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00:02 | this is lecture five of neuroscience. what we started discussing in the last |
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00:07 | lectures and we will continue discussing along same themes throughout the course was different |
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00:14 | of neurons and glia. So we about neurons or about two lectures and |
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00:18 | said that there are different ways in we can distinguish different subtypes of |
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00:24 | We talked about morphology, their morphological . And we'll talk about some of |
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00:28 | cells that are on this diagram Today talk about dorsal root ganglion cells and |
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00:34 | talk about motor neurons that are shown . Uh morphology is not enough because |
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00:41 | of the cells look alike morphological really the same layers or the same areas |
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00:48 | circuits of the brain but there's still different subject. And so we talked |
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00:54 | the fact that there's other ways in we can distinguish different subtypes of cells |
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01:01 | their projection cells which most of the cells overwhelmingly excitatory parameter cells or where |
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01:08 | local network into neurons that are inhibitory have Gaba in cns is the major |
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01:20 | . They also have self specific markers that's a lot of times it will |
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01:24 | you distinguish the self subtype that looks same and that even fires these action |
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01:30 | that we described as a dialect that the same pattern of action potentials but |
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01:35 | can be distinguished by the substance. is neurotransmitters, neuro peptides, calcium |
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01:41 | proteins that one cell expresses that looks same and fires the same and then |
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01:46 | cell doesn't which also is a functional for at least the cellular signaling inside |
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01:51 | cells which makes those two cells a subtypes of cells of neurons. So |
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02:00 | spent quite a bit of time on circuit. And the take home message |
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02:05 | you have to know from the circuit not necessarily the names of the markers |
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02:10 | CD or PV. But the general that you have this three layered structure |
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02:16 | is in the campus when we go the neocortex is going to be six |
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02:21 | into connectivity that we'll discuss in the and outputs are gonna be more complex |
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02:27 | we're discussing here. But in the , what happens is that in the |
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02:33 | we have these diverse subset of inhibitory , 21 different subtypes of inhibitory cells |
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02:39 | the local inter neurons that will dictate will control the output of these |
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02:46 | excited ourselves. This projection excited will project out of campus to other |
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02:52 | of the brain, communicating the information is being processed in this network and |
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02:58 | control of that communication that goes out much is dependent on the activity of |
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03:04 | surrounding inhibitory cells. These inhibitory cells these excitatory parameter cells will actually receive |
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03:12 | same farmer excitatory input. So there's to be excitation. It's not like |
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03:18 | of a sudden there's some spontaneous activity this circuit of the hippocampus is a |
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03:22 | prominent excitatory input. It's gonna come and it's going to excite inhibitory cells |
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03:30 | inhibit ourselves get excited. They start other cells because they start releasing gaba |
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03:37 | the excitatory cells are excited they excite the cells. They start releasing glutamate |
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03:43 | they start communicating that information to the networks. And so once these cells |
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03:50 | the common input then you have a dialects in which that common input gets |
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03:56 | in the output by the inhibitory cells finally deciding whether excitatory cells are going |
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04:03 | pass that input projected onto the interconnected of the brain. And that's pretty |
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04:11 | all you have to know. Three structure the rabbit hole, south livin |
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04:15 | criminality 90% and they're boring because they have intracellular marker that distinguishes them but |
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04:23 | else. And aspires morphology or So in this next slide and I |
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04:34 | that cells can receive the same input they will produce a different pattern of |
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04:39 | and that pattern of output the action . And if we look in the |
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04:46 | regions of the brain and we actually to insert the electrodes are recording electrical |
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04:56 | from another subset. This is a . What I described is especially these |
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05:03 | inter neurons are going to produce complex different patterns of action potential output which |
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05:11 | call a dialect of the south, languages action potentials but how you speak |
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05:16 | language very much depends on different sometimes . We need that complexity because we |
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05:23 | complex frequencies affecting our visual inputs. have sensory auditor information coming in. |
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05:31 | frequencies Have some out of sensor information is car vibrations can be very slow |
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05:38 | can be very fast and this is different frequencies that are still being perceived |
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05:42 | the brain and processed by those And some of the cells will be |
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05:47 | fast. The fastest into neurons in brain can fire 600 action potentials a |
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05:54 | 600 hertz. That's super fast. then there are some others that fire |
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05:59 | slower patterns and just a few action are or patterns and bursting patterns |
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06:06 | So we need that in order to all of the inputs, process all |
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06:13 | our thoughts, intellectual abilities and things that and put out the output whatever |
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06:17 | is hitting a ball with a tennis or speaking to the audience and so |
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06:28 | . Then we moved on to glia we discussed different subtypes of glia and |
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06:34 | not gonna go through all of the we discussed but throughout the last couple |
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06:41 | lectures have pointed out certain pathologies and that we discussed. So as it |
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06:47 | to my elimination, we talked about which is basically an inflammation following an |
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06:56 | . But then we discussed two One is the P. N. |
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07:00 | . Disorder Charcot Marie tooth and one a C. N. S. |
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07:05 | disorder which is multiple sclerosis. So should review those also. And then |
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07:13 | the end we summarized uh summarized the of the major they're not all of |
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07:24 | sub types of glial cells will be . For example, radio glial cells |
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07:27 | not shown here. But Michael, you remember the most mobile elements to |
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07:33 | activated injury, inflammation are responsible for inflammatory autoimmune response in the brain. |
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07:43 | have a little tender sides that provide in the C. N. |
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07:47 | Have Schwann cells that provide myelin and PNS spinal nerves and then exercise. |
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07:54 | have that are controlling here. You see by the synapses so that they're |
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08:00 | synaptic activity but they also have their on the blood brain barrier. So |
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08:06 | are part of one of the checkpoints substances to cross into the brain. |
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08:13 | good thing that you can do with like this is write down all the |
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08:18 | that you know on the slide, do do, what does Elizabeth underside |
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08:25 | ? Has already shown what disastrous I'd what is another cell in the |
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08:30 | M. S. You can transfer in the P. M. |
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08:32 | So these are great for taking notes studying and reviewing And then we ended |
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08:38 | about briefly the blood brain barrier. introduced the blood brain barrier when we |
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08:43 | about covid 19 infections and we talked the fact that if you have a |
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08:48 | high viral load in your blood diary and your blood and you have |
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08:55 | Those processes like inflammation can make blood barrier loose other than that under normal |
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09:02 | blood brain barrier as tight junctions between , the real cells so things cannot |
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09:07 | . You have parasites and then you the astra acidic and feed here, |
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09:12 | also has another checkpoint for things. remember that if Covid 19 crosses then |
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09:19 | will hang on to a stew receptors those ace two receptors are expressed by |
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09:24 | and Julia. So there's a way covid to infect neurons and glia once |
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09:29 | inside the brain tissues and for the part, blood brain barrier serves this |
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09:36 | protective function. So if you drink drink or something that gives you a |
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09:42 | boost of some element, it doesn't that all of the drugs into the |
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09:46 | you get protected only certain things that allowed to pass and have transporters that |
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09:51 | small or that are like a filling designed to pass through the blood brain |
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09:56 | , allowed to pass other things are and kept within the blood. And |
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10:02 | uh in some instances blood brain especially if you're talking about neurological pharmaceutical |
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10:12 | can become an obstacle. Why is an obstacle? Because most of the |
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10:20 | are kills that gets swallowed, it through your digestive tract, a fraction |
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10:26 | that active ingredient gets into your bloodstream then from your bloodstream, a fraction |
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10:32 | that active ingredient can cross through the brain barrier. And if you have |
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10:37 | example, if you're watching some commercials Tv and they're talking about antidepressant drug |
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10:44 | PTSD post traumatic stress disorder and they're all of these side effects. So |
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10:53 | you take this drug you know it help your depression, you will help |
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10:56 | PTSD but you will have abdominal maybe abdominal bleeding rashes on the |
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11:03 | Okay, what what why are you all of these things? Because these |
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11:07 | side effects. These are side Because you're taking a drug you're targeting |
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11:13 | condition in the in the brain but receptor, similar target molecules and cells |
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11:18 | also found in the body. And a fraction of that drug will cross |
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11:23 | the blood into the brain. So designing a neuro drug, a good |
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11:30 | drug or a good molecule, you to keep this in mind and the |
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11:37 | that we want to do in this is have neural drugs that can cross |
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11:43 | blood brain barrier very efficiently. So should be small. You hear about |
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11:49 | medicine, nanoparticles, making things nano maybe they should be like a |
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11:57 | so they dissolve through the membranes and into the brain ultimately you want that |
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12:04 | to bind to specific cell subtype. we know that specific cell subtypes like |
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12:10 | example pyramidal cells in hippocampus and pyramidal are in the cortex and there throughout |
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12:15 | brain? So you're still going to all of the parameter cells. But |
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12:20 | if you guys got so smart and advantage of those cellular markers that are |
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12:27 | to the cells and somehow managed to the drug to that particular cell subtype |
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12:33 | a particular part of the brain. is really the ultimate that we want |
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12:37 | do. You want to get as to the problem as possible if your |
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12:41 | is being generated from the temporal lobe the side and you have a clear |
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12:46 | that starts the seizure, Most of drugs will treat the entire brain, |
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12:52 | that area, but ultimately what we is to get the drugs that are |
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12:57 | specific and that can easily cross the brain back. It also brings a |
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13:03 | . It's like, well, what the other delivery methods then? This |
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13:07 | quite inefficient if we're swallowing tail. other delivery methods like inhalation, what |
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13:12 | in your lungs almost immediately goes into blood. There's an advantage to speed |
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13:17 | to get things into the blood. other things, nasal sprays. We |
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13:23 | about substances crossing directly to the So for certain conditions and not just |
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13:28 | sinus uh information for epilepsy for there are some nasal sprays and this |
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13:35 | something that I think is going to explored more and more. It's just |
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13:39 | the hat we are the creatures of now carrying a nasal spray to spray |
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13:45 | I'd rather just, you know, and take the pill. Um, |
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13:58 | , I mean, we it's it's getting there but it's not to the |
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14:03 | that that I'm describing where you'd be to identify cell number 17 in the |
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14:09 | and target that salad, avoid that 17 and other parts of the |
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14:13 | So not to that extent. But definitely being, you know, |
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14:18 | you know, the cells that have in oncology themselves that would be recognized |
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14:24 | they're mutated and they have certain There's a certain extent, yes. |
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14:29 | to the extent that I'm talking about more of a sci fi and and |
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14:33 | solution for the center and really, , so we are moving on to |
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14:44 | of this good staff that we Okay. And today we're gonna talk |
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14:51 | resting membrane potential and what is resting potential. I explained to you these |
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14:58 | , electro physiological recording techniques where we little electrodes and those electrodes can be |
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15:03 | inside the cells. So when you an electrode, this micro electrode and |
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15:09 | have this micro electrode outside the I'm gonna say that outside of the |
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15:13 | environment is grounded or it's zero, no charge. It's charge neutral. |
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15:21 | as soon as you cross the membrane neuron, your volt meter will show |
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15:28 | drop to about -65 million poles. we know that neurons are excitable. |
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15:37 | also know that muscles are excitable. know that there's a charge separation, |
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15:42 | unequal distribution of charge on the inside the cell verceles outside of the south |
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15:47 | all of the action in the membrane near the membrane, all of the |
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15:53 | accumulated. The negative charge on the The core inside of the cell is |
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15:59 | neutral. So only the outside edges the membrane is charged -65. And |
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16:06 | outside is positively charged because we have charge, we have the ability to |
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16:14 | ions across plasma membrane in a very fashion to produce this very fast action |
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16:22 | . So when you talk about action , this is active member and |
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16:26 | And when we talk about resting membrane , they're called passive membrane properties because |
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16:31 | cell is not actively producing this action . But we're talking about excitable |
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16:38 | And before we talk about wrestling number potential, we're gonna remind ourselves of |
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16:44 | of the activities. And the reason you need this fast activities and fast |
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16:50 | in ions is because we have to not only to uh sensory stimuli coming |
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16:57 | , but also motor stimuli, You want to jump out the bears |
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17:02 | at you. You want to not there and think although sometimes, you |
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17:06 | , you don't know what to do the bears coming after you sometimes maybe |
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17:09 | it's good to stand, you watch videos of the bears. Uh people |
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17:16 | the trails hiking and come across the and some run and some just stand |
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17:21 | wait to see what happens. But any case if you step on the |
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17:25 | , you wouldn't think for long. you put your hand over something |
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17:28 | you wouldn't think for long intellectually. this really causing my skin to melt |
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17:34 | not? Is it really painful? this reflexive behavior? So you need |
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17:38 | reflexive behavior. Reflexive behavior that we're to discuss today is the simple reflex |
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17:44 | , the simplest part of our simplest of reflex pathway. And this kind |
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17:50 | a test that is exhibited here with stimulation of the attendant here is performed |
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17:58 | the doctor's office. So even if go to see your primary care physician |
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18:04 | an annual checkup, he or she do that. Put a little mallet |
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18:09 | your patella tendon, tap it. the effect should be that your leg |
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18:14 | up a little bit like this. normal hotel attendant reflex, arch, |
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18:22 | , knee jerk, reflex stretch or tendon. It's all interchangeably used. |
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18:28 | the stimulus here, there's a little , a little mallet, neurologists will |
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18:35 | that for sure. Actually doctors will it when the kids are growing |
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18:39 | You know, they'll have them follow pen with their eyes and check everything |
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18:44 | this reflex to So when this tap here, this information at the level |
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18:52 | the quadriceps or extensive muscle, that's muscle that's going to kick up the |
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18:56 | . So if the contract is going kick up the leg, you have |
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19:00 | root ganglion cells. So take good here because you already know that dorsal |
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19:06 | ganglion cells a pseudo you Nicole Like we talked about morphology, these |
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19:14 | neurons have a peripheral axon, peripheral will pick up mechanical information, mechanical |
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19:25 | tapping here from this area. This axon will send the information into the |
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19:31 | dorsal root ganglion cell selma's that are outside the spinal cord. That's why |
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19:37 | form that ganglion that bundle. Because Soma said that, and then there's |
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19:42 | much through the central axon. So is studio una foto sell through the |
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19:47 | axon. It's an excitatory cell. is going to release glutamate onto the |
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19:56 | neuron here. Motor neuron is a cell that we discuss morphological and |
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20:05 | This motor neuron will cause the release acetylcholine by motor neurons at what is |
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20:13 | a neuro muscular junction neuron to So just with the mama synaptic |
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20:22 | this self except the sensor activity exercise glutamate motor neuron motor neuron releases the |
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20:29 | locally and this muscle will contract. a very reliable synopsis, a very |
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20:35 | synapse. The charge for the synaptic is very high in amplitude. So |
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20:41 | always have a twitch. If this activated and the motor neuron is |
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20:46 | you will have a contraction of this . However, we know that when |
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20:51 | select your biceps, what happens to triceps, it's relaxed, it's the |
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20:57 | muscle action. So when you have contraction of your quads here on the |
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21:06 | for the reflex to be effective and your leg to effectively move up and |
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21:12 | you actually have to relax the For the flex a muscle hamstring will |
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21:20 | if you're bringing it in now you to relax this muscle so it just |
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21:24 | what you're activating. In this case activating the contraction off the quadriceps. |
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21:31 | do you relax the hamstring? So this reflex to actually be effective you |
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21:39 | have to involve a local interneuron in spinal cord. So when the same |
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21:45 | neuron is excited will release glutamate on inhibitory interneuron here. It's also a |
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21:52 | cell and this inhibitor interneuron will release inhibitory neurotransmitter and it will inhibit this |
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22:01 | neuron and by inhibiting this motor neuron motor neuron is not releasing any acetylcholine |
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22:08 | the muscle is kept relaxed so that can have a proper contraction of the |
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22:15 | . One thing to note that's very to data said that the major excited |
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22:20 | your translator of the CMS is The major inhibitory neurotransmitters. Gaba gamma |
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22:25 | butyric acid. These inter neurons in spinal cord they release glycerine. So |
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22:33 | the neurotransmitter they release. This is exception in the sense of exception to |
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22:39 | in the C. N. S the spinal cord glycerine is an inhibitory |
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22:45 | that gets released by these multipolar into . Okay and inhibit in this case |
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22:52 | hamstring motor neuron relaxing the hamstring in words is mono synaptic single synapse |
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23:01 | Is it enough to contract the Yes it is. But is the |
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23:06 | like it's going to be fully effective relaxing the hamstring? No. And |
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23:11 | do that you're now looking at policy circuits because it's multiple synopsis that are |
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23:18 | . And it's still a very simple synaptic 123 synapse circuit. Some of |
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23:24 | complex reflexes that we have that involves synapses and sometimes different parts of the |
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23:31 | of the brain I can think of example as a gag reflex. Uh |
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23:39 | something if you inhale or if you something nauseous or even emotional response could |
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23:48 | a gag reflex that it's a reflexive . You don't control. Many synopses |
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23:52 | be involved in order to execute That would be more of a more |
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23:57 | reflex. So for this part please yourself you know the sensory afghans caring |
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24:05 | into the spinal cord DRG cells, neurotransmitter, their anatomy. You have |
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24:12 | processing in the spinal cord and you activation off the output which is at |
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24:21 | is going in a e is going of the spinal cord into the |
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24:29 | Um And this is multipolar cell. self inhibitory interneuron licensing, excited. |
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24:36 | remote. Yes. Yes. Yeah it's a good question because I'll confuse |
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24:49 | even more toward the end of this because glycerin also turns out to be |
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24:55 | little made receptor co factor in the don't take these notes now. We'll |
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25:00 | back to it later. Okay so as as I said in in and |
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25:05 | every science and the Neurosciences always So this is an inhibitory neurotransmitter in |
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25:10 | spinal cord. And slicing will serve different function in the cns. Now |
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25:15 | is that? It because it depends what receptors are expressed by the post |
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25:19 | cell. So the response of the will depends what receptors it expresses. |
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25:24 | it have only excited there is an only inhibitors analysis. This is also |
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25:29 | very simple circuit because this is excitation excitation excitation. Okay, so |
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25:38 | build up this charge across plasma membrane creatures of water and we have a |
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25:44 | of water in the brain and oxygen extra electrons and has negative charge, |
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25:51 | has negative net positive charge held by bonds. Water molecules and other polar |
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25:59 | such as ion sodium chloride will dissolve in the water and they will form |
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26:06 | bonds and some of the ions will protons and electrons that are different than |
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26:16 | . So some of them will have valence. Your charge mono valent charge |
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26:22 | as chloride minus mono valent dive allen calcium two plus so the valances to |
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26:33 | ions are positive ions, N. plus calcium two plus K. Plus |
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26:41 | cat ions and and ions are negatively ions. So the most important one |
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26:47 | be discussing chlor idea. And as know, neurons are surrounded by plasma |
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26:55 | is possible lipid bi layer and this lipid bi layer as it is does |
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27:01 | allow for ions to cross through the . In order for the science to |
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27:07 | through the bi layer, you have have channels. And the major ions |
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27:12 | we will be discussing over the next lectures are sodium potassium chloride and |
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27:20 | There is an abundance of sodium chloride the outside of the South is |
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27:26 | There a salinity environment on the outside the south and the inter cellular environment |
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27:31 | dominated by potassium. There is very calcium inside the South there's a lot |
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27:38 | calcium. Um Outside of the The reason why there's very little calcium |
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27:42 | the South is calcium is not only ion once calcium enters inside the South |
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27:47 | also a secondary messenger calcium can also calcium release from intracellular stores and activation |
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27:57 | transcription factors. Which means it can something about the translation and transcription mechanisms |
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28:05 | the self. That's why you don't that much of the three sides. |
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28:09 | the calcium just floating around the one comes in typically gets bound up or |
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28:16 | or bound up by these calcium binding . So it's not just really floating |
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28:22 | and then finally hear what you have an ionic pump and this ionic pump |
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28:28 | a K. T. P. . S. It will use |
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28:31 | T. P. A lot of and it will always transport ions against |
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28:36 | concentration gradient. So there's a lot sodium fluoride on the outside. So |
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28:43 | a high concentration gradient of sodium and concentration gradient on sodium on the |
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28:47 | But this pump will be putting sodium concentration gradient, putting potassium inside the |
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28:53 | against concentration gradient by using energy in form of A. T. |
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28:59 | Uh So these channels that will allow passage of the ions I made out |
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29:07 | the building blocks the nino assets that like a high school teacher and some |
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29:14 | them are essential and that is not and essential amino assets you have to |
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29:20 | . They come from food and others have in our bodies but they're building |
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29:26 | , they make these peptide bonds and building blocks for the proteins to form |
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29:32 | through these peptide bonds and you have lot of them. So it's called |
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29:36 | peptides. And this is a primary of these amino assets. And then |
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29:43 | secondary structure would be that you can this chain of amino assets and you |
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29:47 | make a coil out of it almost a corkscrew. And this is called |
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29:53 | alpha helix. And it's a secondary and also take these strings of amino |
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29:58 | and you can lay them as sheets you will hear their referred as beta |
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30:04 | . So there will be a helix there will be sheets. There will |
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30:07 | other secondary structures that you can find the secondary structures will form a |
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30:14 | So several of these alpha helix is can be trans membrane segments. Several |
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30:22 | these trans membrane segments will form a subunit and then multiple subunits will come |
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30:29 | and form in this case a channel some of the channels uh some of |
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30:37 | uh ion channels that you're seeing here , some of the protein receptors are |
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30:42 | not channels that could be g protein receptors but they'll also have a certain |
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30:47 | composition. And certain anatomy says all complex strings of immune assets and the |
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30:56 | ordinary structures finally form the channels and channels are specific to each eye |
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31:05 | So as you can see, sodium have its own sodium channel and it's |
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31:11 | to control the flux of sodium potassium have potassium channel, calcium, calcium |
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31:17 | chloride. Some of these channels are fast. It's called conductance. How |
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31:26 | of an eye on how much of charge can you pass through the |
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31:30 | So some of them are fast and acetylcholine receptor channel can conduct a million |
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31:38 | a second. So that's current I million islands a second. That's a |
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31:43 | . That's very fast conductance. It's fast and very large amplitude change at |
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31:49 | level of the plasma membrane, some things and other processes. We already |
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31:55 | hope everybody's tweaking onto this That you several temporal scales in the brain. |
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32:00 | have these very fast neurons and then have these super fast neurons and slower |
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32:06 | . Then you have these slower glial . They don't fire action potentials and |
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32:10 | produce calcium waves. And they're concerned with homeostasis, metabolism, inflammation, |
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32:19 | processes. And at the level of membrane, you have some channels that |
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32:23 | fast, open fast, close some are slow. You have to |
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32:28 | of wake them up for them to . And when they open close and |
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32:34 | can be slow to using energy and slowly but steadily pumping against concentration gradient |
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32:43 | and potassium. So channels are selected filters that means that they will accept |
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32:50 | ion sodium channel except the sodium ion it will kick out, potassium ion |
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32:56 | not allow for potassium ion to come . And when these islands come |
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33:00 | they're surrounded by these waters of hydration we called by water molecules. And |
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33:06 | they're entering into what is called the inner lumen of this channel against |
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33:12 | they're losing these waters of hydration and this most narrow point here there are |
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33:19 | acid residues and so as positively charged such as sodium or potassium will have |
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33:27 | negatively charged amino acid residue. So amino acid strings that you have some |
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33:33 | them may have positive charge on the . Studies will have negative but inside |
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33:38 | of the channel for sodium will have charged residue. And there's actually going |
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33:43 | be a little bit of an interaction allows a very quick binding of the |
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33:49 | and propulsion of that sodium molecule into inside of the south and surrounding or |
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33:56 | it with the water sub hydration. it says loading the strip of the |
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34:01 | by amino acid residues enters inside the diameter potassium was trapped and sent back |
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34:09 | . Huh? So that should make think. Does that mean the channel |
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34:15 | ions based on their size purely? it partially the answer is is |
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34:23 | partly on the sides. But you to recall one thing is that sodium |
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34:30 | a smaller ion but sodium will have stronger attraction, smaller ion for more |
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34:38 | set hydration. So it's slightly different dynamics that these ions will have. |
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34:46 | no, it doesn't mean that sodium pass through potassium channel because potassium channel |
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34:52 | bigger. potassium channel will regulate and selective to potassium. And then at |
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35:00 | point, all rules are broken. do I mean by all rules are |
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35:06 | . There's inflammation in the brain hyper , epileptic seizure activity, all the |
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35:15 | are open things are gonna be crossing they can cross And that will depend |
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35:20 | much on the size them. when the rules are broken, the |
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35:24 | becomes an important factor. When the are there normal physiological conditions you have |
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35:31 | interactions of ion the size the waters hydration, the specific amino acid residue |
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35:37 | the binding properties that are designed for ion to selectively control one single ion |
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35:45 | that channel? A little bit of . Right here we have the equals |
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35:54 | arms law. Very basic review where voltage and bolts and for neurons we're |
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36:01 | about miller balls. So the relevant is miller voles current in amperes and |
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36:08 | neurons it's nano amperes, PICO In some instances, micro amperes resistance |
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36:17 | is measured in arms and neurons are small, only 10 micrometers in diameter |
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36:23 | they have high input resistance. So have high resistance which is measured in |
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36:28 | homes, tens and sometimes hundreds of arms conductance is an inverse of |
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36:35 | Existence of G is equal one over . Or R. If you rewrite |
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36:41 | formula V equals IR I is equal times v conductance over change over voltage |
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36:49 | conductance is measured in cement and the scales for neurons is nano and PICO |
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36:55 | . So conductance is how much a ion channel conducts, how many ions |
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37:00 | can conduct. Or let's say overall to the whole cell because the cell |
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37:05 | have 2000 channels each with a specific value and then maybe you can multiply |
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37:12 | 2000 ad 2000 to get the whole conductance of the entire cell. What |
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37:20 | some of the forces that determine this of charge across plasma membrane and some |
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37:27 | the basics that we're going to review based on the concentration. If we |
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37:32 | look at the concentration gradient, which the amount of that molecule, the |
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37:39 | of that molecule. And if you a possibility by layer has no |
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37:44 | everything will stay on that side. when you introduce the sodium channel, |
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37:48 | introduce the chloride channel, the plasma . And if the rules in neurons |
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37:54 | purely based on concentration gradient, then sodium and chloride ions will flow to |
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38:01 | opposite side until both sides become the concentration or equal molar. So these |
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38:08 | you see that an A plus is and then in a plus and an |
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38:13 | plus become exactly the same. Chloride chloride become exactly the same concentration. |
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38:21 | , so diffusion forces. So if have a lot of concentration of one |
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38:27 | and little on the inside and that is gonna try to come inside the |
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38:32 | is going to drive that ion across membrane. However, ionic movement is |
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38:38 | by the electrical potentials because ions are and voltage and voltage changes are going |
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38:50 | determine also very much not only the of potential, but also how much |
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38:55 | an ion is passing through. So have cat ions, positive ions and |
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39:02 | will be repelled by an ode or other positive ions by the positive charge |
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39:08 | they're going to be attracted by cathode by negative charge and by subversive and |
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39:15 | will be attracted by an oats and by the like charge separation of charge |
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39:23 | plasma membrane. This uneven distribution of across plasma membrane is what gives rise |
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39:30 | difference in electrical potential that we measure with these electorates addressing membrane potential. |
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39:37 | resting membrane or VM is the same Inside charge of the cell. And |
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39:44 | what we're measuring. Address this -65 votes. Then by convention you have |
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39:52 | flow and direction of net movement of charge is in the direction of the |
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39:59 | . So cat ions move with the of the current and and ions in |
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40:07 | opposite direction. If you reduce the of negative charge compared to the positive |
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40:13 | on the inside of the membrane from 65 to minus 60 to minus 55 |
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40:19 | causing deep polarization. There is less the polarity separation. You de |
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40:26 | You make two sides more equal in . However, if you increase charge |
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40:32 | and make the inside of the cell more negative than minus 65 minus 70 |
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40:38 | 75 you are causing hyper polarization. increasing the difference in charge separation between |
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40:45 | and positive on the two sides of membrane. So how does it really |
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40:50 | like? So, first of all is really an illustration of what I've |
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40:56 | you before this charge separation and accumulation uneven distribution of charge negative and positive |
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41:03 | at the level of the membrane. you again looked in the side of |
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41:08 | environment more toward the inside of the . You can see it's charged neutral |
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41:12 | minus plus minus on the outside. , positive charge. Now the positive |
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41:17 | negative attract each other. So they up here across by remembering and then |
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41:22 | away in the side of in the side of solid works to settle the |
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41:26 | . It's charge neutrality. Again, there's no charges zero. So if |
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41:33 | was based on just concentration gradient, saw that if you have a channel |
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41:38 | this potassium should flow across the channel you should have the same concentration of |
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41:44 | on this other side. In this we we we we introduce an a |
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41:50 | which is a negatively charged, let's protein. And that protein can of |
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41:55 | or it could be an ion and no channel for that ion or the |
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41:59 | clothes for that. I cannot cross an island but this potassium, as |
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42:05 | can see this huge concentration of potassium potassium here, you open the |
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42:11 | potassium starts flowing and then potassium stops before it reaches the same concentration on |
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42:19 | opposite side. Because as potassium starts from inside of the cell to the |
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42:26 | , this positive charge of potassium will building up on the plasma membrane and |
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42:34 | start repulsing more of the potassium coming . This is the electrical forms. |
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42:42 | the concentration gradient is still gonna say a lot of potassium here, go |
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42:46 | the other side, go to the side is going to drive it to |
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42:48 | other side. On the other The build up of this positive charge |
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42:52 | gonna say uh we're repelling, you back, go back this is what's |
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42:58 | the equilibrium potential that this situation, diffusion all and electrical forces are equal |
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43:06 | opposite to each other in the direction there's no net flux of ions. |
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43:12 | means that some potassium is going to right, some potassium is going to |
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43:16 | left, exact same amount. There's net flux to the left hand side |
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43:21 | to the outside of the south. this is the time and moment. |
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43:27 | the potential value plasma membrane at which I said, the concentration diffusion, |
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43:34 | forces driving in this direction have an repulsion of charge, electrical currents and |
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43:43 | no net movement of charge. So have this net ionic differences at the |
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43:50 | membrane. We will discuss this concept the driving force once you understand today |
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43:56 | to calculate equilibrium potentials and the membrane in general, the resting membrane |
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44:02 | So, hold that thought. But thought indicates that it has something to |
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44:07 | with DM and E. Ion Dion the overall membrane potential. E ion |
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44:13 | equilibrium potential. What does that mean the ionic concentration is known or unknown |
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44:23 | . We can calculate this equilibrium potential island. Welcome back to this |
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44:29 | M minus E. Ionic in a seconds. No it's not just for |
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44:37 | . So the same goes for any or sodium you have a lot of |
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44:42 | on the outside, you open the but sodium will start flowing down concentration |
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44:47 | until the electrical potential says no So it never reaches equal molar |
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44:53 | That's where you have the separation, distribution of charge inside versus outside, |
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45:00 | around the memory. And in addition these channels, as you can see |
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45:07 | certain concentration of these ions that we um in the old days we knew |
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45:14 | concentration of ions for animals like squids example, they have these giant toxins |
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45:23 | where do they live in the very high salinity environment you live in |
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45:31 | you can tell what ions you have right in that water and you can |
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45:36 | the axon and you can squeeze the out. The side is all out |
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45:40 | axon or the cell and you can what ions you have there. So |
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45:45 | knowing the concentrations of ions on the or the outside, you can now |
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45:50 | the equilibrium potential as you can see outside of the cell is dominated by |
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45:58 | and by chloride there's a lot of of the signs on the outside of |
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46:02 | cell and there's little of sodium and on the inside of the cells. |
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46:10 | outside of the cell also has about million moller of calcium And the inside |
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46:17 | the cell has .0002 million mauler of . So when you talk about concentration |
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46:28 | or inequality of concentration, the highest gradient concentration gradient is actually for |
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46:37 | It doesn't mean that this is what's determining the member in the country and |
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46:43 | also doesn't mean that these channels are open. Such thing that we'll talk |
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46:48 | called permeability of these channels, but , you have a lot of |
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46:52 | a lot of chloride, a lot calcium on the outside, little of |
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46:57 | molecules on the inside and the inside the cell is dominated by potassium and |
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47:01 | are the actual no um all of . Okay, And here you have |
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47:10 | fluoride ion with the concentrations and you ride out these concentrations inside versus outside |
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47:17 | ratios to there's 20 times more potassium the inside of the south, there's |
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47:23 | times more sodium on the outside of cell versus the inside of the |
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47:28 | And the other thing that is shown is -60-175. Nobody bothers to ask |
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47:35 | about that. It's about 15, votes. What does that mean? |
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47:40 | means that different subtypes of cells that discussed will have slightly different membrane potential |
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47:45 | rest and that is because they all slightly different composition of these higher |
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47:50 | These ion channels may have different sequences amino acids, which changes their |
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47:55 | how much they can conduct. Maybe can conduct 100 110 gallons a |
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48:01 | That depends. So what does that ? And what value am I gonna |
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48:06 | you what's resting membrane potential minus 60 65 minus 70 minus 75. I'm |
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48:10 | give you a whole step with diagram the values that we will follow because |
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48:15 | textbooks will give you a different answer resting membrane potential. And that just |
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48:20 | , it depends on, as I , how permeable are these cells to |
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48:26 | ions And we get to that in second but also there might be different |
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|
48:30 | . Micro fluctuations of certain ionic concentrations and regional. And then there are |
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|
48:37 | things that are called thermodynamics. When goes up, things start moving |
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48:43 | temperature goes down, molecules and movement ions slows down. Does that mean |
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48:50 | we all are constantly at 37°C to physiological body and brain temperature? |
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48:58 | you may wake up and you'll be and then by the time you had |
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49:03 | coffee, your 37 you get in argument with somebody at 38, you |
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49:09 | sick with fever at 42C, you to go to hospital But is it |
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49:14 | to be always at 37. Now gonna go into a sea of body |
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49:19 | is gonna change slide all of So these all micro fluctuations will determine |
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49:23 | speed of movement to and that speed the temperature will influence the number of |
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|
49:29 | . Now hear what you have the values or equilibrium potential for potassium |
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|
49:36 | 80 sodium positive, 62 calcium 1 and chloride negative 65. The equilibrium |
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49:46 | for an ion can be calculated using famous nerves equation and what nerves |
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|
49:54 | You determined that if we have the which is ionic of liberal potential actually |
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|
50:02 | up with a formula. So an you're not gonna need a calculator, |
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|
50:06 | gonna need to know the terms of formula. So if I write it |
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|
50:11 | you should be able to recognize that have the wrong terms in this |
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|
50:16 | And you should be able to recognize calculations for ions but not having to |
|
|
50:22 | them yourself. So what he came with 2303 R. TCF long based |
|
|
50:29 | algorithm ion concentration on the outside of cell which is oh and I on |
|
|
50:36 | which is iron concentration on the inside the self. R. Is the |
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|
50:40 | constant. T. Is absolute Uh But we can also insert you |
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|
50:47 | in T. When we're going is going by body temperature 37 C. |
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|
50:52 | whatever you wanna do, you can into Calvin or use T. Charges |
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|
50:59 | valence of the ion Plus one Plus -1. The f is saturday's |
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|
51:07 | Again it's electrical constant it doesn't And then the concentration of dials. |
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|
51:13 | if you take this 23 03 remember equilibrium is the balance of two influences |
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|
51:20 | which pushes an island balance concentration chemical gradients and electricity which causes an |
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|
51:27 | to be attracted two opposite charges and by life charges. Increasing the thermal |
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|
51:34 | of each particle increases diffusion. That's I talked about. The second will |
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|
51:38 | increase the potential difference achieved equilibrium. ionic equilibrium is proportional to temperature to |
|
|
51:47 | proportional to T. On the other increasing the electrical charge Z. |
|
|
51:54 | Each particle will decrease the potential difference to balance the fusion. Therefore e |
|
|
52:01 | is inversely proportional to Z over We need not to worry about are |
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|
52:07 | . And nurse equation because there are and when you take the 2303 |
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|
52:13 | T. C. S. And collapse at 37 C it actually collapses |
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52:19 | 61.54 with the middle of all And then you have log of potassium |
|
|
52:26 | versus potassium inside log of potassium sodium versus inside florida outside versus inside. |
|
|
52:34 | this is all the same calculation 61 middle of balls for potassium. Same |
|
|
52:39 | sodium because nothing changes here is plus plus one. Okay except the concentrations |
|
|
52:48 | different here. But here that it's 61.54 for chloride and that's because chloride |
|
|
52:54 | gonna have a Z f minus So that's very easy. And for |
|
|
52:58 | this abbreviated to half of 61.57 which 30.77. And that is because you're |
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|
53:05 | it by two here calcium is two . So you're dividing by the valance |
|
|
53:11 | So you can then take the potassium and potassium on the inside and hear |
|
|
53:17 | ratios. Remember I told you you plug in five on the inside outside |
|
|
53:22 | 100 on the inside or you can 1-20. So here we plugged in |
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|
53:28 | ratios and the outside is 1 20 more than inside this log 1/20 is |
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|
53:35 | negative 1.3 and negative 1.3 multiplied by term here 61.54 million balls. Give |
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|
53:43 | the equilibrium potential for potassium of minus million balls. So if we if |
|
|
53:50 | do the same exercise and you do calculation for sodium and plug in the |
|
|
53:55 | values from here 10 on the one on the inside for calcium and |
|
|
54:03 | . These are the values equilibrium potential that you're going to see for these |
|
|
54:09 | ions. Okay so this is for ions. So nursed equation or equilibrium |
|
|
54:19 | calculation is for single ionic species for or for catastrophe. And notice that |
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|
54:29 | E. K. is -102. here the ion for potassium is |
|
|
54:38 | That's why I don't want you necessarily get hung up on the exact number |
|
|
54:43 | about another lecture when I give you actual scale, there's gonna be fluctuations |
|
|
54:49 | differences. Why? Because there might more of a potassium ion on the |
|
|
54:54 | of certain themselves rather than inside. so that will influence again the value |
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|
55:00 | that ionic equilibrium potential. But what that do for us if we know |
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|
55:07 | equilibrium potential for one ion? Do know the resting membrane potential? We |
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|
55:13 | because sodium will flux, potassium chloride will flux calcium influx. So |
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|
55:21 | membrane potential as we see it at is not just one ion. It's |
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|
55:27 | interaction and interplay of the ions that dominant here sodium potassium chloride, |
|
|
55:34 | And how do we calculate the membrane ? To calculate the number of |
|
|
55:39 | We're using the golden equation and the equation after this part here is exactly |
|
|
55:47 | same as nerves equation. This T. Z. F. Log |
|
|
55:52 | our TCF collapses 61.54 million goals. have a log something new here. |
|
|
56:00 | of all, you have potassium on outside and inside. That's the same |
|
|
56:04 | Newton's equation. But now you have ion that you're taking into consideration and |
|
|
56:10 | sodium multiple ions. The other thing is different is the P. |
|
|
56:18 | Which stands for permeability is it's not uh analytical chemistry PK value. Its |
|
|
56:24 | for podcasting. How much is the permissible to potassium addressing number and |
|
|
56:34 | The cells have these ion channels for that are called leak channels and they're |
|
|
56:42 | be leaking potassium out. So like why are they looking? Because that's |
|
|
56:47 | the nature built it has a lot potassium and potassium is slowly oozing out |
|
|
56:52 | the cells addressing members potential. That that the cell membrane has mostly potassium |
|
|
56:59 | opened And other channels like sodium channels not. So that means that addressing |
|
|
57:07 | in potential there's huge T. permeability value for potassium. 40 times |
|
|
57:14 | permeable to potassium addressing number of potential to sodium. Does that mean sodium |
|
|
57:21 | not flexing? No but 40 times than potash in. Does that mean |
|
|
57:26 | sodium does not contribute to the value the resting membrane potential? No. |
|
|
57:32 | you're also doing the calculation of the is not just the permeability. One |
|
|
57:38 | something doesn't change anything. But if have a different value here with concentrations |
|
|
57:44 | calculation that you run through the potassium four or five. This is real |
|
|
57:50 | moller plugged in here instead of Like we had a nurse equation you |
|
|
57:56 | this, you take the log of 50/4 15 61.4 you get minus $65 |
|
|
58:03 | . So is it the same as equilibrium potential? No not exactly. |
|
|
58:09 | minus. We talked about equilibrium potential potassium typically being around -80. Is |
|
|
58:16 | close anywhere to the equilibrium potential for ? No, but is it influenced |
|
|
58:24 | sodium? Yes, absolutely. So major dominant eye on address and the |
|
|
58:30 | is most formidable to this potassium But that changes from the ability for |
|
|
58:38 | for sodium or potassium chloride can change as permeability changes. Guess who gets |
|
|
58:44 | weight during the rising phase of the potential that will start discussing next |
|
|
58:50 | The cell is mostly permeable to The rules change the permeability ratios |
|
|
58:57 | It's just opposite. The cell becomes times more permeable to sodium. Then |
|
|
59:03 | during the rising phase of action potential the following phase of action potential, |
|
|
59:08 | changes again, it flips and the becomes most formidable to potassium again during |
|
|
59:15 | following phase of the action potential. , overall membrane potential at rest resting |
|
|
59:24 | potential. Deanna's the membrane potential it is dominated by sodium and potassium |
|
|
59:31 | mostly dominated by potassium flocks During the and rise of action potential. It's |
|
|
59:39 | permeable to sodium. And then it backing on. And so you have |
|
|
59:43 | flux in these ratios. Some cell a little bit more permeable to |
|
|
59:49 | others more permeable to sodium. And you'll get different calculation here just put |
|
|
59:56 | or put, you know, 145 13 and you'll see that it changes |
|
|
60:03 | different value minus 67 minus 63. will shift. Okay. And this |
|
|
60:08 | what's happening in reality. And that's when I showed you this measurement and |
|
|
60:13 | , nobody is asking me a question what is the resting membrane potential? |
|
|
60:17 | it minus 16 minus 75? So follows somewhere in between all of these |
|
|
60:22 | on the properties and the qualities of channel and depending how formidable the plasma |
|
|
60:27 | is to give an eye on at particular uh space and time. So |
|
|
60:34 | is actually the last slide uh and we finished for today and when we |
|
|
60:43 | back on Tuesday, we'll continue talking the action potentials. So we'll review |
|
|
60:48 | two formulas again, you don't need do the calculation, but if you're |
|
|
60:54 | tell me that there's way more so on the inside of the south, |
|
|
60:58 | gonna get the question wrong. You , if you're gonna say that it's |
|
|
61:04 | of temperature announced equation, you're gonna the answer on if you're gonna say |
|
|
61:09 | Goldman equation is only calculating based on ion from the ability. Again the |
|
|
61:16 | answer. So we'll review these two because a lot of stuff I think |
|
|
61:21 | podium structures, basic will review these equations and then we'll move into the |
|
|
61:27 | of the action potential and you'll understand about the openings and closings of the |
|
|
61:32 | and you will know more than you to know about action potential after we're |
|
|
61:37 | with it. So thank you very . And I'll see you all on |
|
|
61:45 | . Thank you guys on zoom. |
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