02 | point the two forces are equal to other. They're opposite in direction to |
|
|
53:07 | other. That's the equilibrium potential and that point there is no net |
|
|
53:14 | meaning there is no more potassium flexing the right or to the left. |
|
|
53:18 | may still be flexing through open channels that's normal biology and thermodynamics but there |
|
|
53:23 | gonna be net ionic movement toward one or the other side because it is |
|
|
53:29 | this equilibrium potential. So these are potentials have values for all of the |
|
|
53:36 | of interest for us. The other that's really interesting is that each equilibrium |
|
|
53:43 | will have its own value and its force. What we call driving force |
|
|
53:49 | that ion will depend on its equilibrium and also the difference between that equilibrium |
|
|
53:57 | and the membrane potential overall. So on with that thought. The explanation |
|
|
54:01 | coming in the next two slides, there are any concentrations are known, |
|
|
54:09 | can calculate the equilibrium potentials. An with potassium is not unique to |
|
|
54:16 | This is just replay the same with . A lot of sodium on the |
|
|
54:21 | . Oh there's a lot of potassium the inside. There's a lot of |
|
|
54:25 | florida on the outside, there's a of sodium on the outside have this |
|
|
54:29 | charged on the podium can across the , sodium starts going through the channel |
|
|
54:36 | also never reaches the equal model The size here again indicates the concentration |
|
|
54:43 | the charge here indicates the charge build . Okay, so it's the same |
|
|
54:49 | . That is the moment where you the equilibrium potential or so do I |
|
|
54:56 | also use this term reversal potential or potential interchangeably. And you'll also understand |
|
|
55:04 | I use that term uh because of training in part but also because of |
|
|
55:09 | biology. So you have uneven distribution charge and each one of these ions |
|
|
55:16 | a certain concentration. So you have little bit of the potassium on the |
|
|
55:21 | of the cell. And a lot the potassium on the inside of the |
|
|
55:25 | , you actually have 20 times more on the inside of the cell than |
|
|
55:29 | outside. That's the ratio. And potassium equilibrium potential value. Noticed that |
|
|
55:37 | C, which is physiological temperature. this is an important term in calculating |
|
|
55:43 | equilibrium potential temperature term. It's minus million volts. Is the reversal or |
|
|
55:50 | potential for potassium, sodium on the hand, is abundant on the outside |
|
|
55:56 | the south, there's a lot less on the inside of the south. |
|
|
56:00 | there's 10 times more sodium on the than the inside. And sodium equilibrium |
|
|
56:07 | is positive 62 million volts. It's positive 55 million bolts and some books |
|
|
56:12 | positive 52 metal bolts and other But it's way way up different |
|
|
56:18 | higher value. And you'll understand why calcium very little on the outside. |
|
|
56:27 | , a lot of it on the , a lot of calcium on the |
|
|
56:31 | , very little calcium on the inside the inside. You can't have a |
|
|
56:36 | of free side of solid floating calcium as I mentioned, it's not only |
|
|
56:40 | secondary, it's not only an it's also secondary messenger. So you |
|
|
56:47 | much control the amount of calcium. it also shows you that there's 10,000 |
|
|
56:53 | more calcium on the outside of the than the inside of the cell. |
|
|
56:57 | as far as the concentration gradient calcium is the big big winner |
|
|
57:04 | And the disparity of the concentration of on the outside versus the inside. |
|
|
57:11 | is also abundant on the outside of south about 11 10 times more. |
|
|
57:17 | on the inside of the south and that calc has positive also equilibrium potential |
|
|
57:24 | chloride has a negative equilibrium potential. chlorides negative equilibrium potential is somewhat close |
|
|
57:30 | the resting membrane potential overall which we discuss in the next couple of |
|
|
57:35 | So let me see if I can through this quickly here. Last thing |
|
|
57:39 | I want to say here is the . If you recall A D. |
|
|
57:44 | . And A K palms they work concentration gradients always in the same |
|
|
57:50 | And they use energy 80 P. you chew up the energy. So |
|
|
57:54 | lot of the energy demand in the is to keep up those pumps going |
|
|
57:58 | keeping the homeostasis and keeping the resting potential to its values of approximately negative |
|
|
58:06 | negative 70 million balls. So how calculate the norms potential. And on |
|
|
58:12 | exam you will not need a calculator the exam. You will need to |
|
|
58:19 | the important terms in this equation No ernst equation and important differences in |
|
|
58:27 | concentrations of ions on the outside versus inside. You can remember it by |
|
|
58:32 | molar concentrations 5 to 1 50 or can remember it by ratios is 10 |
|
|
58:38 | more sodium. 15 times more of and so on. So to calculate |
|
|
58:44 | earth equation. You have E I this is what we're calculating equilibrium forgiven |
|
|
58:51 | which is in the equation. 2.303 key over Zf cons log of ion |
|
|
58:59 | on the outside of the south Ion concentration on the inside of the |
|
|
59:04 | . R is the gas constant. . Is the absolute temperature. That's |
|
|
59:08 | I said that temperature is an important for calculation of the equilibrium potential. |
|
|
59:15 | is the charge of the ion. surveillance of the ion F is the |
|
|
59:20 | day Sir electrical constant log is based algorithm. So remember that equilibrium is |
|
|
59:30 | balance of two influences diffusion or which puts us an on balance concentration |
|
|
59:36 | electricity which causes an ion to be to opposite charges and repelled by the |
|
|
59:42 | by life charges, increasing thermal energy each particle, increases diffusion and will |
|
|
59:49 | increase the potential difference achieved at Thus, equilibrium of ion is proportional |
|
|
59:56 | T. Temperature. E r T is constant. Therefore uh on the |
|
|
60:07 | hand, increasing the electrical charge of particle will decrease the potential difference needed |
|
|
60:13 | balance diffusion. The increase of electrical . The difference so Z if Z |
|
|
60:23 | two then you're decreasing. Therefore e is inversely proportional to the charge of |
|
|
60:30 | of the ion. We need not worry about our enough in the first |
|
|
60:35 | because their constant the body temperature is . I said that fluctuates too. |
|
|
60:40 | have fever. You know if it's and four F, that's 42 |
|
|
60:47 | 43 Celsius, that's danger zone. zone that zone. Um So body |
|
|
60:54 | and this equation for these important. let me walk you through this |
|
|
60:58 | So for potassium ion, what we is first of all this term here |
|
|
61:06 | . R. T. Temperature 37 constant third a constant Z. Take |
|
|
61:15 | valence for potassium ions. It all into 61.54 and the term is Mila |
|
|
61:24 | . So all of that can basically our TCF into 61.5 million bells log |
|
|
61:34 | . Based on log potassium on the O. is for the outside of |
|
|
61:39 | cell versus potassium on the inside Of the south. And so for |
|
|
61:48 | , you plug in our T. . Same for R. T. |
|
|
61:55 | as uh And the difference big difference the concentration of the sodium is much |
|
|
62:05 | on the outside versus the inside. is what's gonna be distinguishing the positive |
|
|
62:11 | negative equilibrium potential values chloride. Same here. The same collapse 61 5423 |
|
|
62:19 | three are TCF except dizzy is negative is negative, giving us -61.54. |
|
|
62:29 | follows this. Huh? Here we in council calcium doesn't give us 61 |
|
|
62:38 | because as we collapse this into the of all these term we're having Z |
|
|
62:45 | plus we're dividing it in half. so you get actually half of that |
|
|
62:51 | in positive terms. So the ions as you can see they will have |
|
|
63:03 | their own equilibrium potential. That is much determined by the valence and very |
|
|
63:10 | determined by the charge positive versus And the concentration outside versus inside. |
|
|
63:18 | we continue with this formula we said there is 20 times more potassium on |
|
|
63:23 | inside versus the outside. That's where get 1/20 or you can plug in |
|
|
63:30 | over over 100 Or 1/21. Doing calculation again, you will not have |
|
|
63:38 | do it but you have to know values in these terms. So 1/20 |
|
|
63:43 | of 1/20 is negative. 1.3. you take this portion here which is |
|
|
63:51 | 1.3 and multiply by 61.54. And have the calculation of the equilibrium potential |
|
|
63:59 | potassium right? And you can run the same thing for sodium. And |
|
|
64:07 | you run for the same thing for now, N. A. On |
|
|
64:11 | outside, you can plug in A. On the outside is 1 |
|
|
64:17 | on the inside is 15. Or can use the ratio of 10 to |
|
|
64:23 | . Right. And what you will is that the value for sodium equilibrium |
|
|
64:31 | now is positive 62 million girls. by knowing, you know obviously the |
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64:37 | of the constant temperature was setting at but by knowing the valence changes in |
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64:44 | charge, the valence degree and the outside on the inside of the log |
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64:50 | and scale is what allows us to it to calculate individual equilibrium potentials for |
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64:57 | individual ions. However, and I know, maybe it will answer your |
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65:03 | . However, the member in potential not just one eye on I said |
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65:08 | this membrane possibility it is surrounded by potassium have a lot of it |
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65:13 | a little bit of it here. that means other ions are involved in |
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65:18 | the overall number of potential. Because equilibrium potential for one ion is |
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65:24 | that one ionic species for sodium equilibrium potential for potassium. And the |
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65:31 | for that equilibrium potential for calcium, potential for chlorate equilibrium potential. Individual |
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65:38 | membrane potential is determined by interactions of ions and mostly by sodium and |
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65:48 | And if you want to you can to this equation also chloride but you |
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65:53 | see much difference when you're calculating the and potential in this case using the |
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65:58 | equation golden equation is pretty much the as this abbreviation here. 2303 |
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66:07 | T. Z. F. You have the log base, you still |
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66:13 | the concentrations of potassium on the outside potassium on the inside. The difference |
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66:21 | is that instead of calculating it for ion, you're taking into account concentration |
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66:28 | of another island sodium and outside versus . And the other key term here |
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66:36 | P. K. In this case not like a P. K. |
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66:39 | values permeability. How permeable is the membrane to potassium versus sodium. You |
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66:49 | in the next lecture that at the of the action potential, plasma membrane |
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66:54 | mostly permeable to sodium is dominated by coming in and when the action potential |
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67:01 | going down to resting membrane potential level dominated by potassium leaving the south coming |
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67:08 | of the south. So the permeability change however, addressing member and potential |
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67:16 | membrane potential is dominated and most permeable potassium. This is the T. |
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67:25 | . Value. 40 times more permeable potassium versus sodium. And why is |
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67:34 | ? Because this is just what's happening neurons, neurons have potassium channels and |
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67:41 | channels are leaky and potassium is you see oozing out slowly of the neurons |
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67:49 | potassium channels at wrestling member and These are the most permeable channels and |
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67:55 | have a lot of potassium inside the . Therefore it's very much dominated by |
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68:03 | membrane and equilibrium potential. This resting potential is much closer in value to |
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68:13 | negative 80 value potassium equilibrium potential and 62 value of sodium delivering potential. |
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68:20 | in general in order to derive the Patan trow which is B. |
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68:27 | You have to incorporate at least sodium potassium and you can if you want |
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68:31 | chloride and you have to include the ratios of permeability values for each individual |
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68:40 | . And those p values will change the member and fluctuates and it receives |
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68:45 | and negative inputs. There's p values values where different islands will change and |
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68:51 | will also change dependent on the channel and specific structure that these channels |
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69:00 | So I believe I was actually gonna here today and maybe take one more |
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69:08 | and I want to save this Um So one more question. And |
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69:15 | if you guys have any questions, questions come up after after class ability |
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69:25 | the ability will be influenced by the of the channel and the Connecticut. |
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69:31 | channel, no leaky channels are not same as voltage gated channels, which |
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69:41 | learn about next election. So hang to these questions are great questions. |
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69:47 | are voltage gated channels. We'll talk them about them. Uh As I |
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69:54 | , the flux defiance is dependent on voltage and charge across. But hang |
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70:00 | to that question. That's a great for next lecture because we'll talk about |
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70:03 | compassion and how they play into the potential And the kinetics of those |
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70:08 | Alright, thank you very much. questions today. Really appreciate it. |
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70:14 | had a quick question about the cost exams. Are they going to be |
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70:18 | in person at the casa buildings? that what you talked about in |
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