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00:00 | All right, This is lecture seven neuroscience. Last lecture we were discussing |
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00:07 | resting membrane potential number in potential at , Which means that the cell is |
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00:15 | very active. It doesn't mean that potential value is always at -65 million |
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00:23 | which is the charge separation across plasma compared to the outside. It doesn't |
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00:29 | that the 65 million malls negative value a flat line. The cells are |
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00:36 | sporadic inputs, excitatory an inhibitory inputs that line fluctuates constantly. There is |
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00:44 | dynamics involved and temperature changes locally at foster lipid bi layer. It will |
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00:51 | the fluctuations and nobles as well and activity. But the trust means that |
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00:57 | cell is not generating the action Which will be the discussion of later |
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01:05 | . So addressed what's happening is We have an equal distribution of charge |
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01:21 | we will talk about this ionic species come back. But one thing that |
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01:25 | discussed last lecture was the reflex the knee jerk, stretch, |
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01:31 | tendon, reflex. And I've asked to do a certain thing that will |
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01:36 | you answer several questions in the you have to know the three cell |
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01:43 | that are involved in generating this reflexive . So dorsal root ganglion cells into |
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01:51 | and motor neurons. You have to their morphology whether they're multipolar cells or |
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01:57 | pole or pseudo unit polar. Have know which neurotransmitter they release. Do |
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02:03 | release glazing or glutamate or settle coding something else. And you have to |
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02:07 | whether that neurotransmitter or that cell. excited, turn inhibitor and also the |
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02:15 | meaning you have to understand where those are located. You have to understand |
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02:21 | the selma's of the dorsal root cells located outside the spinal cord and into |
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02:28 | control local network activity within spinal cord motor neurons project the motor command out |
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02:37 | the spinal cord, their axons into muscle fibers. So we talked about |
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02:43 | quadriceps and to have strength, flexor , opposing muscles. And for this |
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02:48 | to be effective, you don't only the muscle but you also relax opposing |
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02:56 | . And if you think about the and this is something that gets tested |
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03:01 | neurologist office if they do even the checkup or if you're having some neurological |
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03:08 | , some movement problems or something like . A little tap on that on |
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03:13 | patella tendon here that picks up the and now by having the circuit behind |
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03:19 | and observing a different kick in the , you can start reducing what might |
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03:23 | wrong in this circuit might not be sensor information. And so the stimulus |
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03:29 | to be really strong. Maybe the doesn't have inhibition and a very light |
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03:33 | produces a very large response. You start addressing actual mechanistic pathological problems that |
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03:41 | be happening by looking at this cap . Patella tendon and also in addition |
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03:47 | those three types of south that I've mentioned. You should also know your |
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03:53 | . It'll sell in the hippocampus and cortex with its projection sell excited to |
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03:59 | and also the inhibitory cells that release . There's a great diversity of those |
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04:06 | . So we talked about ions and talked about water some hydration last lecture |
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04:11 | we talked about the four main ionic that are unequally distributed across plasma |
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04:20 | And in particular those four species are , potassium, chloride and calcium. |
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04:34 | the membrane will express channels for these . And for the next couple of |
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04:42 | will be focusing on what we call gated channels. That means that voltage |
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04:47 | the voltage and chemical gradient will be ions across these channels across plasma |
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04:54 | Later in the course, when we about snappy transmission, we'll talk about |
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04:58 | gated channels. When we talk about , we'll talk about McKenna sensory receptors |
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05:05 | gave a challenge. So sodium is and chloride is abundant as an Aquarius |
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05:13 | solution on the outside of yourself. dominating on the inside of the |
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05:18 | You have high concentration of potassium, highest concentration gradient disparity exists for |
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05:25 | .1 Michael Moller on the inside 10 , sorry millie mole on the |
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05:33 | It's 10,000 times concentration difference. And as I discussed, it's very tightly |
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05:40 | inside side of plaza inside of side all. There is not much of |
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05:44 | free calcium floating around because it acts a secondary messenger. It can influence |
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05:51 | release from internal calcium stores inside the and it can also influence the fusion |
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05:58 | release of the neurotransmitter vesicles. calcium side or solid calcium gets bound |
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06:04 | and calculated by calcium binding proteins and of course another. They're important element |
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06:11 | is a pump, a pump that's a channel that's bringing in sodium and |
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06:18 | against their concentration gradients next to one these. Each one of these ions |
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06:25 | also see this value E N A K E C L E C A |
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06:30 | plus which stands for equilibrium potential I also call it nerves potential value |
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06:38 | ernst equation is used to calculate this . They also call it reversal potential |
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06:44 | ionic reversal potential value. It's all of these terms are used interchangeably |
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06:50 | But each one of these islands have own equilibrium potential value and you'll understand |
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06:56 | why and how it plays into remembering and also generation of different aspects of |
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07:06 | . Now we talked about peptide bonds you know, acid essential non essential |
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07:11 | acids. The building blocks little bricks put together comprise secondary tertiary coordinate repentant |
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07:18 | , prudence, protein channels that we're about are comprised of multiple subunits receptor |
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07:26 | . Multiple subunits trans membrane proteins that g protein coupled receptors. You don't |
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07:35 | a channel there also comprised of multiple 5674. Just depends on a different |
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07:42 | of the channel. Each one of is selected for a given ion. |
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07:49 | we talked about channels. Ionic channels ion surrounded by waters of hydration that |
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07:55 | gets stripped of these orders of hydration with negatively charged amino acid residue inside |
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08:01 | innermost lumen. This channel gets propelled to the south And sodium has the |
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08:09 | channel, potassium chloride, calcium. some point those rules can be broken |
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08:14 | ions that 50 channels can travel through but the ionic channels are selective when |
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08:19 | conduct ions at a fast pace and of discharge or movement of discharge across |
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08:26 | channels influenced the change in the potential possible number. Arms law vehicles. |
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08:36 | voltage current resistance conductance is inverse of . Therefore, if you plug in |
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08:45 | G in here instead of one over . You get G. V. |
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08:52 | I voltages and miller volts relevant skills the brain. Milli amperes micro amperes |
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09:01 | arms for resistance and neurons and PICO nano siemens for conductance is of individual |
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09:08 | or individual neurons. There's irrelevant scales measuring these events, diffusion is a |
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09:20 | gradient. You have the diffusion of . So if you have a lot |
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09:24 | sodium fluoride on one side and you the channels for sodium fluoride purely based |
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09:30 | the concentration gradient. If you're just at the chemistry, you're going to |
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09:34 | equal molar or equal concentration distribution across plasma membrane but ionic movement is also |
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09:43 | by electrical potential and each one of island's essentially has a battery representation electrical |
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09:51 | . You have battery and cat eye such as sodium will be attracted to |
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09:58 | end of the battery. To capture and Lauren will be attracted to pano |
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10:03 | positive. And then the battery discharge is again across plasma membrane. And |
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10:10 | is the charge separation. Is the between the voltage on the inside of |
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10:15 | cell versus the voltage on the outside the south. So what is the |
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10:20 | on the inside of the cell? voltage on the inside of the cell |
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10:23 | accumulation of this negative charge across plasma . What is the voltage on the |
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10:28 | of the cell is presumed to be or zero neutral zero mobiles charged. |
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10:36 | the difference across Bosnia membrane. The versus out of 65 million difference at |
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10:44 | . Some basic information current flows direction net movement of positive charge of Catalans |
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10:51 | into con direction and ions move opposite direction. If you increase the charge |
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10:59 | , that means if you accumulate more more negative charge, you hyper polarized |
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11:05 | from -65 to -75 to -80. you decrease this negative charge and you |
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11:12 | it with respect to the outside of cell, you are causing a deep |
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11:17 | of this plasma membrane. It's really to plasma number but equilibrium potential for |
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11:25 | ion exists because ions have a Yeah. And equilibrium potential is a |
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11:33 | at which point the chemical forces that driving these ions across plasma number and |
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11:40 | the channels to equalize the number of they encounter. Electro motive or electrical |
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11:49 | . And that electrical force a lot times is created by the movement of |
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11:55 | same ionic species across plasma membrane, charge now becomes repellent to a positive |
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12:02 | . So let's look at the situation as an example, potassium and a |
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12:07 | , let's say, protein, negatively protein that's stuck in potassium channel opens |
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12:12 | potassium goes down its concentration gradient from there's a lot of potassium to where |
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12:18 | a little potassium but it never equalizes both sides. Because as this positively |
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12:26 | catan and potassium moves across the it accumulates the charges accumulating on the |
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12:34 | member and on the outside and the of the positive charge now starts repelling |
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12:40 | charged potassium from further coming down its gradients. At this point, the |
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12:48 | force that is pushing the number of pushing to equalize with the other |
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12:55 | The same number of ions is the force. And the electrical potential electrical |
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13:02 | pushing it is exact same and they're equal to each other and they oppose |
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13:12 | other. And ions will still be across the membrane and the channel. |
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13:17 | there isn't going to be any net movement. That means there isn't gonna |
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13:21 | net movement to the inside or outside this equilibrium potential value. That's the |
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13:27 | potential value is the value. And the membrane it's a value at which |
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13:36 | chemical force is the same and opposite the electrical force. And there is |
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13:43 | not bionic movement. Right? You see that there is an accumulation of |
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13:50 | across the plasma membrane here. But you go on the extra cellular |
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13:55 | or even if you go on the inside of the side, a plasma |
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14:01 | the cell, the core of the charge neutral, just like the outside |
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14:06 | charged, mutual. So all of charge accumulation and separation of charge and |
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14:12 | distribution of charge by physically is at level of the plasma membrane. And |
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14:20 | we're discussing is we're discussing another important that's called the driving force. Driving |
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14:27 | is the difference between the voltage of membrane and each ion if the Librium |
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14:33 | . So, we'll come back to uh concept of the driving force, |
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14:38 | just introducing it in the slide will back in the following slides. |
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14:44 | if the ionic concentration is known, can calculate equilibrium potential for each |
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14:55 | So, how do we know you're the concentration inside accents or inside |
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15:01 | I'll show you the movie a little later, but it's basically taking these |
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15:06 | squid axons and squeezing the tube like giant action, squeezing the inside of |
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15:13 | tube and measuring the concentration of ions the inside and then taking where the |
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15:18 | live in the ocean and taking taking acquis environment that's inside the squid which |
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15:27 | going to be a lot more saline ours. So it will be high |
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15:33 | of sodium chloride. And so these the only concentrations also differ by species |
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15:38 | environments and which surround those different You can get all of the |
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15:43 | Now you know what's the concentration of your four major ions. Now you |
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15:50 | use a equilibrium potential formula to calculate . This is an example of |
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15:55 | sodium is abundant on the outside. will be driven into the cell down |
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16:00 | concentration gradient with a sodium ions and charge accumulate on the inside of the |
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16:06 | sodium gets repelled by its own electrical reaches its equilibrium potential value. So |
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16:17 | pumps are different and the pumps always against concentration gradient. We use |
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16:22 | T. P. And the export sorry. The import to potassium stand |
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16:31 | the export sodium always against the concentration is always never changes the direction. |
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16:38 | reverses and uses energy 80 p. do so. Yeah. So now |
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16:44 | you look at these major ionic sodium potassium calcium chloride, what you're |
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16:49 | is known concentrations of these ions on outside in mill imola and on the |
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16:57 | and we talked about how the greatest or the greatest disparity and ratio exists |
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17:04 | calcium. Uh huh. And additionally can also this is useful for calculating |
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17:13 | equilibrium potentials and you will need a for the exam that you'll need to |
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17:18 | the variables and the values that we're . Yeah. Answer properly the questions |
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17:23 | the movement potential but It's five million on the Outside for potassium. 100 |
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17:32 | the inside. So another way of it is 1-20. The ratio of |
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17:38 | on the outside vs. Inside. 20 times more potassium On the inside |
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17:43 | the selling outside. There's 10 times sodium on the outside of the cell |
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17:49 | inside of yourself. Huh? So can either use the minimal of |
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17:54 | you'll see how it plays in the time or you can use the ratios |
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17:58 | the science inside versus outside. And you can see at 37 C because |
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18:05 | temperature dependent equilibrium potential potassium is sodium is 62, calcium 123, |
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18:14 | chloride -65 minus 70. And by way these values are slightly different in |
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18:22 | books. Like for example, here will say wait a second, you're |
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18:26 | us that reversal potential for potassium is 80. And here it says reversal |
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18:31 | for potassium is 102 You're telling us five inside and 100 outside and this |
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18:39 | here there's 135 inside and three So I'm not going to confuse you |
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18:47 | I'm not going to ask you three 65 480 was 80, 70. |
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18:58 | And why is there a difference? measurements are taken from slightly different neurons |
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19:04 | they're slightly different neurons express different subsets these channels and they have maybe variations |
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19:10 | the local concentrations of the ions Mhm. So this is this is |
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19:16 | this is the disparities and you'll see of these disparities and that's not something |
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19:21 | worry about. What is to worry is understanding the main variables that learns |
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19:28 | equation. So you have 23 Ion stands for equilibrium potential 2.3 artie |
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19:37 | zf log of ion concentration on the of the cell versus ion concentration on |
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19:43 | inside of the south R stands for constant and t. Is absolute temperature |
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19:49 | in this case we're using 37 why? Because of his body Physiological |
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19:56 | temperature is 37 7. Again, is the charge of the ion or |
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20:02 | valence of the ion. So it's for mono Vaillant. It's too, |
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20:09 | -1. For an eye on this haven f is an electrical or Faraday's |
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20:17 | . So you have two constants gas third a constant. You know the |
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20:21 | which is 37° centigrade. And if plug in a single mama valent Cat |
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20:31 | on such as potassium or sodium, can abbreviate and collapse this 2.3 artie's |
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20:42 | , Into what becomes 61.54 million So this this whole 2.3 are TCF |
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20:51 | available value 61.54. And then you to plug in the outside concentration of |
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20:59 | versus the inside concentration of potassium. you do that here on the |
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21:04 | there's little potassium 1 to 20. this ratios I was just discussing and |
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21:10 | slide about But you can plug in actual values, you can plug in |
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21:15 | million mole and 100 million moller into nearest equation. Or you can just |
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21:19 | in the ratio. It will mathematically make a difference, 1-20. So |
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21:24 | you plug in This calculation here, log 1/20 is -1.3 And you multiply |
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21:36 | 1.3 times 61.54 million balls. You have a equilibrium potential value for |
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21:46 | So this is how you calculate You don't need to know how to |
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21:49 | the narcissist equation. You don't need use the calculator to calculate it, |
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21:55 | you have to be able to recognize differences. Let's say if the noticed |
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22:01 | is written where there is 20 potassium the outside and zero on the |
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22:11 | you know this is wrong. So have to know these values. You |
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22:15 | have to know the calculation. You to recognize what is the RtC. |
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22:20 | . You also have to recognize that you pull again a cat eye on |
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22:25 | into the Z into the valence value get 61.54 abbreviation, 61.54 for Mama |
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22:32 | Ion. This value becomes -61.54. ? Because you plugged in chloride which |
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22:42 | -1 for violence In the case of which is a dive. A |
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22:49 | A tie on. This abbreviation becomes Because you have to divide it by |
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22:57 | , You plug in valence of 2-plus over here. So when you do |
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23:04 | calculations and the abbreviation for each eye You have the individual equilibrium potential values |
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23:11 | region for these ions. Okay, is a liberal potential values freeze on |
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23:18 | centigrade. Okay, this is for eye on each ion has its own |
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23:24 | potential. But the plasma membrane contains for multiple ions which means that the |
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23:33 | potential of the plasma members. We're talking about equilibrium potential. When we |
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23:37 | about the equilibrium potential for one we're talking about that specific ionic channel |
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23:42 | the chemical and electrical forces opposing each . That's what we're talking about. |
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23:47 | we talk about the equilibrium potential, we talk about the number of |
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23:51 | it has to do a lot with chemical and electrical forces but it's not |
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23:56 | on just one high on. And to do the calculation for Goldman equation |
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24:03 | for the membrane potential we use the one equation And goldman equation has two |
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24:10 | from nerves equation. The main difference that it has a permeability ratio it |
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24:19 | the permeability value. What is the for potassium? What is the permeability |
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24:26 | sodium? The other thing that it , it's not for one ion. |
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24:31 | is a calculation that incorporates potassium and if you want to you can add |
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24:37 | too. And this tells you that overall VM. It's not E. |
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24:44 | . Which is a liberal potential for DNA equilibrium potential sodium. This is |
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24:49 | . The number of potential value is using the same abbreviation from the previous |
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24:54 | . T. Z. F. have to monitor villain Catalans here and |
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25:02 | what else? The premier ability. then this calculation shows that if the |
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25:08 | membrane I am from the ability to is 40 times greater than it is |
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25:15 | sodium, then this is the solution you will get. Okay. What |
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25:22 | that mean? That means that at you sunk in that electorate and you |
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25:29 | negative 65 millibars. When the selling is not very active At resting number |
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25:34 | potential. The foster lifted by. is 40 times more permeable to potassium |
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25:41 | . This is the biophysics. The of this plasma membrane neurons are slowly |
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25:47 | potassium. That's what the cell number his most permeable to. So addressed |
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25:54 | is dominating the membrane potential and sodium very little permeability. That for the |
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26:05 | rule or ratio if you make 40 more permeable to potassium versus sodium changes |
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26:13 | the number of potential changes. And you enter the action potential phase two |
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26:18 | the cell phone, Ostpolitik beyeler becomes impermeable to sodium and and some other |
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26:25 | things started happening. No. Let me put this in perspective in |
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26:32 | class supporting materials. You have this that I drew last year and I |
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26:40 | recommend that you draw the slide and these values on there. So maybe |
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26:45 | can dedicate a half a page to page of your mouth because this is |
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26:49 | you're going to be able to understand . And also answer quite a few |
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26:56 | about the action potential. I'm going show you the slide now, but |
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27:00 | going to come back and talk about slide in the minutes. The reason |
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27:06 | I want to show you the slide first of all, you have the |
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27:10 | scale and the Y scale is in balls. Uh and you're measuring |
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27:18 | which is member in voltage remembering potential in voltage member of potential. This |
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27:24 | zero value here. Our Mp stands resting membrane potential, Resting membrane potential |
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27:35 | -65 million ball value here. It's line here. But as I |
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27:42 | address the cell is fluctuating a little here. It's deep polarizing, a |
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27:48 | bit hyper polarizing a little bit. it will be following this this line |
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27:52 | this. Okay, up and down and down up and down. |
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28:00 | You have the equilibrium potential values here have a equilibrium potential value for calcium |
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28:06 | chloride and for potassium. So once equilibrium potential value which is calculated by |
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28:16 | equation is for one eye on value it's electrical forces for the ion oppose |
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28:25 | are equal to the chemical gradient. potential for VM is dictated by several |
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28:34 | ionic species which saw example address that's by sodium and potassium and it's very |
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28:41 | dependant on permeability cell number and may a lot of different channels and say |
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28:47 | have a lot of sodium channels that channels are closed. So the cell |
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28:51 | is not permissible to sodium. So becomes not a significant contributor, chloride |
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28:58 | not a significant contributor. But those change this resting number and potential. |
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29:04 | the cell is receiving excitatory glutamate vitamin synopsis are activated to sell D |
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29:13 | , the cell D polarizes, the becomes more positive. If the cell |
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29:19 | receiving inhibitory inputs, inhibitor synapses are , the cell will be hyper polarizing |
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29:27 | the cell will go down to the again, positive emphasis will come back |
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29:32 | the positive If it reaches this value is actual potential threshold value of about |
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29:39 | million barrels produced this event and not or non event which is the actual |
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29:48 | event. Mhm. If the excitation strong enough and excitatory synapses are activated |
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30:02 | it drives the member and potential to threshold value for action potential. The |
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30:08 | will produce is very fast deep polarization the form of the action potential produces |
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30:15 | very fast deep polarization will have a influx of sodium and then it will |
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30:22 | followed by the following phase of the potential. The potassium e flux is |
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30:29 | to be dominated, it's going to to this level here and get slowly |
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30:34 | to the resting number and potential. the help of that make a |
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30:39 | Okay, so now you understand what's potentials? Each eye on each island |
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30:48 | its own channel. Each island has own equilibrium potential. But these ions |
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30:53 | part of the bigger game. And membrane, they're part of the several |
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30:57 | that are flexing back and forth. part of the several channels that have |
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31:02 | own opening and closing kinetics and some them could be open and some of |
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31:07 | could be closed. Sure. Okay for for you for a second, |
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31:22 | slide kind of overviews everything you've learned resting, remember and potential bonds law |
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31:33 | circuit the main cells in that the building blogs of this protein |
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31:39 | the selectivity of these channels, the , the diffusion concentration gradient and also |
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31:48 | electrical gradient. Of course, the of the neurons potential just overlap with |
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31:58 | of the slides. Yeah, Goldman , this is the major difference. |
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32:07 | ? This is the nicest equation where have each ion with its concentration and |
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32:13 | equation where you have to you can a third eye on and see how |
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32:17 | changes the calculation here, How it the voltage value if you want |
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32:23 | And also the permeability ratios for these . A very important thing that we |
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32:30 | where we discussed astrocytes was that We said when we talked about, |
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32:35 | are responsible for synaptic transmission for uh of the neurotransmitters. So their end |
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32:46 | are involved in synoptic regulation, Synoptic regulation. And the other end processes |
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32:52 | feet are involved in blood brain barrier what things enter into the interstitial space |
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33:00 | the brain. Yeah. Astra sites these very extensive branches and as specific |
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33:09 | are interconnected with other ostracized, it's the brain through gap junctions. So |
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33:14 | electrical junctions that allow for the passage ions across different cells. It's very |
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33:22 | because the ionic concentrations, if you an ionic concentration you can change the |
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33:30 | potential overall membrane potential of the sell quite a bit. And this is |
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33:35 | example of how extra cellular potassium, is potassium k Plus on the outside |
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33:41 | milan moller and normal potassium is about to 5 million moller in this range |
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33:48 | in the outside concentration this outside normal of potassium, the membrane potential value |
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33:56 | close to -70 -65 million balls. if you change the Miller moller concentration |
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34:04 | potassium to 10 million balls, Look where you are already, you're about |
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34:10 | million balls. So if you change concentrations of ions locally on the outside |
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34:19 | the cells, you can change the membrane potential Which is influenced by other |
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34:26 | and it will now influence other aisles well. If you change this to |
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34:31 | million more Year at -40 million what does that mean? The cell |
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34:39 | be starting to fire action potentials. if you increase potassium concentration from the |
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34:46 | of the south to 10 15, million moller you will generate abnormal firing |
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34:52 | neurons. You will generate abnormal synchrony high potassium. A lot of models |
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34:58 | different lives biochemistry, electrophysiology neuro lives used potassium chloride, high potassium florida |
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35:04 | listen. A lot of selectivity. potassium is also a model for generating |
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35:12 | activity by d polarizing the south and abnormal synchronization. So astrocytes come in |
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35:19 | handy because they're supervised the synaptic transmission they supervise these local changes in the |
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35:28 | and as soon as their local rises potassium concentration on the outside astro science |
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35:36 | slurp up this potassium will distribute it its own cellular network and then we'll |
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35:47 | it through the interest connected a specific networks, essentially balancing out any local |
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35:55 | persistent increases in ionic concentrations. Its buffering it spatially buffers potassium concentration from |
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36:04 | active neurons, very active brain regions networks and buffers it to essentially avoid |
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36:13 | situation where there's too much potassium and much deep polarization of the plasma membranes |
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36:19 | too much firing of neurons causing abnormal . See how this is still part |
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36:28 | the Galileo function. Astra sites we about, we call them I think |
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36:35 | chores and again, you know if don't do household chores, you know |
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36:41 | car chores like fill up the gas kind of driving when it runs out |
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36:45 | gas. So it's very important course and it tells you that ostracized and |
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36:52 | can now influence and regulate neuronal excitability they do so by spatial buffering of |
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36:59 | that do so. So you later neural transmission by cycling with the neurotransmitter |
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37:07 | and before we move and go back talk about action potential. Again I |
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37:13 | to highlight this person that I highlight year and uh I wish actually I |
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37:20 | just read his story. Maybe it's little bit longer or maybe you talk |
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37:26 | it in a much longer way. Dr roderick Mackinnon uh medical doctor is |
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37:34 | medical doctor and uh Harvard and he very interested in the protein channel |
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37:45 | So you have to realize that what understand about these channels that they're building |
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37:51 | amino acids that the form the structure tertiary co ordinary that they have all |
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37:56 | least of the units that we can protein structures and now we can calculate |
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38:04 | without even visualizing them. I don't if you guys heard but last year |
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38:08 | was a big breakthrough, artificial Being able to calculate protein structures better |
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38:16 | X ray crystallography. Which actually allows to visualize the protein structures. That's |
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38:22 | significant. But at the time when Mackinnon did his MD, he wanted |
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38:28 | know what structure and function those channels . Imagine you have this long string |
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38:35 | amino acids. Now you kind of wound it up into sausages, sheeted |
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38:42 | up, flat it up, you , made sub units. Not all |
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38:48 | these sequences are very important. And roderick Mackinnon wanted to know which sequences |
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38:58 | important, which sequences controlled the opening closing of these channels. And so |
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39:06 | you have simpler systems. You can to fruit flies and say, what |
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39:10 | you doing with fruit flies and studying channels and making things like shaker |
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39:16 | It's a potassium mutation in the in fly that makes the fly shape. |
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39:21 | fly is essentially a productive. What that have to do with the |
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39:27 | Well, we have conserved amino acid which means we have certain parts of |
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39:35 | very large protein. Certain sequences could conserved in fruit flies and warms in |
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39:44 | and other higher low order species shared . So if you identify sequence in |
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39:53 | fruit fly and the potassium channel that important. Let's say that that sequence |
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40:00 | the keyhole. The whole door is large. How do you unlock the |
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40:10 | ? It's just a little tiny mechanism the actual key. Not even the |
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40:16 | hall. Just make sure that the of the key match precisely. It |
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40:21 | the door. And then do you the entire door when you open the |
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40:27 | ? You lower the handle when you the handle. Some doors have springs |
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40:33 | they will help you open them. this whole sequence of the pro dam |
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40:41 | very important to have the door. the key, the one that unlocks |
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40:47 | door or the handle, the one opens the door are the most important |
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40:53 | . And if you find that they're and you mutate them and you see |
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40:57 | change in the channel function then you're something. So he used side directed |
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41:03 | genesis to do these mutations. And potassium channel. We also use toxins |
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41:10 | electrophysiology use toxins because nature makes very molecule, spiders, snakes, fish |
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41:21 | , whatever it is and those molecules staining molecules will bind us. Their |
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41:27 | sequences. They could be the key fits into the keyhole and keeps the |
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41:33 | shut. It interferes with the mechanism opening the door. It could be |
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41:38 | opposite, it could be binding on side of the door and preventing it |
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41:44 | closing completely. Just keeping it barely . This is what these toxins do |
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41:49 | binding to different sequences. Then the . And we'll talk about this later |
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41:54 | the course when we talk about agonists antagonists. But agonists of the substances |
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41:59 | will open the channels, antagonists of substances that will close the channels. |
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42:05 | you will use electrophysiology because if you the channel there's gonna be more current |
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42:12 | more conductors through that channel. So , you know that you either mutated |
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42:17 | or you've used the toxin to a sequence, a certain part of this |
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42:23 | that now opens the channel a lot . Use another mutation, you use |
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42:28 | talks and now you found a part this long protein structure that is responsible |
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42:34 | keeping the channel closed, not closing keeping it closed. Then you find |
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42:40 | part of this pro to him that responsible for closing or opening the |
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42:47 | So this is what roderick Mackinnon And he's using these models and he |
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42:54 | a lot and uses mathematical models to predict the structure of the potassium |
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43:02 | But then he says, I'm still happy because I want to visualize the |
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43:10 | . So he then gives from this , flies gene mutations and establishes a |
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43:19 | Brexit crystallography and his colleagues tell him , you know, you're kind of |
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43:25 | little bit nuts because you did. . You kind of did a one |
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43:32 | and postdoc and professorship with the structure mutations. Now you're going to do |
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43:38 | PhD imposed up in professorship in X crystallography which is completely different from electrophysiology |
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43:46 | molecular biology, its biochemistry, it's a tiny protein inside a crystal. |
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43:53 | projecting X ray across that protein inside crystal, visualizing its structure. Using |
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43:59 | of the other tools including mathematics, finally derive the precise structure with the |
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44:08 | included. And so when his colleagues , you know, what are you |
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44:12 | , you're like entering completely new He says don't worry about it. |
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44:15 | one of the visual as his So he does extra crystallography and all |
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44:20 | his studies. All of this persistent over decades uh leads to this beautiful |
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44:26 | potassium channel here, the innermost limit . And he also describes the hairpin |
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44:35 | which is the selectivity filter inside the that allows for the passage of different |
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44:43 | species that we talked about, such potassium or sodium. And the reason |
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44:47 | I like his story is Path of the book. This is the section |
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44:53 | Path of Discovery. The reason why like his story is because he has |
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44:58 | goal. He has a passion and goal is to understand and to visualize |
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45:08 | channel to understand the structure. To this function structure equals function, adjusting |
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45:14 | , adjust function and so adjusting function structure to. They're both interconnected that |
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45:21 | his goal. And that is his . In other words, his fashion |
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45:25 | not to have an MD tag on flap coat are PhD tiger on his |
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45:32 | coast or a second huge d tire his lap code and some people would |
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45:39 | , well you know, you went medical school now, you're well you're |
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45:44 | deep into science. So he's passionately a goal and that's why I use |
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45:49 | example also because in career paths you wind in different ways. People pick |
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45:54 | a new career in their 60s, don't retire at 70 anymore. They |
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46:00 | new hobbies at 75. That means things and and pursuing your goals and |
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46:07 | your passions and you have to think things further in the future when you |
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46:14 | about yourself, if your career this and graduate next year, I don't |
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46:18 | the forget it. You know like have to do it now. My |
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46:21 | told me I need to have PhD now law medicine, you know, |
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46:28 | a goal and it may take you this way, stopping, turning |
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46:35 | going this, going this way, . Skyrocketing. When you hear stories |
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46:41 | all of the entrepreneurs and billionaires in the world. You on mosques and |
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46:49 | such. You hear those stories, , Second register 3rd Richardson, how |
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46:56 | he done amazing right. He's an or something or not. Your |
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47:04 | Unbelievable. What about 15 stories of failures before that one success About 15 |
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47:15 | nighters to earn a grade that leads to a degree that leads you to |
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47:21 | amazing opportunity that you never had. you don't highlight the failure story is |
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47:28 | lot of times. But in life a list and the mistakes a lot |
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47:33 | times will make you more experienced. . And it will work smarter and |
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47:41 | harder. But you have to go the grind and you have to do |
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47:46 | yourself and make mistakes and reading other stories. And I'm going to help |
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47:51 | . But having a perspective and that , having multiple avenues forks into leading |
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47:59 | the end goal and having time that potentially no limitation is a good and |
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48:09 | way to look in the future. . All right. So now we |
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48:16 | on to the action potential And now going to learn everything about from resting |
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48:21 | potential state where the cell is not active to when the cell gets |
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48:26 | The rising phase, the overshoot about Noah balls. The falling phase. |
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48:31 | undershoot, which is below the resting and potential. And rebuilding of this |
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48:37 | into the resting membrane potential with the of the epa's palms. Remember, |
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48:43 | the morse code, It's the morse . If you think of everything that |
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|
48:50 | at the resting membrane potential, everything happens, what we call sub |
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48:55 | Sub threshold is that threshold potential value action potential generation -45 syllables. Everything |
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49:02 | happens in this range between -45 and cells don't go lower than about -90 |
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49:09 | balls. And they never stabbed minus 90 because minus 15 minus 60 65 |
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49:19 | , 60, 70, 66 surround walk the resting number and potential. |
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49:24 | you can imagine that this random walk an analogue code. These are synaptic |
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49:32 | . And the action potential is all none. So what? It is |
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49:38 | or 1 But in digital code. . And it's a very fast digital |
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49:44 | . So you have essentially both sort analog coats of threshold and the digital |
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49:51 | . That is the action potential Alright, for this. I'm gonna |
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49:57 | into when I thought I had it , wait a second. I must |
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50:12 | been here almost closed it. so when we start talking about the |
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50:21 | potential, I really like this old . If we should watch and understand |
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50:26 | it's sort of all began understanding of action potential is in studying national potential |
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50:39 | business. Right. Mm. The bonds, body plans and have it |
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50:53 | because of humans and all those behaviors another world. So it's not surprising |
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|
51:00 | took a long time for scientists discovered there are fundamental similarities treatment other systems |
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51:07 | parts. And yes, it was recognition of a useful difference in the |
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|
51:16 | system which enabled scientists to undertake research has led to a growing understanding of |
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|
51:23 | our own nervous system. The breakthrough that control the contraction of the mental |
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|
51:30 | using precautions. This archive shows a thing is tracking mental models. Even |
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|
51:39 | moderately science with inject a huge amount water with great force. Uh |
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|
51:46 | mm wow. In the mid the British geologist Professor Jay Z's young |
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51:53 | engaged in the study of Squeeze Young observed an array of large tubular |
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52:01 | , each as much as an enemy a squeeze mantle. I think structures |
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52:06 | never fill with blood. They were being blood vessels from their similarity surrounding |
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52:13 | young, they must be single Giant axons transmitted million ounces from the |
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|
52:19 | of the tissue called hysteria Gambia to natural models. Mhm. Using electro |
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|
52:30 | stimulated the surrounding fighters and how that can only produce large muscle contraction in |
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|
52:36 | battle for the large tubular structures remain . So these were indeed giant |
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|
52:49 | Mhm. Scientists proof we appreciate the of young findings. But here it |
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52:57 | an excellent bars and robust enough to with the beginnings available at the time |
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53:02 | one can survive for several hours when from many years. The interest in |
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53:12 | context of the giant Verizon could be and analyzed, leading to the discovery |
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|
53:17 | sodium islands were more concentrated outside the cell and potassium islands more concentrated |
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|
53:26 | I'm refilling the empty Exxon solution to chemical composition experimenters were able to unravel |
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|
53:32 | mechanisms of iron transport across the Okay, yeah. The general tax |
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|
53:42 | large enough fast enough the final electrodes be inserted through the cell membrane. |
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|
53:47 | into the accident in these early But fine glass tube was conserved. |
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|
53:59 | acts on and security friends. Oh. Mhm. Then the deal |
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|
54:23 | used to introduce a fine wire electricity was devoted to the inside and the |
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|
54:29 | the measure. But the formation of early impacts was far too rapid for |
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|
54:36 | study with any of the electrical measuring of the late 1930s, It wasn't |
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|
54:42 | the 1950s following the wartime improvement of equipment such as the capital greatest |
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54:49 | The major progress was made. Scientists that further in urban cross was transmitted |
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|
54:57 | an accurate way of electrical potentials. this all or nothing action potential regenerated |
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55:04 | by transient movements of Syrian cassie. Times across the middle membrane deception squid |
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|
55:13 | that song unravel. The mechanism cervical and propagation of the action potential. |
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|
55:20 | led directly to the development of drugs block action potential formation and those actors |
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55:26 | and effect painkillers and dentistry and minor . Yes. Yeah. Mhm. |
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|
55:42 | . Okay. Right. Pretty This is how it all came |
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|
55:56 | Isolating john toxins, tying them practicing fishing knots on the Exxon's |
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|
56:07 | accidental transport, slow fast uh external composition inside the cell concentration of islands |
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|
56:17 | the cell. Um And the recordings recordings of the action potentials with the |
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|
56:25 | scopes that became finally available. Uh . So for the action potential methods |
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56:35 | recording action potential, most of these inter cellular that we talk about |
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56:41 | So when we talk about electricity, and neurophysiology, you cannot do these |
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|
56:49 | uh inside the cells and living humans example. So you can do it |
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|
56:58 | mostly in the brain tissue and you do living animal brains with certain |
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|
57:05 | And you can see that intracellular recorded potential and so on the order about |
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|
57:10 | million balls. So you have about million old fluctuations about one to |
|
|
57:14 | That's how large of a change it in the plasma membrane, then how |
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|
57:20 | it is on the outside. You also record extra several action potentials. |
|
|
57:24 | so a lot of neurosurgical techniques. operative neurosurgical techniques. Before operations, |
|
|
57:31 | may utilize extra cellular recordings even in brain to shoot the humans. Those |
|
|
57:37 | are very small on the order of 100 microphones. So you need to |
|
|
57:41 | very powerful amplifiers in order to pick the action potentials or any activity from |
|
|
57:47 | outside of the cells. How does cell generate action potentials? Well, |
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57:52 | already talked about the fact that the receives an input. And if that |
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57:59 | is strong enough. And if that is excitatory, that means the cell |
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58:04 | going to de polarize and as it polarizes, it generates a number of |
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58:10 | potentials. So if you look at this is the current on top that |
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|
58:17 | injected into the south through the micro and these traces is what we call |
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|
58:22 | wave like pulses because they look We turn on current positive current and |
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58:31 | off positive current. If the cell a little bit of this current and |
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58:37 | can equate this small deep polarization, a little bit of this current too |
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|
58:43 | or weak stimulus or weak input. cell mate d polarizes plasma membrane and |
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|
58:50 | can see the cellular response of the potential is not square. And that's |
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58:57 | the membrane has resistance and capacity of . So you have to build up |
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|
59:02 | charge across possible membrane. It takes milliseconds. The membranes are very good |
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|
59:08 | overall it takes several milliseconds to build the charge. But the action potentials |
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59:14 | get generated if it's a stimulus or input is stronger. If there is |
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59:22 | deep polarization and more active. Synopsis for synopsis are engaged, the cell |
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59:29 | reach the threshold production potential will produce certain output, certain frequency of action |
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59:37 | the terminal. If that cell receives even stronger stimulus, a stronger deep |
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|
59:44 | that will respond by producing higher frequency action potentials. So in a way |
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59:50 | frequency of action potential. So the of action potentials over a certain period |
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59:55 | time, over a certain stimulus period time is equal to the strength of |
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60:02 | response, weak response or weak Sub threshold response, stronger stimulus action |
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60:12 | . Maybe a few really strong stimulus strong input. You generate a number |
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|
60:19 | frequency of action potential. So this one way in which the cells encode |
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60:26 | strength of the stimulus is through the and frequency of the action potentials that |
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|
60:33 | produced. Uh huh. Ionic driving . Yeah, that's what we discussed |
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|
60:44 | . I mentioned the driving force to when we said we're going to talk |
|
|
60:47 | the equilibrium potentials. We talked about equilibrium potentials. Let's look at this |
|
|
60:53 | example here. First of all you potassium channels and sodium channels here and |
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|
61:02 | of the channels are closed and there's membrane potential across plasma membrane. There's |
|
|
61:13 | car influx, there's no conductance, just reversal potentials for these two |
|
|
61:19 | There's nothing the channels are closed. the channels are closed there's no conductance |
|
|
61:25 | there's no charge accumulation. Now you potassium open potassium channels and potassium starts |
|
|
61:35 | the cell. Okay. And that and potential from zero value becomes |
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|
61:43 | Uh huh. And so you have conductance that is dominating and you have |
|
|
61:51 | potassium current that is greater than zero the ions are flexing. What happens |
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|
62:00 | potassium ions in this flux of ions the number and potential to minus 80 |
|
|
62:08 | revolts. You reach the equilibrium potential . That means that at this point |
|
|
62:18 | electrical force is equal and opposite to chemical force. And there is a |
|
|
62:25 | . You see the conductance of potassium actually greater than zero But the current |
|
|
62:32 | zero for a while because the driving , which is the difference between the |
|
|
62:39 | and potential and equilibrium potential for potassium zero here. If the number of |
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|
62:48 | is the same as equilibrium potential for eye on there will be a flux |
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|
62:54 | ion. So there will be conductance there will not be net ionic movement |
|
|
63:00 | means no current flow into one favoring one direction of that zero. |
|
|
63:11 | , let's look at the action This is just one eye on trying |
|
|
63:15 | reach its equilibrium potential value. I place it all within the context and |
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|
63:20 | slide the PowerPoint slide that I was earlier with the driving force and all |
|
|
63:24 | the potential values on it. So is happening at the rest is addressing |
|
|
63:30 | and potential. As we discussed, cell is leaking to potassium, potassium |
|
|
63:36 | is high. During the rising potassium conductance goes down, sodium channels |
|
|
63:43 | up this influx of sodium, more goes in, there's more deep |
|
|
63:48 | it's a positive feedback loop sodium This was dominating over potassium and the |
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|
63:55 | potential is going to positive values at rising at the very top of the |
|
|
64:01 | this deep polarization of action potential. you're actually reducing the driving force for |
|
|
64:09 | , increasing the driving force for potassium the falling phase is dominated by potassium |
|
|
64:17 | . So these phases four phases of potential. address. That's dominated by |
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|
64:24 | rising phase sodium falling face potassium and to rest which is dominated again by |
|
|
64:32 | channels being leaking. Mhm. Next we'll discuss voltage clown and I will |
|
|
64:43 | today's lecture by going over this one time. There's an action going on |
|
|
64:55 | the plasma membrane and it is resting at rest the plasma number and is |
|
|
65:03 | some excitatory inputs deep polarizes a little receiving inhibitor airports. This is the |
|
|
65:10 | member and potential that we're tracking. number of potential is dictated and is |
|
|
65:17 | on the interplay of four major ions potassium chloride, calcium. Each one |
|
|
65:25 | these ions has an equilibrium potential Nonce potential value reversal potential value on |
|
|
65:33 | sand, we can calculate the equilibrium values using the first equation. If |
|
|
65:39 | know that on the concentration of the RTZ f constant surveillance temperature log outside |
|
|
65:48 | inside. So we have the equilibrium Address. The numbering is about |
|
|
65:57 | This is zero millet balls Valium. is an overshoot well. This is |
|
|
66:04 | undershoot during the following phase of the potential. The membrane potential value falls |
|
|
66:11 | the resting number of potential value and gets rebuilt by sodium and potassium |
|
|
66:19 | So what happens here? And how this driving force influence the whole situation |
|
|
66:27 | rest? If you're addressing member and which is -65. The equilibrium potential |
|
|
66:34 | potassium is about -80 -19. So difference between B. M. And |
|
|
66:41 | . And P. And V. . E. K. Is a |
|
|
66:45 | big it's about $10 million. It's small driving force for potassium. It's |
|
|
66:51 | the rules of the biology that potassium are open and they're leaking. So |
|
|
66:56 | was dominated. Although the driving force is VM the difference between numbering potential |
|
|
67:03 | numbering potential is this trace here -65 . And the Vienna equilibrium potential value |
|
|
67:11 | sodium sodium have a big driving force . Yes it has a huge driving |
|
|
67:19 | . Remember the driving force is the between the membrane potential which is several |
|
|
67:24 | and the equilibrium potential for that ion has even greater driving force fluoride has |
|
|
67:32 | no driving force around its own equilibrium value. When the cell d polarizes |
|
|
67:39 | reaches the threshold value. This all non action potential event causes the opening |
|
|
67:45 | the sodium channels. sodium channels That means more sodium flexes in. |
|
|
67:51 | means more deep polarization. That means sodium flexes. Um more channels |
|
|
67:55 | More sodium flexes in. It's a feedback cycle. What sodium is trying |
|
|
68:01 | do is sodium is trying to drive overall number of potential. The overall |
|
|
68:08 | on toward its own equilibrium potential value positive 55 million balls. All the |
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68:15 | are open and we're rushing in but doesn't reach equilibrium potential value for sodium |
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68:21 | two reasons why. The closer the of potential value comes to the equilibrium |
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68:28 | value for sodium. The small of driving force gets for sodium and the |
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68:35 | force for potassium increases tremendously. These polarized potentials because the difference between where |
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68:42 | equilibrium potential for potassium is and where membrane potential is is great at this |
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68:48 | . Okay, so now you have situation where the driving force has |
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68:56 | The second reason why the member and doesn't reach equilibrium potential value for |
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69:03 | It's because of the kinetics of the channel. sodium channels actually close sodium |
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69:09 | when they open and sodium is rushing and more channels open. They also |
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69:14 | closed very quickly. So we'll discuss sodium channel kinetics and on thursday before |
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69:21 | review. So, it never reaches sea equilibrium potential. But now, |
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69:27 | is empowered which our island has the driving force. Now it's potassium sodium |
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69:35 | are closed. So, guess what now? potassium the fluxus influx me |
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69:42 | sodium coming in, potassium rushes out the cell. And what is the |
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69:47 | trying to do this is entity potentially that is trying to drive the potential |
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69:54 | to its own equilibrium potential value. , selfish sodium wants to take it |
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70:02 | sound equilibrium. potassium wants to take down to some So it succeeds and |
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70:07 | drags down between below the resting number potential because it's also a wiki to |
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70:14 | . And then, with the help sodium Ak TPS pump. It gets |
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70:19 | into the this fluctuating resting membrane potential during this rising and early falling phase |
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70:27 | the actions. With our show the is in the absolute refractory period. |
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70:33 | means that if you were to stimulate cell to produce a very strong stimulus |
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70:39 | that we were talking about that produces frequencies of action potentials. If you |
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70:43 | to do during this absolute refractory you would not be able to produce |
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70:47 | action potential. You have to rebuild channel kinetics. You have to close |
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70:53 | the channels, redistribute the ions across plasma membrane to prime it again for |
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70:59 | next action potential. At this very of the following phase of the action |
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71:04 | and the undershoot period. You have relative refractory period, which means that |
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71:12 | cell is less likely to fire if receives the stimulus of an input. |
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71:16 | if the stimulus and the input was enough, it could make the cell |
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71:21 | . So it's relative the factory. during the action potential itself, it's |
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71:28 | so you cannot have one action potential top of another action potential. And |
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71:32 | cell dynamics. And the channel dynamics to change. We polarized in order |
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71:37 | the south to produce the next action and to sustain the frequency of firing |
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71:43 | these action potentials throughout the continuous Sure. So when we come back |
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71:48 | thursday, we'll look at the sodium potassium channel dynamics. We'll discuss |
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71:54 | clown and tetrodotoxin. So we'll do half an hour of new material to |
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72:02 | this section and then we'll dedicate however it takes half an hour, 45 |
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72:09 | to review in any questions that you have. So if you don't |
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72:14 | please check with casa support before you with me. If you're having difficulties |
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72:20 | casa, please check your notes and . Uh the video points for the |
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72:27 | , Make sure you have access to and bring your questions to give the |
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72:32 | on thursday so we can have a session. You can guys do a |
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72:37 | study over the weekend and face Thank you all. See you |
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72:42 | Thank you for being on |
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