The Nervous System, Part 2 - Action! Potential!: Crash Course Anatomy & Physiology #9 — Transcript
Full transcript
- 0:00What if everything you did, and thought, and felt could be communicated by pushing a button?
- 0:04It’d be like using the world’s simplest app -- one that just sends out a little ping,
- 0:07always at the same volume and length -- to communicate everything from, “It sure is
- 0:11cold in here,” to, “I love churros,” to, “Boy, I sure would like to breathe sometime soon.”
- 0:16Well, that is actually exactly how your neurons send ALL the impulses responsible for every
- 0:22one of your actions, thoughts, and emotions.
- 0:24When a neuron is stimulated enough, it fires an electrical impulse that zips down its axon
- 0:29to its neighboring neurons.
- 0:31But they’ve only got one signal that they can send, and it only transmits at one uniform
- 0:36strength and speed.
- 0:37What they can vary is the frequency or number of pulses -- like this [buzz buzz buzz] is
- 0:42distinct from this [buzz buzz buzz buzz buzz buzz buzz].
- 0:45And your brain can translate these signals, reading them like binary code, organizing
- 0:49them by location, sensation, magnitude, and importance, so that you know the difference
- 0:52between “turn up the thermostat” and “Oh my gosh I’m on fire.”
- 0:55That buzz, that nerve impulse, is called the action potential.
- 0:59It’s one of the most fundamental aspects of anatomy and physiology, and really life in general.
- 1:03It’s happening inside of you right now. And we want to make sure that you understand
- 1:06what all that buzz is about.
- 1:18Before we delve into how neurons communicate, we’ve first got to understand a little bit
- 1:21of our old friend electricity.
- 1:23Basically, think of your body as a sack of batteries.
- 1:25NO, I mean, you don’t look like a sack of batteries, I’m just saying that, your body
- 1:29as a whole is electrically neutral, with equal amounts of positive and negative charges floating
- 1:33around. But certain areas are more positively or negatively charged than others.
- 1:37And because opposite charges attract, we need barriers, or membranes, to keep positive and
- 1:41negative charges separate until we’re ready to use the energy that their attraction creates.
- 1:46In other words, we keep ‘em separated to build potential.
- 1:49A battery just sitting on its own has both a positive and negative end, and the potential
- 1:53to release energy. But it doesn’t do anything until it’s hooked up to a flashlight or
- 1:58a phone or a kids’ toy that lets those charges move toward each other, on the way converting
- 2:03electricity into light, or sound, or children’s laughter.
- 2:06In much the same way, each neuron in your body is like its own little battery with its
- 2:09own separated charges.
- 2:11It just needs an event to trigger the action that brings those charges together.
- 2:15If you’re thinking that this sounds more like engineering than anatomy, that might
- 2:18not be a bad thing. It might even help to think of your neurons in the same terms an
- 2:22electrician might use.
- 2:23Voltage, for example, is the measure of potential energy generated by separated charges. It’s
- 2:28measured in volts, but in the case of your body, we use millivolts because it’s a pretty small amount.
- 2:33In a cell, we refer to this difference in charge as the membrane potential. The bigger
- 2:37the difference between the positive and negative areas, the higher the voltage, and the larger the potential.
- 2:42And just like there’s voltage in your body, there’s also current -- the flow of electricity
- 2:46from one point to another. The amount of charge in a current is related both to its voltage and its resistance.
- 2:51Resistance is just whatever’s getting in the way of the current. Something with a high
- 2:55resistance is an insulator, like plastic, and something with a low resistance is a conductor, like metal.
- 3:00Now, when we talk about these concepts in terms of you, we’re typically talking about
- 3:04how currents indicate the flow of positively or negatively charged ions across the resistance
- 3:09of your cells’ membranes.
- 3:11And again, these membranes separate the charges, so they’re what provide the potential to
- 3:16convert the electricity into something useful.
- 3:18K, now that we’ve got Electricity 101 down, let's see how it works inside your nervous system.
- 3:22A resting neuron is like a battery just sitting in that sack that is you. When it’s just
- 3:28sitting there, it’s more negative on the inside of the cell, relative to the extracellular
- 3:31space around it.
- 3:32This difference is known as the neuron’s resting membrane potential, and it sits at
- 3:36around -70 millivolts.
- 3:37Where do those charges come from?
- 3:39Outside of a resting neuron, there’s a bunch of positive sodium ions floating around, just
- 3:44lingering outside the membrane.
- 3:45Inside, the neuron holds potassium ions that are positive as well, but they’re mingled
- 3:50with bigger, negatively-charged proteins. And since there are more sodium ions outside
- 3:55than there are potassium ions inside, the cell’s interior has an overall negative charge.
- 4:00When a neuron has a negative membrane potential like this, it is said to be polarized.
- 4:04Now, these ions didn’t just show up in this arrangement on their own. This is all orchestrated
- 4:08by one of the most important bits of machinery in your nervous system, the sodium-potassium pump.
- 4:14This little protein straddles the membrane of the neuron, and there are tons of them
- 4:18all along the axon. For every two potassium ions it pumps into the cell, it pumps out
- 4:22three sodium ions.
- 4:24This creates a difference in the concentration of sodium and potassium, and a difference
- 4:27in charges -- making it more positive outside the neuron.
- 4:31This difference is an electrochemical gradient, and you probably know enough about biology
- 4:35by now to know that NATURE HATES GRADIENTS! It wants to even out all of those inequalities,
- 4:41in concentration and in charge, to restore balance.
- 4:44But the only way to even out that gradient, is for the ions to pass across the membrane.
- 4:48Thankfully, the sodium-potassium pump isn’t the only way in or out of the cell -- the
- 4:52membrane is also riddled with ion channels, large proteins that can provide safe passage
- 4:57across the membrane, when their respective gates are open.
- 5:00And these gates open and close for different reasons, depending on their structure and purpose.
- 5:05Most are voltage-gated channels, which open at certain membrane potentials, and close
- 5:09at others. For example, sodium channels in your neurons like to open around -55 mV.
- 5:14But some others are ligand gated channels -- they only open up when a specific neurotransmitter,
- 5:19like serotonin, or a hormone latches on to it.
- 5:21And then we also have mechanically gated channels, which open in response to
- 5:25physically stretching the membrane.
- 5:27In any case, when the gates do open, ions quickly diffuse across that membrane down
- 5:31their electrochemical gradient, evening out the concentrations, and running away from
- 5:35other positively charged ions.
- 5:37This movement of ions is the key to all electrical events in neurons, and thus is the force behind
- 5:42every. single. thing. we think, do, and feel.
- 5:45Of course, not all of your body’s electrical responses are the same. And neither are the
- 5:48flows of ions going in and out of your neurons.
- 5:50If only a few channels open, and only a bit of sodium enters the cell, that causes just
- 5:55a little change in the membrane potential in a localized part of the cell. This is called
- 5:59a graded potential.
- 6:00But in order to send long-distance signals all the way along an axon, you need a bigger
- 6:04change -- one big enough to trigger those voltage-gated channels.
- 6:07That is an action potential!
- 6:09And your best bet for making that happen is to depolarize that resting neuron -- I mean,
- 6:14cause a big enough change in its membrane potential that it’ll trigger the voltage-gated
- 6:18channels to open.
- 6:19It all starts with your neuron sitting there at resting state. All of the ion channels
- 6:23are closed, and the inner voltage is resting at -70 mV.
- 6:26And then something happens! Some environmental stimulus occurs -- say like a spider brushes
- 6:31up against a tiny hair on your knee -- triggering those sodium channels to open, increasing
- 6:35the charge inside the membrane.
- 6:37Now, the stimulus -- and the resulting change -- have to be strong enough to cross a threshold
- 6:41for the true action potential to kick in and that threshold is about -55 mV.
- 6:46Remember that number. Because this is an all-or- nothing phenomenon. If the stimulus is too weak, and
- 6:51the change doesn’t hit that level, it’s like a false alarm -- the neuron just returns
- 6:55to its resting state.
- 6:56But kind of like Doc Brown hitting 1.21 gigawatts in the Delorean, once it hits that threshold
- 7:01-- you’re not going to travel in time, but you are going to see some serious action potential.
- 7:04At that threshold, the voltage-gated sodium channels open, and there are tons of these,
- 7:09so all of the positive sodium ions rush in, making the cell massively depolarized -- so
- 7:14much so that it actually goes positive, up to about positive 40 mV.
- 7:18This is action potential in … action.
- 7:21It’s really just a temporary reversal of a membrane potential -- a brief depolarization
- 7:26caused by changes in currents.
- 7:27And unlike graded potentials, which are small and localized, an action potential kicks off
- 7:32a biological chain reaction, which sends that electrical signal down the axon.
- 7:36Because each of your neurons has lots of voltage-gated sodium channels. So when a few in one area
- 7:40open, that local current is strong enough to change the voltage around them. And that
- 7:45triggers their neighbors, which triggers the voltage around them, and so on down the line.
- 7:49As soon as all that’s underway, the process of repolarization kicks in. This time the
- 7:53voltage-gated potassium ion channels open up, letting those potassium ions flow out,
- 7:58in an attempt to rebalance the charges.
- 8:00If anything, it goes too far at first, and the membrane briefly goes through hyperpolarization:
- 8:05Its voltage drops to -75 or so mV, before all of the gates close and the sodium-potassium
- 8:11pumps take over and bring things back to their resting level.
- 8:14Now when part of an axon is in the middle of all this, and its ion channels are open,
- 8:18it can’t respond to any other stimulus, no matter how strong. This is called the refractory
- 8:23period, and it’s there to help prevent signals from traveling in both directions down the
- 8:27axon at once.
- 8:28So that is the surprisingly simple app that your nervous system uses to let you experience the world.
- 8:34And because the voltages in this process are always pretty much the same -- the initial threshold
- 8:37around -55 mV, and the peak at depolarization at +40 mV -- your neurons only communicate
- 8:43in a single, monotone buzz.
- 8:45It doesn’t matter if it’s a spider on your knee or an elephant, a paper cut or stab
- 8:50wound, the strength of that action potential is always the same.
- 8:54What does change is the frequency of the buzz.
- 8:56A weak stimulus tends to trigger less frequent action potentials. And that includes if the
- 9:01stimulus is coming from you, like your brain telling your muscles to perform some task.
- 9:04If I need to do something delicate, like pick up an egg, the signal is low-frequency: [buzz...buzz...buzz...]
- 9:10But a more intense signal -- like trying to crush a can -- increases the frequency of
- 9:14those action potentials to tell your muscles to contract harder, and the message turns
- 9:17into something that you can’t ignore -- [buzzbuzzbuzzbuzz]
- 9:20Action potentials also vary by speed, or conduction velocity.
- 9:24They’re fastest in pathways that govern things like reflexes, for example, but they’re
- 9:27slower in places like your glands, guts, and blood vessels.
- 9:30And the factor that affects a neuron’s transmission speed the most, is whether there’s a myelin
- 9:34sheath on its axon.
- 9:35Axons coated in insulating myelin conduct impulses faster than non-myelinated ones,
- 9:40partly because, instead of just triggering one channel at a time in a chain reaction,
- 9:44a current can effectively leap from one gap in the myelin to the next.
- 9:48These little gaps are the delightfully named Nodes of Ranvier, and this kind of propagation
- 9:53is known as saltatory conduction, from the Latin word for “leaping.”
- 9:57But what happens when an action potential hits the end of its axon and is ready to do
- 10:01more than leap … and jump all the way to another neuron?
- 10:04That you will find out next time!
- 10:06Today you learned how your body is kinda like a big bag o’ batteries, and how ion channels
- 10:10in your neurons regulate this electrochemistry to create an action potential, from resting
- 10:15state to depolarization to repolarization and a brief bout of hyperpolarization.
- 10:20Thanks for watching, especially to all of our Subbable subscribers, who make Crash Course
- 10:23possible for themselves and for everyone else. To find out how you can become a supporter,
- 10:27just go to subbable.com.
- 10:28This episode was written by Kathleen Yale. The script was edited by Blake de Pastino,
- 10:32and our consultant is Dr. Brandon Jackson. It was directed by Nicholas Jenkins and Michael
- 10:36Aranda, and our graphics team is Thought Café.
- 10:39One more thing before you leave.
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- 10:51But younger people, not so much.
- 10:54And so we are creating Crash Course Kids. Hosted by Sabrina Cruz from NerdyAndQuirky,
- 10:58Crash Course Kids will start out focusing on fifth grade science, but will keep expanding
- 11:02to other topics as the the channel grows.
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