Lecture #2 - Action Potentials, Synaptic Transmission and EC Coupling Flashcards
Use of Ion Chanels
- Signlaing Devices
- Move ions across epithelia
- Move ions in chemiostatsic circuts
- Maintain Ion homeostasis
There are more ion channels in multi cellular organisms because they are important in communication across long distances
Ion Chanels (Overall) - Why ion channels act as signaling devices
Ion channels open/close very fast (miliseconds)
Ion chanel opens –> chanel conducts millions of ions down electrochemical gradient –> ions moving causes a rapid and large change in membrane potential (change in charge difference) across membrane and change in ion concetration–> Change in membrane potential/ion concetration activates protein –> protein triggers downstream events
- Conductance = 10^6 ions per second (moves millions of ions/second)
NOTE - Voltage difference/charge difference/membrane potential = ALL same thing
Downstream events that are caused by changes in membrane potential/ion flow (change in membrane potential can trigger)
- Action Potential
- Muscle contraction
- Secretion
Ion chancels can signal for a cell to have an action potential or contract muscle or release vesicle
Types of signaling events mediated by ion Channels
Ion Chanels can allow for:
1. Chemical signals to be converted to electrical signals (Example – Nuerotransmission at a synpase
2. Electrical signals to stimulate more electrical signals (Example – Action potentials moving a nerve)
- Propagation = electrical signals give rise to more electrical signals
3. Electrical signals to be converted to chemical signals (Example – Electrical signal at the end of nerve/ nerve going to muscle gives rise to chemical signals to causing excitation-contraction and excitation secretion coupling)
4. Spontaneous electrical signals (Example – Pacemaker activity in heart activating heart to beat using ion channels)
Techniques used to measure ion channel activity
- Intracelular microelectrode
- Voltage Clamps
- Patch Clamp
Intracellular Microelectrode
Use - measures voltage across the membrane (measures membrane potential)
Micro-electrode uses a glass capillary pipette (pipette opening is very small ; pipette is filled with solution of conducting AgCl)
Process – insert the capillary pipette into a cell
- Property of the glass and the membrane being hydrophobic causes the glass pipette to form a tight seal (has high resistence) at the edges when it is inserted into the cell
- Because of the seal –> any movement of charge is through the electrode into the cell
Measuring membrane potential using a Intracellular electrode
Experiment – Have bath that contains a excitable cell –> Intracellular electrode is inserted into the cell –> electrode measures the charge difference between the inside of the cell and the bath that the cell is in
- Need a reference electrode sitting n the bath to use the charge of the bath as a reference
Start the Volatge (V) is 0 –> electrode enters the cell and volatge decreases to -60mV - -90mv (cell is polarized) –> remove the electrode and the volatge goes back to 0
- Start V=0 –> because both the electrodes are in the bath
- Volatge of -60mV –> means the inside of the cell is more negative (Negative membrane potential)
Polarized Vs. Depolarized Vs. Hyperpolarized
Polarized – inside if the cell is more negative compared to the outside (negative membrane potential) (Ex. -60mV inside cell)
Depolarized – Inside of the cell becomes less negative (Ex. Membrane potential goes from –60mV to 0mV)
HyperPolarized – Inside of cell/membrane potential becomes more negative
REMINDER - negative inside cell = negative membrane potential
What does it mean for a cell to be excitable
ALL cells have membrane potential across the membrane BUT NOT all cells are excitable (nerve and muscle = excitable)
Excitable means the cell is able to become depolarized AND can fire an action potential (Non-excitable cell does not fire AP no matter how depolarized it gets
When cells are depilarized a little the pumps and transporters bring the cell back to resting potential BUT if depolarization crosses a certain threshold in excitable cells then cell fires an AP)
Voltage during Action potential
Cell fires an action potential –> the membrane potential goes from negative to 0 (depolarizes)–> membrane potential cross beyond 0 (becomes positive ; ‘overhoot’) –> membrane potential will return to a negative value (membrane is polarized again) and membrane potential goes below the resting potential (hyperpolarized) –> drifts back to resting potential
Hogdkin and Huxley
Insert a micro-electrode into the squid axon –> measured the measuring membrane potential) –> Saw a huge and quick waveform
NOW we know this wave form was the action potential
Current
Current = rate of charge movement over time
Characteristics of Action potential
- Steroyticpical size and shape —> AP always looks the same (Same size/shape) for any axon/exitable cell even if the same cell fires many times
- When an AP is fired the mmebrane enters a refractory period –> Once AP fires/membrane is in refractory period membrane can’t fire a second action potential (can’t get 2 additive APs to get larger AP)
- Means action potential is always a defined thing
- If a cell is depolarized there is an all or none response (fire AP or nothing)
- Propagation –> AP move down the length of the axon
- IF you depolarize cell at one point in the axon –> THEN measure the membrane potential farther down the axon the AP propegates (AP fires in one place then fires nearby)
- AP waveform is unchanged during propgation (AP does not fizzle out as it goes down the axon)
- IF you depolarize cell at one point in the axon –> THEN measure the membrane potential farther down the axon the AP propegates (AP fires in one place then fires nearby)
Issue with looking at membrane potnetial/mechanism during action potential
Issue - Hard to find what is happening because at every point on the Action potential wave form there are many things happening/changing (many ions moving in and out/many currents)
Solution – Clamp/fix the voltage at any given point (study the cell when it is at a specific voltage)
- Example - Fix/clamp the voltage at resting potentials and see what the currents across the membrane –> THEN change and clamp at new voltage and see the currents going in/out of cell at the new voltage
Chart (Time Vs. Membrane potential) ; Yellow line = Action potential wave form ; Purple – current of Na Chanels ; Red = curent of K chanels
Voltage Clamp
Overall – Keep the membrane potential constant (clamped ; fix membrane at a voltage) and measure the the currents flowing across the membrane at a given membrane potential
Process – As a current goes across the membrane and the voltage changes a second electrode connected to the feedback amplifier (FBA) injects or removes charges to compensate for the change in voltage due to ion channels and keep a constant voltage in the cell (keep constant membrane potential)
Voltage clamp of squid Axon Experiment - Results
Top chart – start at -65mV then clamp at -9mV to give a 56mV depolarization (enough to get AP)
- Square trace = indicates the membrane potential
Chart – measuring current (Im = mA/cm)
- Line A (Total Current ; Have Na gradient) –> + charge (Na+) goes into cell (Negative Current ; Na gradient is the driving force) ; AT end have a positive curent
- Line B - No Na gradient –> no driving force –> No Na Current ; STILL have positive current (has to be caused by something other than Na)
Voltage clamp of squid Axon Experiment - Results Line A - Line B
Line C - Line A – Line B –> shows the curent caused by the Na Ions
- Negtaive current at the start of AP = Na going into the cell BUT then Na stops (because Line C Na current goes to 0)
NOTE - know the time of current in the AP based on top trace
Na and K current
Na is causing the negative current at the start of line A (based on line C) and K causes the K current at the end of line A/B ( based on line B)
- Positive current in line A/B is K leaving cell (know K because Na current never goes to positive in Line C –> + value in lineA/B has to come from a different ion)
Line B - shows the K chanels slowly activate at the start –> THE K channels stay open for as long as the membrane is depolarized (stay open until the membrane potential goes back to –65mV in the AP trace at top)
Positive and negative current
Positive going into the cell = negative current
Positive charge going out of cell = positive current
Patch Clamp
Use - Isolate and describe properties of one channel (look at 1 channel)
Process – apply the micro electrode into a patch of the cell and apply gentle suction –> Pull away so the patch of membrane tears off –> membrane will stick tightly to the electrode and make a seal around the microelectrode pipette because the membrane is hydrophobic
- End – isolate a small patch of the membrane where the is only 1 or a few chanels –> NOW can put patch in bath –> measure the current across one/few ion chanels in the patch of membrane
There are many configurations of patch clamp - Whole cell gives Outside-out or On-Cell gives In-side out
Patch recoridng of an ion channel
Start – Ionic current = 0 –> current becomes negative (dips) –> current stays at 0 for a while –> channels open and the current becomes negative
- When the current becomes negative –> channel opens and closes Vs. current stays at 0 the chanels are closed
Patch recording shows the ion channel has stochastic properties
Stochastic properties of proteins
Single ion chanel has stochastic properties –> when looking at a single chanel don’t know when it will open/close
SAME applies for ALL enzymes (are stochastic)
- If watch a single enzyme you can’t know at which point the bond would break or product is release because it is random)
Stochastic properties of ion chanels:
1. Gating is independent and is described by a proability function
2. An ion chanel has only 2 states (ion channels is either open or closed)
- Ion chanel opens and ions move through –> then the chanel closes and the current (charges moving) stop
- Open Vs. Closed states = because the protein is moving from one state to another
3. Conductance is finate
Stochastic properties of ion chanels - Gating is independent and is described by a proability function
Opening and closing (gating) of a channel is a independent property and is based on a probability function
- Don’t know when the channel opens/closes just know the probabiility that a chanel open (proability stays the same)
- Chanel open/close once is independent of the same chanel open/closing again AND each of those events there is an equal probaility that the chanel open/closes
- Chanel can bind to a ligand/be phosphorylated to increase the probabiliy of opening
Stochastic properties of ion chanels - Conductance is finate
Conductance (dip in chart) is a property of the chanel
- Each chanel has its own conduacted (never changes for the chanel)
Conductance is finite –> goes to the same value of negative current for each dip
Low conductance = smaller dip (less change in membrane potential)
Big conductance = bigger dip (Bigger opening = more ions go through = bigger change in current = bigger dip)