POTENCIAL DE MEMBRANA 1: Definición y factores que lo establecen — Transcript
Full transcript
- 0:09How’s it going? Welcome to Medical
- 0:11Led. Today we will talk about a very
- 0:14important topic to continue with this
- 0:16video program that we have practically
- 0:18dedicated to electrophysiology, and the
- 0:21topic today is the membrane potential.
- 0:24This concept is super important to know
- 0:26before getting into all the mechanisms
- 0:28and processes. related to the action
- 0:31potential. First, what is the membrane
- 0:33potential? What does this concept refer
- 0:36to? Here is the definition for you. The
- 0:39membrane potential is the difference
- 0:41between the intracellular charges
- 0:43represented by the Greek letter psi.
- 0:47Psi i means psi of inside, that is,
- 0:49inside the cell. And psi obviously has
- 0:53to do with the difference in relation
- 0:56to the extracellular charges, which is
- 0:59noted as psi of outside. Right, the
- 1:03membrane potential will depend on
- 1:05several factors. The most important are
- 1:08these three here, which I have put in
- 1:10bullet points and that we will discuss
- 1:13little by little. The first one,
- 1:16intracellular electronegativity. For
- 1:20this, I left you a drawing that will
- 1:23help us understand why
- 1:24electronegativity is involved here in
- 1:27the membrane potential. Well, the
- 1:30drawing basically represents a neuron.
- 1:33The neuron has a body, which would be
- 1:36this part here, right? It also has
- 1:39something we call dendrites, which are
- 1:41these extensions that allow it to
- 1:43receive signals from the outside
- 1:45environment or from other neurons as
- 1:47well, okay? From the soma comes what is
- 1:51called an axon, which is practically
- 1:53this extension of the neuron that ends
- 1:55in what would be a synaptic button,
- 1:57right? If we were to zoom in on the
- 2:01axon membrane here, we would find
- 2:04something like this. Right. We have
- 2:08here, if you notice, a blue line that
- 2:10delimits two spaces. An extracellular
- 2:15space, which would be this one here,
- 2:18and an intracellular space. Okay? Both
- 2:22inside and outside the cell we have
- 2:24different charges, and the charges are
- 2:26provided precisely by the positive and
- 2:28negative ions present. For example,
- 2:31here on the intracellular side we have
- 2:33a positive charge that is representing
- 2:35a potassium ion, right? This other one
- 2:38that is negative could be representing
- 2:39a phosphate. This positive one here
- 2:42could be another potassium and so on,
- 2:43right? Same thing out here, look, out
- 2:45here there is a positive charge that
- 2:47could be sodium, right? We know that
- 2:49sodium is the most abundant cation in
- 2:51this space. We can also have negative
- 2:53charges, such as what? Like chlorine.
- 2:55Okay? And if you notice, in most of
- 2:58these regions, both inside and outside,
- 3:00the charges are practically balanced.
- 3:03There is a positive, a negative, a
- 3:05positive, and a negative. However, as
- 3:08we get right up to the lipid membrane,
- 3:11we will notice that this changes. The
- 3:14fact is that negative charges
- 3:16predominate in the intracellular space.
- 3:19If you look here, that is, right up
- 3:21against the membrane, we have many
- 3:22negative charges. Negative, negative,
- 3:24negative. An occasional positive one.
- 3:26Maybe a potassium there, right? That
- 3:28moved in closer. Negative, negative,
- 3:30positive, negative, negative, negative.
- 3:32The opposite of what happens on the
- 3:34other side. Outside the cell, we now
- 3:37have a predominance of positive charges
- 3:39. It could be sodium, sodium, sodium,
- 3:41sodium, one negative. That could be
- 3:43chlorine there, right? Sneaking in,
- 3:44positive, positive. What does this tell
- 3:49us? Well, basically, if we had a
- 3:52voltmeter, right? that would allow us
- 3:59to measure the millivolts inside and
- 4:01outside using electrodes. I place one
- 4:04here and another that goes into the
- 4:06intracellular fluid. If I measure the
- 4:11difference between one and the other,
- 4:12what will happen? Well, the negative
- 4:16charge right in this part will be
- 4:19compared to the positive charge, and so
- 4:23I will find that the intracellular part
- 4:26is more negative. This difference is
- 4:30exactly what we call membrane potential
- 4:33, okay? And membrane potentials also
- 4:35vary according to the cell type. For
- 4:38example, here we have some resting
- 4:40membrane potential values, okay? In the
- 4:43case of our example, the neuron has a
- 4:45membrane potential of -70 mV. What does
- 4:48this mean? That the inside, that is,
- 4:51the intracellular space, is 70 mV more
- 4:54negative than the extracellular part.
- 4:58Yes, it varies a little here in
- 5:00skeletal muscle. If you notice here,
- 5:02the difference is even greater, it is
- 5:05-95 mV. Cardiac muscle -90. Smooth
- 5:08muscle -60. Okay? So, this means that
- 5:12the difference in smooth muscle is not
- 5:14as great as the one we have, for
- 5:15example, here in skeletal muscle. These
- 5:20four cells that we saw here, cells and
- 5:23muscle tissue itself, stand out because
- 5:26they are excitable tissues, which we
- 5:28saw in the previous video. I will leave
- 5:32the information for that video here for
- 5:34you to check out. What happens? Lastly,
- 5:38the erythrocyte is not an excitable
- 5:40cell, right? However, it will also have
- 5:42a membrane potential. This one, if you
- 5:45notice, is not that pronounced, okay?
- 5:47The difference is only -1 mV. Okay?
- 5:52With this, we would then be talking
- 5:54about the first factor. I repeat, the
- 5:56first factor that determines the
- 5:58potential would be intracellular
- 6:00electronegativity. What are the next
- 6:03ones? We have the diffusion of
- 6:05potassium and sodium. Okay? Let's use
- 6:07this same neuron example. Now I'll
- 6:09expand it a little bit more here. What
- 6:11do we have? Well, we have here the
- 6:16extracellular and here the
- 6:17intracellular. All right. They are
- 6:20flipped here with respect to the image,
- 6:21but basically we will also distinguish
- 6:23them by the type of ions inside and
- 6:25outside. The extracellular space, what
- 6:28does it have? Mostly it has sodium ions
- 6:30, right? Since we had just seen in past
- 6:34videos that sodium outside the cell had
- 6:37what? An approximate concentration of
- 6:43140, right? 140 milliequivalents. On
- 6:47the other hand, inside the cell, sodium
- 6:49, if you look, well, it's nothing like
- 6:51that, right? It is around 14
- 6:53milliequivalents. There is a much lower
- 6:56concentration of sodium inside than
- 6:58there is outside. Conversely, potassium
- 7:02, potassium is what predominates in the
- 7:03intracellular space, around 140
- 7:05milliequivalents. Now, out here,
- 7:09outside the cell, how many are there?
- 7:12Well, there is a difference and it is
- 7:14between 3.5 and 5 milliequivalents. Now
- 7:18, what does this tell us? The fact that
- 7:20there is a difference will mark a
- 7:22tendency for the ions to leave
- 7:24depending on the concentrations. First,
- 7:27what should we keep in mind? Potassium
- 7:30leaves the cell because of this
- 7:32concentration difference, thanks to the
- 7:34fact that there are specific channels
- 7:35that allow it to leave, okay? They are
- 7:38channels that are open so that
- 7:40potassium can leave and go from one
- 7:43side to the other. Okay? So, let's draw
- 7:45the line here. All right, that will be
- 7:50it, right? Let's imagine that inside
- 7:53the neuron we have precisely that
- 7:55membrane potential I mentioned, right?
- 7:57-90. Right, this will be the resting
- 8:01membrane potential by pure logic. What
- 8:08do we assume when potassium leaves the
- 8:10cell? Meaning, the positive charge that
- 8:13potassium has goes from inside to
- 8:14outside. What do we assume could happen
- 8:17to my membrane potential? It will
- 8:19change, of course, but which way will
- 8:21it change? If I am losing positive
- 8:24charges from the inside, that tells me
- 8:26that the potential will be even more
- 8:28negative, okay? So the potential would
- 8:30no longer be -90, it would be what? -94
- 8:33, or even less. If it kept leaving,
- 8:37well, even more so. However, what
- 8:39happens? Sodium, for its part, will
- 8:42also have a passive movement, but it
- 8:44will do so in the other direction,
- 8:46because sodium predominates in the
- 8:48extracellular space and it will enter
- 8:50through specific sodium channels. So,
- 8:54it will go this way. What happens now
- 8:59if I am putting positive charges inside
- 9:01the cell? Right? I am gaining positive
- 9:05charges. So, the potential difference
- 9:07that will happen now will not go down,
- 9:09but will go up. Okay? So, basically,
- 9:12what is happening? Potassium leaves,
- 9:14sodium enters. Now, you are surely
- 9:17wondering something. Okay, I am letting
- 9:19potassium out, right? And the potassium
- 9:21is slowly, but surely, leaving and the
- 9:23sodium is slowly entering, it is slowly
- 9:26entering. I mean, a moment will arrive,
- 9:28if we follow that logic, where almost
- 9:29all the potassium is outside and almost
- 9:31all the sodium is inside. How do I
- 9:33maintain these concentrations? And
- 9:35above all, how do I maintain this
- 9:37membrane potential? Well, now the third
- 9:39factor comes into play, which is
- 9:41precisely the sodium-potassium ATPase
- 9:43pump. What function will this pump have
- 9:46? As we saw in the membrane transport
- 9:50video, which I’ll leave up here for
- 9:53you to check out, this pump is in
- 9:56charge of translocating two potassium
- 9:58ions inside, that is, it brings in two
- 10:01potassiums and at the same time it will
- 10:04take three sodiums out of the cell,
- 10:07okay? So, three sodiums will go this
- 10:14way. That is, outward, and two
- 10:18potassiums inward. Got it. That is how
- 10:25the sodium-potassium ATPase pump works,
- 10:27right? And I repeat, why is "ATPase"
- 10:30added? Well, because for this pump to
- 10:33work, it precisely needs ATP molecules,
- 10:36right? Which we basically obtain from
- 10:39aerobic metabolism and metabolic
- 10:40pathways that, surely thanks to the
- 10:42videos we have uploaded in recent
- 10:44months, you are already familiar with,
- 10:46right? They are metabolic pathways that
- 10:49properly allow for generating cellular
- 10:51respiration and, therefore, ATP. Well,
- 10:54now, finishing up this video, all that
- 10:56remains is for me to thank you for
- 10:58continuing to watch all the Medical
- 11:00content. The second part of the video
- 11:04will be precisely about a couple of
- 11:06equations that are necessary to
- 11:07integrate today's knowledge, which
- 11:09would be the Nernst potential and the
- 11:11Goldman equation. We will leave those
- 11:14for the second part, and I hope you
- 11:16enjoyed this video.
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