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Cardiovascular | Electrophysiology | Intrinsic Cardiac Conduction System

Ninja Nerd · 8,690 words · 40 min read

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0:07all right engineers in this video we are

0:09going to talk about

0:10electrophysiology this is an extremely

0:12important topic and the reason why is

0:15because the heart is so special it has

0:17the ability to intrinsically depolarize

0:20itself it doesn't really depend upon the

0:23nervous system we'll talk about how the

0:25nervous system like the extrinsic

0:26inovation of the heart can speed up the

0:29heart rate or decrease the heart rate as

0:31well as maybe even increase the

0:33contractility of the heart we'll discuss

0:34these things but again I want you to

0:36understand something about the heart the

0:37heart exhibits what's called

0:38automaticity what is automaticity so the

0:41heart exhibits a a very important

0:43characteristic and this very very

0:45important characteristic is called

0:49automaticity what is automaticity

0:52automaticity is basically the heart has

0:54its the intrinsic ability on its own to

0:58spontaneously deep polarize itself and

1:02then Trigger action potentials to send

1:04it out to all the other parts of the

1:06heart that is automaticity so one more

1:08time automaticity is the intrinsic

1:10ability of the heart to spontaneously

1:12depolarize and Trigger action potentials

1:15that are spread out all the entire

1:17myocardium the muscle layer of the heart

1:19to trigger the heart muscle to contract

1:22okay that is its intrinsic ability how

1:24does this happen let's get started on

1:26that so what I'm doing is I'm zooming in

1:30here on some cells so before we get into

1:32all that Nitty Gritty components of the

1:34cells I want to take a look at the

1:36larger kind of like gross structure of

1:38this so let's come over here to this big

1:39old heart so in the heart you're going

1:42to have two different types of

1:44components of The myocardium so when you

1:45look at The

1:46myocardium you have two parts so when

1:49you look at The myocardium it's actually

1:51broken up into two components one is

1:55it's broken into what's called nodal

1:58cells which are basically your

2:00non-contract house these are the ones

2:02that generate automaticity these are the

2:04ones that can spontaneously depolarize

2:06generate Action potentials so they don't

2:09contract these for to name a few is

2:11going to be like the SA node which

2:14stands for sinoatrial node AV node which

2:17stands for atrio ventricular node the AV

2:21bundle which is the atrio ventricular

2:23bundle sometimes you might even hear it

2:25referred to as the bundle of

2:28His and there's also going to be What's

2:31called the bundle branches and you have

2:33one bundle branch going to the right

2:35side of the heart one bundle branch

2:36going to the left side of the heart so

2:37for your bundle branches you have both a

2:41left and a right and you have these very

2:44specialized structures that are digging

2:46into very very small components of The

2:48myocardium and these are called your

2:50preni

2:51fibers so again with The myocardium

2:54there's two types of tissue one is these

2:58nodal cells and the noal cells are

3:00non-contractile cells they're the ones

3:02that can intrinsically depolarize

3:04generate action potentials and Trigger

3:05the contraction of the heart these are

3:08SA node AV node AV bundle or bundle of

3:10hiss right and left bundle branches and

3:12your peni fibers the other component of

3:15The myocardium is the contractile cells

3:18so these are the ones that consist of

3:20the actual contractile proteins these

3:23are the ones that consist of actin and

3:27mein and they consist of uh the you know

3:30the troponin and the tropomyosin we

3:33could just keep going on right they

3:34consist of a lot of these contractile

3:36proteins what else they're the one that

3:39actually consist of the sarcoplasmic

3:41reticulum so they consist of that very

3:42specialized structure called the

3:44sarcoplasmic

3:45reticulum so with that said two parts of

3:48The myocardium nodal cells and

3:50contractile cells the ones that are

3:52Contracting they make up the big big

3:54portion of the heart these are the ones

3:56that consist of these contractile

3:57protein units as well as psychop plasmic

3:59ium they're the ones that generate the

4:01force that pushes the blood out of the

4:03heart the nodal cells are the ones that

4:05set a rhythm or a

4:07pace where does this whole pacing or

4:10automaticity start and where can you

4:11find all these structures within the

4:13heart well you got to look right at the

4:15actual pacemaker of this actual

4:18cardiovascular system now that we know

4:19that the myocardium is made up of two

4:21different types of cells nodal cells and

4:22contractile cells we want to focus on

4:24these guys first these nodal

4:26cells where can you find these bad boys

4:29well we got to look at at the pacemaker

4:30we got to look at the one who's actually

4:31generating the heart rhythms or the

4:33sinus rhythm that's this guy he's

4:35actually located right here so what do

4:37we call this guy here he is called the

4:38SA node This Guy's super important where

4:43would you actually find him you're going

4:44to find him if we look here at the

4:45orientation of the heart this is your

4:47right atrium right this is the right

4:49ventricle this is the left ventricle and

4:51this is the left atrium so if you look

4:53into the right atrium right here you're

4:55going to find in the superior component

4:57of the right atrium just beneath this

4:59large vessel here called The Superior

5:01vnea you're going to find this

5:04crescent-shaped structure consisting of

5:06nodal cells that is called the SA node

5:08the SA node is the pacemaker he sets

5:10What's called the sinus rhythm now sinus

5:13rhythm for the SA node is generally he

5:15sets the pace at around 60 to about 80

5:19uh beats per minute now that's really

5:22important because when we have this type

5:24of pace that's the normal heart's

5:27ability so the heart can generate about

5:2960 to 80 beats per minute on its own

5:31without any extrinsic inovation okay

5:33without any autonomic nervous syis so no

5:35sympathetic effect no parasympathetic

5:37effect this is what it can generate on

5:39its own so this normal Pace that we're

5:42setting here around 60 to 80 beats per

5:43minute this is called your sinus rhythm

5:46okay so it's called your sinus

5:51rhythm okay that's your sinus rhythm so

5:54sinus rhythm is generated by the SA node

5:56where it's generating Action potentials

5:59right about 60 to 880 to trigger this

6:02actual heart to beat 60 80 times per one

6:05minute okay that's the normal Sous

6:07Rhythm now we're going to talk about how

6:09it generates Action potentials but

6:11before we do that we need to see where

6:12these Action potentials are getting sent

6:13to we need to know the normal conduction

6:15pathway so this guy is the one that's

6:18generally setting the pace when he sets

6:20this pace he sends this information from

6:23the right atrium into the left atrium

6:25how does he do that you know there's a

6:26specialized structure over here that's

6:29connecting the essay note over here to

6:31the left atrium kind of like a little

6:33special structure over here kind of

6:35spreads out like this it's coming from

6:37over here this right here is called the

6:39Bachman's bundle okay it's called

6:41Bachman's

6:43bundle so this is called

6:46Bachman's bundle and what happens is is

6:50these electrical potentials that Theo

6:52generates he can send some of these

6:54electrical potentials over here through

6:57Bachman's bundle to activate depolarize

7:00the Atria so Isn't that cool so you can

7:02send action potentials from the sa no

7:04which is in the right atrium over to

7:06depolarize the left atrium via Bachman's

7:09bundle another

7:11thing is we have to connect this SA node

7:13here to other parts of the Atria so we

7:16have to connect to other parts of the

7:17Atria so there's other parts here that

7:19can come and Supply different parts of

7:22the Atria here like this what is these

7:26guys here this is actually called the

7:28internodal pathway so all of these guys

7:31here will come out and stimulate

7:32different parts of the Atria and

7:33eventually converge onto that big

7:35structure right there but again what are

7:38all of these fibers right here that are

7:40coming from the essay node outward to

7:42all the other parts of the left atrium

7:43all of these fibers here like this one

7:45and this one and this one these are

7:48making up what's called your

7:51inter

7:54nodal

7:56pathway so saay note to Bachman's bundle

7:58is going from the right atrium to the

8:00left atrium to supply the left atrial

8:02myocardium from the SA node to these

8:04internodal Pathways this will supply all

8:06the other parts of the right atrium but

8:09eventually all of this internodal

8:11pathway will converge onto this second

8:13important structure what is the second

8:15important structure called this second

8:18important structure is called the AV

8:20node okay it's called The Av node the AV

8:25node is so important because look what

8:27he's doing so he's kind of peing

8:30underneath this actual uh pulmonary

8:33trunk here it's actually running from

8:35the actual right atrium and into the

8:37actual this whole thing right here what

8:38is this big structure right here if you

8:40guys watched the video on the structures

8:41and layers of the heart you know that

8:42this would be the interventricular

8:43septum right so that's the

8:45interventricular septum what happens is

8:47this bundle here this AV node runs from

8:51the actual right atrium into the

8:53interventricular septum so it's acting

8:55as a connection the Gateway between the

8:58Atria and the ventricles because what

9:02happens is some of these potentials from

9:03the Bachman's bundle can actually make

9:06their way over here to the AV node also

9:09so some of the action potentials from

9:10the Bachman's bundle can make their way

9:13over here to the AV node so either way

9:15all of the action potentials that are

9:16coming from the SA node that are being

9:18spread out for the interal pathway or

9:19the Bachman's bundle are converging onto

9:21the AV node once the AV node receives

9:24these

9:25signals it's going to take a little bit

9:28of time how long it the actual action

9:32potentials here take about 0.1 second

9:35about 0.1 seconds which is a little bit

9:38longer than how much it takes for them

9:39to move through the SA node cells the

9:41Bachman bundle cells the internodal

9:43pathway cells so because it takes a long

9:46time what's the significance of this

9:47because it has

9:48significance one of the significance

9:51allowing for the AV node to take a 0.

9:53one second delay before it sends the

9:55action potentials down through the

9:56interventricular septum to the bundle of

9:58hiss is because it wants to give

10:02time for Atria to

10:06contract

10:10before the ventricles

10:12contract I can't express how important

10:15this is because of this 0.1 second

10:19delay it gives the time enough adequate

10:22time for the Atria to contract and push

10:24their blood into the left ventricle

10:26because if the AV no were to fire not

10:28have that1 second delay it would it' be

10:29depolarizing The myocardium while the

10:32left atrium and right atrium are trying

10:33to empty their blood into the ventricles

10:35if that's the case then as the

10:36ventricles are getting depolarized they

10:38might start Contracting at the same time

10:40that the Atri are Contracting that's

10:41counterintuitive we don't want that we

10:43want to allow for this guy to contract

10:44squeeze all the blood into the

10:45ventricles then let the ventricles

10:47attain the blood and then squeeze the

10:49vent squeeze the ventricles to push it

10:50out through the aorta and the pulmonary

10:52circulation okay now question is why

10:56does it take 01 second we know that it's

10:58the purpose it gives the time for the

11:00Atria to contract before the ventricles

11:01contract but there's two microscopic

11:04reasons

11:05why these nodal cells are riddled with a

11:08ton of Gap Junctions which are just

11:10basically channels that allow for ions

11:12to pass from cell to cell however the AV

11:16node which consists of a bundle of those

11:17nodal cells it has a lot fewer Gap

11:21Junctions than these other nodal cells

11:24so a lot less Gap Junctions so a lot

11:26less ions can flow from cell to cell

11:28that decreases the ual speed at which

11:30it's moving that's one reason that's why

11:31it takes a little bit longer another one

11:34is because they have a smaller diameter

11:37so the actual fibers are actually a lot

11:41smaller in diameter and if you know a

11:43little bit about conduction we know that

11:45the larger the diameter of the structure

11:47the faster the velocity of that

11:49conduction is going to move so the

11:50smaller the diameter the slower the

11:52conduction speed okay so again we went

11:55from SA node which was the first one

11:57through the Bachman's bundle internodal

11:58pathway into the AV node AV node was the

12:00second one took 01 second delay to give

12:02the time for the Atria to contract empty

12:04their Chambers so that the ventricles

12:06can attain the blood and then they can

12:08contract why does it take the 0.1 second

12:10delay because the AV node has less Gap

12:12Junctions and it has fewer D smaller

12:15diameter muscle fibers okay then where

12:18does it go from here it goes into the

12:21next structure here this next structure

12:24here is going to be kind of like a nice

12:27bundle it's consisting of a big old

12:29bundle right here this guy right there

12:32is called the bundle of hiss okay so

12:35this guy right here is called the bundle

12:37of His or the AV

12:39bundle when he receives these Action

12:41potentials from The Av node he then

12:43conducts it into these two bundle

12:46branches this bundle branch right here

12:49we're going to put here four is going to

12:51the right myocardium so this is the

12:53right bundle branch so which one would

12:55this one be right bundle branch over

12:58here this is going to the left

13:00myocardium so because this is going to

13:02the left myocardium what we say this one

13:03is this is the left bundle branch

13:07because it's going to left myocardium

13:09then from there it goes into these nice

13:11little breaking units you see how this

13:13is branching off branching off branching

13:15off branching off these bundle branches

13:17these are called your preni fibers okay

13:20so these are your preni

13:24fibers okay these are your peni

13:27fibers all right so let's go ahead and

13:29recap these let's recap them in order

13:31now I'm about to get a little taller

13:32okay don't you dare laugh at me I'm

13:34short all right so let's go ahead and

13:36recap the flow so how does it go we said

13:38first things first started at the SA

13:41node he's the pacemaker of the

13:44respiratory I'm sorry the pacemaker of

13:45the actual cardio Cardiovascular Center

13:47right specifically for this actual Pace

13:49setting of the heart rate then what

13:52happens he goes to the next one how does

13:54he get to this next one he goes to the

13:56AV node how does it get to the AV node

13:58remember it travel within the actual

14:00right atrium via the internal pathway

14:02but then the SA node can transmit

14:03impulses to the left atrium via the

14:05Bachman's bundle eventually all of those

14:07fibers converge onto the AV node though

14:10the AV node we said takes about a 0.1

14:13second delay because of the fewer

14:14diameter uh fibers and less Gap

14:17Junctions and to allow for the Atria to

14:19contract and then the ventricles to

14:20contract then from The Av bundle we go

14:23to the bundle of His or again you can

14:26call it the AV bundle doesn't matter

14:29from there it goes into the right and

14:31left bundle branches okay so we're just

14:34going to combine these you can go into

14:35the right and left bundle branches if

14:38it's the right one it's going to the

14:39right myocardium if it's the left bundle

14:40branch it's going to the left myocardium

14:42then from here you're going to go into

14:44the last one which is going to be the

14:46pereni system so the pereni fibers and

14:49this will supply different components

14:52within The myocardium and Trigger The

14:54myocardium to contract we did that now

14:58so now we've covered the actual cardiac

15:01conduction

15:02system okay

15:03sweet from there now what are we going

15:06to do we now now we know the cardiac

15:08induction system the actual gross

15:09anatomy like flow but now we got to be

15:11even more specific how does it generate

15:13these Action potentials how does it

15:15actually do it so now what we're going

15:16to do is we're going to do two things

15:18I'm going to take this sa noal cell I'm

15:21going to take out out of this sa no I'm

15:22going to take and expand on one of the

15:24cells then I'm going to take a piece out

15:28of the myocard and I'm going to expand

15:29that and look at one cell so we're going

15:30to look at two different types of cells

15:32we're going to look at a nodal cell and

15:34we're going to look at a contractile

15:36cell and see how these cells are

15:37communicating and what's all these ion

15:39channels and stuff okay so let's go and

15:41get

15:41started so this cell right here let's

15:44actually just toote it right away this

15:46is our nodal cell okay this is going to

15:48be the nodal cell and this one over here

15:51just so we can get right out of the way

15:53this is going to be the contractile

15:55cell now what did I tell you right away

15:59about the Cellular

16:01Connections we said these two cells okay

16:04because not only are nodal cells because

16:05look I could actually kind of make a

16:06tiny little mini diagram here I can say

16:08that if I have this nodal cell here this

16:10nodal cell could be connected to many

16:12other nodal cells and how could they be

16:15connected what are these little things

16:16that are connecting the nodal cells the

16:18actual Gap Junctions and so if I have

16:21Gap Junctions here this can allow for

16:23ions to pass from this cell to this cell

16:25to this cell to this cell right it's

16:27basically allowing for ions to pass from

16:28cell to to cell the same thing happens

16:31and exists between let's say that this

16:32is a nodal cell and just to make it very

16:34simple I changed the color of the actual

16:36contractile cell I make the contractile

16:38cell black these also have connections

16:42so if these have connections we can

16:43actually allow for ions to flow from a

16:45noal cell into a contractile cell and

16:48then help the contractile cell to start

16:50depolarizing so we're going to see how

16:52that happens but but first before we do

16:54that we got to see how does this guy

16:55depolarize

16:57itself so you know something funny

17:00within these noal cells very funny very

17:02very interesting little cells and they

17:04actually consist of what's called funny

17:07Sony sodium channels you think I'm being

17:09funny but I'm not there's actually funny

17:11sodium channels these channels that are

17:15within this nodal cell are very leaky

17:17and they allow for a little bit of

17:20sodium to leak into the cell very very

17:24slowly very very very slow flow of this

17:27sodium into this noal cell now generally

17:31nodal cells don't have a stable resting

17:33membrane potential normally resting

17:35membrane potential is like -70 toga 90

17:37MTS it depends upon the cell but these

17:40nodal cells don't really have a stable

17:41resting membran potential so their kind

17:43of membrane potential fluctuates but in

17:46general before these sodium channels uh

17:48these funny sodium channels open they

17:51generally are going to have a membrane

17:52potential

17:54around -60 molts that's approximately

17:57where it's at

17:59so now look what happens here let's

18:01let's represent these funny sodium

18:02Channels with

18:03blue these funny funny sodium channels

18:06start actually causing the inside of the

18:07cell to become a little bit more

18:10positive because we're bringing positive

18:11ions into the cell sodium as the sodium

18:15starts coming into the cell something

18:16else really weird starts happening as

18:18you approach the threshold potential

18:20sodium gets a little bit of help okay so

18:22first things first was the sodium is

18:24coming into the cell bringing some

18:26positive charges with it all right this

18:29happens around 60 molts but then what

18:31happens is these other channels they're

18:34called

18:37ttype calcium

18:40channels these are called t types

18:42calcium channels these calcium channels

18:44open

18:45up approximately around - 55

18:50molts so these positive ions are

18:52bringing it from -60 Mill volts to what

18:5655 because it's a really slow flow of

18:58sodium

18:59as it starts flowing in this 55 molts

19:02becomes a stimulus for these ttype

19:06calcium channels when they stimulate

19:08these ttype calcium channels start

19:09opening and calcium starts flowing in

19:11nice and slowly also so now we have the

19:13combined effect of these funny sodium

19:14channels what are these guys here called

19:18funny sodium

19:21channels these are your funny sodium

19:23channels these guys are slowly allowing

19:26for the sodium minus to trickle in then

19:28what happens happens is it stimulates

19:29these ttype calcium channels to come in

19:31once they reach about 55 as these

19:33calcium ions start accumulating with the

19:35sodium ions guess what happens to the

19:36membrane potential it becomes even more

19:38positive let's show that down here so

19:40now if you look you're going to notice

19:43that this is going to be representing

19:44the calcium channels and the sodium

19:46channels look oh shoot they hit

19:49threshold potential what is our

19:51threshold potential here generally

19:53within the cell the threshold these

19:54actual nodal cells is around -40 Ms

19:57normally it's like 50 five in most cells

19:59but in this one it's about

20:01--4 once we hit that -40 another type of

20:05Channel opens up when this channel opens

20:07up it blasts open a lot of calcium and

20:12you're going to see what happens here

20:13that this guy actually Rises pretty

20:15quickly here it rises up very very

20:19quickly and we'll see what happens here

20:21in just a second okay so for right now I

20:23want you to know that whenever we're

20:24inside the cell 60 Ms funny sodium

20:26channels open then around 55 these uh

20:29ttype calcium channels open then when we

20:31hit threshold what channels open these

20:34green channels what are these green

20:35channels here called these green

20:37channels are called L

20:39Type calcium

20:42channels so these are called your L Type

20:45calcium channels they're very very

20:46sensitive to voltage so once this

20:48happens it gets to around -40 Mill volts

20:50and guess who starts flowing in very

20:53powerfully calcium starts flowing in

20:55very very powerfully as the calcium

20:58starts flowing in in very very

20:59aggressively what would you expect to

21:01happen to the inside of the cell to

21:03become super super super positive and

21:05that's what happens look it goes up to-4

21:07and W shoots up how high does it go up

21:11to it generally goes up to

21:15approximately in this cell because the

21:17calcium is coming in very very very

21:19aggressively It generally comes in to

21:21approximately around positive 40 molts

21:26so it comes into about positive 40 molts

21:29as these L Type calcium channels open

21:30the calcium starts rushing in you're

21:32bringing a lot of positive ions into the

21:34cell and as you start bringing tons and

21:37tons and tons of positive ions into the

21:39cell what is it going to do to the

21:40inside of the cell it's going to

21:41depolarize the cell so what's the

21:43overall result here well let's actually

21:45kind of follow what happened here if we

21:46look at this in kind of like a nice

21:47little flow diagram here 60 MTS was the

21:51resting membrane potential the funny

21:53channels open and we brought it to 55

21:55mols right this was when we opened up T

21:58type calcium Chann but T calcium then we

22:01got it from that to threshold potential

22:02which is around 40 MTS this opened up L

22:06Type calcium channels then from that we

22:09took in this L Type calcium channels

22:11when they open calcium flooded in so

22:13aggressively that it completely flipped

22:15the membrane from -4 to about posi 40

22:18molts this is when it's

22:21depolarized so the inside of the cell is

22:23depolarized and extremely positively

22:26charged okay

22:29now we've depolarized the cell it didn't

22:31require any nervous system functioning

22:33isn't that beautiful now here's the

22:35thing how in the heck does that affect

22:37this actual contractile cell these

22:40beautiful Gap Junctions so what happens

22:43is is what are we accumulating a lot of

22:45inside of this cell lots and lots of

22:47positive charges lots of cations ions so

22:50as a lot of these cat

22:52ions are being loaded into these uh into

22:56these actual nodal cells what can happen

22:58well guess what these beautiful Gap

23:01Junctions are connecting they're acting

23:04as the communication Gateway between the

23:06nodal cells and other nodal cells or the

23:08nodal cells and contractile cells so

23:11what do these Gap Junctions actually

23:13made up you know they're made up of

23:13what's called proteins uh specifically

23:16called conin so they're called conin

23:19proteins so there basically a whole

23:21bunch of different types of

23:23conin now these cat I they actually move

23:28through these Gap Junctions into the

23:30other cells they can go from cell to

23:32cell to cell to cell to cell now because

23:36of that I'm bringing positive ions over

23:39into this cell through the Gap Junctions

23:42which is so darn cool but here's the

23:45thing how do we keep these cells so

23:47tightly close together so that the Gap

23:49Junctions aren't separating whenever the

23:51heart's being stretched because we don't

23:53want these actual Gap Junctions to get

23:55separated because it's actually two

23:56different proteins between the cells

23:57connecting together how do I actually

24:00prevent this from happening to keep the

24:01cells so tightly together we have these

24:04special structural proteins here what is

24:06this what is this protein here called

24:09this protein here is called desmosome

24:12okay it's made it has what's called

24:14desmo

24:15zomes now desmosomes are super cool

24:18because they consist of a bunch of

24:19different proteins like for example

24:21these green proteins here that are

24:22connecting the cellto cell lying for the

24:24cellto cell communication these are

24:25called

24:27cadherin and then these proteins here

24:29these blue proteins these are actually

24:31your your attachment plaques and there

24:33could be many different proteins that

24:34make this up it could be what's called

24:36um desmo

24:39plen there could be what's called uh

24:42other different types of chemicals we're

24:44not going to go into all of these

24:45different types I don't want to do that

24:46but there's many different types of

24:47proteins that are making up these

24:49attachment plaques

24:50okay then there's other proteins which

24:54are consisting of these other types of

24:55filaments here that are consisting of

24:57substances like Artin okay so we know

25:01that these desmosomes are basically

25:03acting as like adhesion molecules from

25:05cell to cell connecting the cells

25:08together keeping them very tightly

25:10connected that's really really important

25:12now that leads to a concept whenever I

25:15have two cells communicating together

25:17and I have a combination of

25:19desmosomes and GAP Junctions they

25:22decided hey let's give it a different

25:23name like always right let's let's let's

25:25give this a name so they said it's

25:28actually right over here they said that

25:31whenever you take Gap

25:34Junctions and you add into the

25:37mix

25:38desmosomes they're like oh you know what

25:40let's call

25:42this

25:44inter

25:47collated

25:49discs so inter collated discs are just

25:52basically a bunch of Gap Junctions and a

25:54bunch of Desmos zones connecting the

25:56actual cardiac cells together that's

25:59it so now again what will be happening

26:01over here a lot of cat ions sodium and

26:04and calcium ions are flowing through

26:06these Gap Junctions into this other cell

26:08this contractile cell how does this help

26:10the contractile cell all right let's

26:13see the cell starts becoming a little

26:15bit more positive right we'll see what

26:17happens whenever this cell relaxes in a

26:19second we'll do the relaxation period

26:20together let's keep going with the

26:22depolarization positive ions come over

26:23into this cell when the positive ions

26:26come over into this contractile cell we

26:28have have to think about what is the

26:29actual resting membrane potential of

26:31this cell this one's a little weird this

26:33one was like -60 we said the resting

26:35membrane potential of this cell is right

26:37around 85 to 90 molts okay so its

26:42resting membrane potential is in between

26:45like 85 to 90 Mill volts okay so right

26:49around that now these positive ions

26:54those positive ions that are leaking

26:55into the cell via the Gap Junctions they

26:58start trying to bring the actual

27:00membrane potential closer towards the

27:03threshold that's what they're trying to

27:05do they're trying to bring this closer

27:06towards threshold that's their

27:09purpose but what happens is along that

27:12way okay what's what's threshold

27:14potential within these cells threshold

27:16potential is approximately right around

27:1870 Mill volts within these cells so you

27:21see how different cells can have

27:22different resting member potentials and

27:24threshold potentials it depends upon the

27:26movement of potassium ions okay and

27:29we'll talk about that when we talk about

27:30resting membrane potential with the nerd

27:32equation but what happens is these ions

27:36these cat that are flowing into the cell

27:38are bringing the resting membrane

27:40potential closer to threshold potential

27:42as it does that we reach threshold and

27:45these specialized voltage gated sodium

27:48channels blast open let me see let me

27:51show you where these guys are so here

27:53are the positive ions what is it doing

27:55and originally the cell is at resting

27:57membrane potential it brings it to about

28:00threshold potential which is around -70

28:03molts this stimulates these voltage G

28:06sodium channels these voltage gated

28:08sodium channels start opening when they

28:11open who starts flowing in sodium and

28:14when sodium Flows In he Flows In very

28:17very fast as the sodium lons start

28:20flowing into the cell the inside of the

28:21cell starts becoming very very positive

28:24so it starts becoming very very

28:27positive as it becomes very positive

28:29this positive charge starts moving

28:32across the actual cell membrane or in

28:34this case what's the cell membrane of a

28:35muscle cell called It's called The ccma

28:38so these positive charges start moving

28:40in like a wave around the actual ccma of

28:44the muscle cell

28:45membrane so look at the graph what are

28:47we going to see we were originally at90

28:50we went to 70 through those Gap

28:52Junctions hit threshold potential and

28:54opened up what channels those voltage

28:56gated sodium channels and Rises

28:59up now it rises up kind of a little bit

29:02you know a little bit slower but um what

29:06happens is it gets to

29:09about positive around positive 10 molts

29:14so it gets to approximately around

29:16postive 10

29:18molts now along the way along the way

29:23throughout this process you're

29:24approaching positive 10 molts some other

29:27channels open up a a little bit and

29:28allow for a little bit of calcium to

29:29start trickling in so along this way

29:33another thing that can happen is if we

29:34look over here these black channels

29:36these black channels are calcium

29:37channels these are your calcium channels

29:40and along the way as the sodium is

29:42starting to approach and start causing

29:44the cell to depolarize some of these

29:47calcium channels start slowly opening

29:48only a little bit of them start slowly

29:50opening and calcium starts coming in too

29:52okay so start calcium starts kind of

29:54slowly trickling in also with the Sodium

29:56and this causes that Rising phase there

29:58there it gets to about positive 10

30:01molts when it gets to positive 10 molts

30:04the sodium channels inactivate okay so

30:07they turn off so now the sodium channels

30:09are closed but what else what other

30:11channels open a little bit a little bit

30:12of calcium channels are open very very

30:14little though not too many but what else

30:17decides to open up at the same time

30:19another channel that decides to open up

30:22at the same

30:24time over here is going to be

30:28pottassium

30:29these potassium channels they like ah

30:32you know what it's the perfect time for

30:34me to open up the cell is super super

30:37depolarized let me go ahead and open up

30:39a little bit because we're at positive

30:4110 mols that can't happen we got to

30:43bring it down a little bit so what

30:45happens is these potassium channels open

30:47up and they allow for pottassium ions to

30:49start coming out now the potassium ions

30:52start coming out a little bit more than

30:53the calcium ions are kind of slowly

30:55slowly trickling in so a lot of

30:57potassium ions are going to go out here

30:58for moment of time as that starts

31:01happening what starts happening to the

31:02inside of the cell it's losing positive

31:04charges it's becoming a little bit more

31:06negative what happens then because the

31:09pottassium leaks out of the cell for a

31:11moment it drops down a little bit weird

31:14right has a little drop and it drops

31:17from about 10

31:19molts to around

31:21zero so because of that because of that

31:24actual sodium ions coming in and a

31:26little bit of calcium trickling in it

31:28brings it up to posit 10 MTS at positive

31:3010 sodium channels close potassium

31:32channels open and potassium starts

31:34slowly leaking out a tiny tiny bit of

31:36calcium is coming in and it causes it to

31:39drop down to

31:41around 0

31:44molts when it hits Z molts the calcium

31:47channels those actual volt those voltage

31:49calcium channels become even a little

31:50bit more active they become even a

31:52little bit more active now so once you

31:54hit about positive

31:55zero I guess there is no such thing as

31:58positive z z is positive no matter what

32:01you hit zero Mill volts that becomes a

32:03very powerful stimulus for these L Type

32:05calcium channels okay so these are your

32:07L Type calcium channels as these hit

32:11positive zero they become a little bit

32:12sensitive and the calcium starts flowing

32:16in very

32:18powerfully okay it starts coming in

32:20these positive ions from the calcium

32:22starts coming into the cell but don't

32:25get that Twisted because guess what else

32:26is leaving out at the same time time

32:28just a little bit with it these

32:30potassium ions are also leaving the cell

32:33so because of that we're having

32:34potassium ions leave the Cell at the

32:37same time cat I calcium ions are coming

32:40into the cell so if you think about it

32:42positive ions are leaving and positive

32:43ions are coming in so really there's no

32:45change in the membrane potential well

32:47that's weird so what would that be then

32:50it's going to kind of plateau for a

32:52little bit and it's going to Plateau

32:54actually for a decent amount of time

32:55about 250 milliseconds that's pretty

32:58long time for a cell okay to be in this

33:00depolarized or plateaued like state so

33:03to get this clear first things first we

33:06have this 90 to70 that's due to those

33:09actual uh c those Gap Junctions bringing

33:12the actual ions in to get us to the

33:13actual threshold to allow for the

33:15voltage G the sodium channels to open up

33:17then after that there's a little drop

33:19that little drop there is do the

33:20potassium channels open and more

33:22potassium leaves out than calcium is

33:23coming in and it causes it to go to

33:25positive Z molts or zero molts once we

33:28hit zero those L Type calcium channels

33:30become a little bit more active open up

33:31and a little bit more calcium than

33:33normals coming in but because positive

33:35ions like calcium is coming in and

33:37positive ions like potassium are going

33:38out okay so it's going to Plateau then

33:41let me get some terms out of the way

33:42here just real

33:44quickly doctors I guess wanted to make

33:46it a little bit more complicated for us

33:47so they added

33:49phases the phases that they actually

33:51ordered in it goes from zero to four so

33:55this depolarization phase where the

33:57sodiums are coming in they call that

33:59phase zero okay so phase zero is where

34:01the sodium ions are coming in very

34:03aggressively through the that

34:04depolarizing current the voltage gated

34:06sodium channels then this little dip

34:08down where the potassium channels open

34:11and the potassium starts leaking out to

34:12bring the membrane potential from

34:14positive 10 to zero mainly potassium

34:16very little calciums are coming in this

34:18is called phase one the plateau phase

34:22which is where the calcium is coming in

34:23because we get it to positive Zer and

34:25pottassium are going out so positive

34:27ions are coming in positive Gs are going

34:28out so it's kind of staying around the

34:30same membrane potential not really

34:31changing much this is phase

34:34two now we're going to stay here at

34:36phase two for a little bit because we

34:38have to see how these actual calciums

34:40are leading to contraction so now look

34:42what happens

34:43here these calcium ions until recently

34:46they kind of came up with a theory of

34:48how these calcium ions are actually

34:49triggering the release of other calcium

34:52it's weird right calcium induced calcium

34:54releas is what they call it so what

34:56happens is these calciums that are

34:58flowing in cuz do you know they can

35:00actually flow in what is this little

35:02invagination trust me it's a word I

35:04know these positive ions these actual

35:07calcium can also flow in through this

35:10area too what is this little

35:11invagination here called that

35:12invagination is called a t tual so from

35:15these invaginations sodiums can flow

35:17into the cells and Trigger the calcium

35:18to be released here also from the actual

35:20T tubules reason why I'm telling you

35:22this is because these calcium mines when

35:24they're coming in they're going to go to

35:26this special area with inside the cell

35:28special organel this organel is called

35:30the sarop

35:32plasmic

35:35reticulum what happens is these calciums

35:38have these special special calcium

35:41sensitive channels okay so I'm going to

35:43zoom in on one of these calciums for a

35:45second calcium comes over here and binds

35:48onto a protein one of the proteins is

35:50called

35:51calmodulin now what happens is calcium

35:54and Cal modulin or just calcium can come

35:56over here and bind on to this receptor

35:59very sensitive receptor to calcium this

36:01receptor is called a

36:04ryanodine receptor type two so I'm just

36:07going to put R yr ryanodine receptor

36:10type two this ryanodine receptor type

36:13two which is very sensitive to calcium

36:14whenever there's increas in calcium

36:15levels this ryanodine receptor opens up

36:18a

36:19channel and when it opens up the channel

36:22guess what starts coming out calcium so

36:26now calcium is going to be really

36:28concentrated inside of the sarcoplasmic

36:30culum very very concentrated through

36:32different mechanisms but it's very very

36:34very concentrated guess what starts

36:36coming out of this area now the calciums

36:38so now a lot of calcium is going to get

36:40released out into this actual

36:43sarcoplasm so what happened just over

36:45they're clear calcium stimulate the

36:46Radine receptor type two it can either

36:48do it directly by itself or it can

36:50combine with calmodulin and bind onto

36:52the area which opens up the Radine

36:54receptor type two which is kind of like

36:55a mechanical receptor opens up this

36:58Channel and allows for calcium ions to

36:59come out in excessively large amounts so

37:02now calcium is going to start being very

37:04high within the cytoplasm what is that

37:06calcium going to do well calcium we're

37:08not going to spend a lot of time because

37:09we already have a video on how muscles

37:11contract if you guys haven't seen it go

37:12watch that okay we have a muscle

37:14contraction playlist right where we go

37:15over all this stuff so what happens is

37:18calcium binds onto a special protein

37:21this protein here is called

37:23troponin now this is the only one I want

37:25to spend a little bit of time on is

37:26actually consisting of of three

37:27components troponin i troponin t

37:29troponin c troponin c is where the

37:32calcium binds troponin T is where the

37:35tropomyosin is binding to the troponin

37:37and troponin I is where the troponin is

37:39bound to actin so quickly here it's

37:42bound to actin it's bound to

37:45tropomyosin or it's bound to calcium so

37:49calcium binds onto the troponin cite

37:52which changes the shape of the troponin

37:54it binds with it pulls on troponin t

37:57troponin T pulls on that tropomyosin

37:59protein this orange protein see this

38:01orange protein right here that's

38:03tropomyosin what is it doing it's

38:05impeding the interaction between this

38:08red guy to that green guy what is that

38:09red guy there called that red guy is

38:11called mein so this red this actual red

38:14guy here is called mein this green guy

38:17here is called

38:18actin what happens is calcium binds on

38:21jonin which changes the shape of the

38:24tropomyosin if it changes the shape of

38:26the tropomyosin what happens happens

38:27then let's actually show tropomyosin

38:29like this now so now tropomyosin is out

38:31of the way it's out of the way it's not

38:33impeding it anymore so same thing over

38:35here if calcium binds over here what's

38:37going to happen it's going to move the

38:38tropomyosin out of the

38:40way when tropomyosin is out of the way

38:43guess what can happen the mein head can

38:45interact with the

38:48actin so calcium coming to this area

38:53increases cross

38:56Bridges cross Bridges between the Act

38:59and the me if that's the case then

39:01you're going to have more what is this

39:03kind of representing here me kind of

39:05showing the lines coming in it's

39:06representing the contraction so more

39:08cross Bridges means more

39:12contraction and then that's going to

39:13help to be able to create that pump to

39:17squeeze the blood okay so increase in

39:19the crossbridge interaction increases

39:21the contraction which is going to cause

39:23the heart

39:24to

39:26pump

39:27action okay another

39:31thing because Gap Junctions are

39:33connecting cell to cell this is really

39:35really really really important that

39:37means that these cells are

39:38interconnected that means that these

39:40cells are basically synchronized that

39:42means that whenever these cells are

39:43receiving signals they're receiving it

39:45pretty much all at the same time very

39:46very quickly very very rapid and fast so

39:48these muscle cells that are Contracting

39:52again I could actually say that this is

39:53one muscle cell but at the same time if

39:55I were to come over here for just a

39:56second let's say that I had over here

39:58here's another muscle cell and the ions

40:00from this one are flowing to this one or

40:02they flow over here to this one all of

40:04these muscle cells are going to be

40:05getting depolarized around the same time

40:08so they synchronize their action to

40:10where they contract as a unit they call

40:11this a functional centium not even going

40:14to attempt to spell that okay you can

40:16try to look that up or something okay

40:17how to spell it but again the whole

40:19purpose is is I want you to understand

40:21is that these actual nodal cells are

40:23extending these Action potentials to All

40:25The myocardium through the these Gap

40:27Junctions so because of that they

40:29contract as a unit or they don't

40:31contract at all so this Contracting as a

40:32unit is actually the action of the

40:34functional

40:35centium holy crap that's a heck of a

40:37word right all right so that's that now

40:40so we've seen that action now let's get

40:43into how we actually get this cell to

40:45rest how do we get this cell to rest

40:48well we were at positive 40 molts

40:49because these voltage calcium channels

40:51these L Type calcium channels are open

40:53when we hit positive 40 they shut

40:56off when they shut off another Channel

40:59starts opening very very very powerfully

41:02this is actually going to be called a

41:04potassium Channel and this potassium

41:06Channel opens and potassium starts

41:08exiting the cell as you start losing ton

41:11and tons and tons of pottassium ions you

41:13lose positive ions what starts happening

41:15to the inside of the cell you start

41:16losing positive ions the cell's going to

41:18start becoming a little bit more

41:19negative and it's going to become

41:21negative and more negative and more

41:23negative and then what starts happening

41:24to the inside of the cell it's starting

41:26to

41:27repolarize so you're going to see this

41:31actual line going down on the graph

41:34you'll see it going down and it'll hit

41:36this point of resting membrane potential

41:39so now whenever the pottassium ions are

41:40coming out of the cell it's bringing the

41:42cell from positive 40 molts to around 60

41:45MTS around the resting membrane

41:46potential but again remember these noal

41:48cells don't really have a stable resting

41:50membrane potential once they get to

41:51about -60 the potassium channels close

41:54and those funny sodium channels start

41:56open opening so around 60 you might

41:58notice again these funny sodium channels

42:00opening and then the T type and then the

42:02L Type and then potassium repolarization

42:04okay so it's the same

42:06thing so because of that less cations

42:09are going to be coming into the cell so

42:10this cell is at its peak point now it's

42:12at that platto phase if this cell is at

42:15the plateau phase where the calcium ions

42:16are coming in and pottassium ions are

42:18going out it gets to a point where the

42:21calcium ion channels start closing so

42:25now what happens is

42:28these L typee calcium channels start

42:31closing as these L Type calcium channels

42:33start closing less calcium ions start

42:34coming in another thing we don't want

42:37our muscles to contract forever we got

42:39to get that calcium out of there because

42:40if calcium is there it's just going to

42:41keep binding toonin and keep moving the

42:43tropomyosin out of the way so that the

42:44cross Bridges can keep moving and

42:46creating power strokes and Contracting

42:47the muscle pumping the heart but

42:49eventually the heart's going to get weak

42:50if that happens all the time we have to

42:52give it time to rest so we got to get

42:54this calcium back into the sarcoplasmic

42:57reticulum and out into the extracellular

42:59environment to replenish the calcium

43:01levels in the outside of the cell and

43:03replenish the calcium levels inside of

43:04the sarcoplasmic reticulum how do we do

43:07that so once this happens there's going

43:10to be these special channels over you

43:11see these black channels here in the

43:13coplas reticulum these black channels on

43:16the sarcoplasmic reticulum are actually

43:18going to

43:19move some of this calcium back in so

43:23some of this calcium is going to get

43:24pumped right back into the sarcoplasmic

43:26culum but calcium is moving against his

43:29concentration gradient because you know

43:31calcium is actually going to be in lower

43:34concentration outside the cell and in

43:37high

43:38concentration inside of the coplas

43:40critic so I'm pumping it against so that

43:43means I have to utilize ATP and usually

43:46whenever you utilize the ATP in this

43:47process you're also pumping a proton out

43:50usually so there's usually going to be

43:51an antiporter likee system where you're

43:53pumping a proton out at the same time

43:55you're pumping calcium ions in and it's

43:57utilizing ATP that's get that's

43:59replenishing the calcium levels how else

44:01can we get calcium back in there another

44:04way that we can get calcium back in here

44:05is these

44:07calcium can actually come over to these

44:09other channels over you see these these

44:10actual red channels here these channels

44:13can actually pump some of the calcium

44:14back in also so get some of that calcium

44:18back in but again we have to have

44:20someone to help him because he's going

44:22against his concentration gradient so we

44:23found someone else and he was like Hey

44:25dude no worries I'll help you out I can

44:27move down my concentration gradient and

44:29his name is sodium and sodium moves down

44:33his concentration gradient out of the

44:34cop plasma culum into the cycop plasm

44:37and this is an example of secondary

44:39active transport so again we got calcium

44:42back into the SR through sodium calcium

44:44exchangers or through the calcium proton

44:46ATP ases cool how do we get it back out

44:49the same channels the exact same channel

44:52so now if I take over here this black

44:55channel it's the same thing thing I'm

44:57going to take some of the calcium and

44:59pump it out into the extracellular

45:01environment so this is the ECF the

45:03extracellular fluid this is the protons

45:05I'm going to pump it in I'm going to

45:07have to utilize ATP okay to do this

45:10process because it's primary active

45:11transport then for this one same thing

45:14I'm moving sodium down his concentration

45:18gradient and I'm moving the calcium

45:21against his concentration gradient onto

45:22the ECF that's replenishing the calcium

45:25levels back out here okay say trying to

45:27get your calcium levels out here

45:29replenished and the calcium levels in

45:30the SR

45:31replenished so now that's going to

45:33prevent the contraction so now once that

45:36happens these calcium channels shut off

45:38calcium gets sucked back into the SR

45:39pushed out into the extracellular

45:41environment potassium channels are the

45:42primary ones that are going to be

45:43functioning now functioning now so

45:47pottassium channels are going to even

45:49open up even more and they're going to

45:50start aggressively moving out even more

45:52so as the potassium channels start even

45:54aggressively moving out even more

45:57again you're going to start losing more

45:59and more and more positive ions with no

46:01counteracting of the calcium so what do

46:03you expect if calcium is not

46:05counteracting this anymore what's going

46:06to happen it's going to start dropping

46:09and it's going to drop and it's going to

46:10drop until it gets the resting membrane

46:11potential and then when it drops at the

46:13resting membrane

46:14potential it'll have this brief period

46:17in time where it'll actually kind of

46:19stay rested

46:23until ions from this cell let's say noal

46:27cell leak into this myocardial

46:29contractile cell again via the Gap

46:31Junctions and if that happens what

46:32happens it goes back up to threshold

46:35potential so to finish off phase two is

46:38the plateau phase so let's kind of like

46:40cut that off right there phase one is

46:42the drop down from the potassium

46:43channels phase two is the calcium and

46:45the potassium channels phase three is

46:47just the potassium channels and then we

46:49get into this last phase which is called

46:51phase 4 and phase four is where there's

46:54just no sodium no calcium ion movement

46:56and just potassium ions kind of leaking

46:58out very very slowly to keep it at the

47:01stable resting membrane potential until

47:03the sodium ions or other cats from The

47:05Gap Junctions leak into the cell again

47:07and triggered to go to

47:09threshold holy crap okay that's that

47:13now with that said we see exactly how

47:18this muscle is communicating that's the

47:21intrinsic ability all right Niners if

47:22you guys have stuck in there throughout

47:23this entire video here where we talk

47:25about electrophysiology and very great

47:27detail um I want to thank you guys

47:28enough we're going to I can't thank you

47:29guys enough but we're going to go into

47:30part two so we talked about the

47:31intrinsic ability of the heart what I

47:33want to do now is I want to get into a

47:34little bit more of the detail of the

47:35extrinsic interation of the heart how

47:36that can actually uh bring the actual

47:39Baseline of the intrinsic ability of the

47:40heart above the actual like you know

47:44basically increase in the heart rate or

47:45how we can bring it below that actual

47:47basil rate which is going to be decrease

47:49in the heart rate which is called

47:50bradicardia increase in the heart rate

47:51Tac cardia so we'll talk about how the

47:53sympathetic and parasympathetic nervous

47:55system affects this activity so I hope

47:57to see you guys in part two all right

47:58see you soon n nerds

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