1 / 17

LECTURE 3: ION CHANNELS & THE RESTING MEMBRANE POTENTIAL

LECTURE 3: ION CHANNELS & THE RESTING MEMBRANE POTENTIAL. REQUIRED READING: Kandel text, Chapters 7, pgs 105-139. + + + + + + + + + + + + + + + + + + + + + + + + + + + + +. V m = V in - V out. - - - - - - - - - - - - - - - - - - - - - - - - - -. In resting neuron:.

harlan-paul
Download Presentation

LECTURE 3: ION CHANNELS & THE RESTING MEMBRANE POTENTIAL

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. LECTURE 3: ION CHANNELS & THE RESTING MEMBRANE POTENTIAL REQUIRED READING: Kandel text, Chapters 7, pgs 105-139 + + + + + + + + + + + + + + + + + + + + + + + + + + + + + Vm = Vin - Vout - - - - - - - - - - - - - - - - - - - - - - - - - - In resting neuron: Vm ~ - 60 to - 75 mV - - - - - - - - - - - - - - - - - - - - - - - - - - + + + + + + + + + + + + + + + + + + + + + + + + + + + + + Membrane potential is a BATTERY providing power to drive currents when the cell is activated This lecture discusses how membrane potential is established and maintained

  2. MEASURING THE RESTING MEMBRANE POTENTIAL: MICROPIPET FILLED WITH HIGH SALT For this method, recording pipet has a very fine tip and is filled with a high salt solution (e.g. 3M KCl), so that pipet has very low resistance. In this way, the voltage measured by amplifier accurately reflects the voltage across the cell membrane. (method not useful in very small cells due to pipet salt poisoning of cells) Rpipet Rm(actual) Vpipet Vm(actual) Vm(measured) = Vm(actual) + Vpipet when Rpipet <<< Rm(actual) Vm(measured) = Vm(actual)

  3. MEASURING THE RESTING MEMBRANE POTENTIAL: PATCH PIPET IN “WHOLE-CELL” CONFIGURATION Patch pipet filled with cytoplasm-like solution is touched to cell membrane; with negative pressure, the pipet makes a very tight “cell-attached” or “on-cell” seal onto membrane (leak resistance > 10 GW) Applying gentle suction can break the membrane inside the pipet, making pipet fluid contiguous with the cytoplasm. This is the “whole-cell” configuration. When break is made into cell, the pipet can record the membrane potential

  4. TWO TYPES OF PROTEIN COMPLEXES CONTRIBUTE TO ESTABLISHING THE RESTING MEMBRANE POTENTIAL ION PUMP -- drives a specific ion or group of ions from one side of the plasma membrane to the other side Pumps drive ions ONE-WAY and use energy from ATP hydrolysis to make the process energetically favorable ION CHANNEL -- protein complex containing a small pore which allows a specific ion or group of ions to pass Flow of ions through channels is PASSIVE and is driven by the prevailing chemical and electrical gradients A channel is an ion-specific resistor with a certain conductance ( g ) For most channels, the conductance is the same for ions flowing IN or OUT Other channels allow ions to pass with greater conductance in one direction; these are called RECTIFYING CHANNELS e.g., a channel with greater conductance of inward current is called an inwardly rectifying channel

  5. 2 K+ outside inside 3 Na+ ATP ADP + Pi Na/K ATPase PUMP Na+/K+ ATPase USES ENERGY FROM ATP HYDROLYSIS TO PUMP SODIUM IONS OUT OF CELL & POTASSIUM IONS INTO CELL AT A 3 Na+ : 2 K+ RATIO CONSEQUENCES OF PUMP ACTIVITY [ K+ ]in>> [ K+ ]out [ Na+ ]in << [ Na+ ]out Net positive charge pumped out of cell causes a matching amount of permeable chloride anions to move out passively through channels [ Cl- ]in <<[ Cl- ]out

  6. IONS CHANNELS K+ outside Na+ POTASSIUM CHANNEL (non-gated, “leak”) inside Some types of ion channels are “gated”, meaning the ion-selective pore can be either open or shut (not in-between) Such channels can be gated by ligands, phosphorylation, or voltage Other types of ion channels are open all the time These channels referred to as “leak” channels

  7. Cl- Na+ Cl- Na+ K+ K+ + - + - + + + + out out in + - + - in - - - - K+ K+ A- A- Cl- Na+ Cl- Na+ POTASSIUM CHANNELS FAVOR A NEGATIVE MEMBRANE POTENTIAL Potassium channels are the most abundant leak channels in neurons. Because the Na/K pump makes [K+]in>> [K+]out , potassium ions move outwards through channels due to the chemical driving potential, EK . (EK can be thought of as a potassium “battery”) Net outward ion flow continues until opposed by a membrane potential, Vm , of equal force built up in the membrane capacitor. AT EQUILIBRIUM When Vm = EK, zero net K+ flux When Vm = 0, large K+ efflux

  8. Cl- Na+ Cl- Na+ K+ K+ + - + - + + + + out out in + - + - in - - - - K+ K+ A- A- Cl- Na+ Cl- Na+ CIRCUIT REPRESENTATION OF POTASSIUM CONDUCTANCE, POTASSIUM BATTERY, AND MEMBRANE CAPACITANCE When Vm = 0, large K+ efflux When Vm = EK, zero net K+ flux gK gK IK IK = 0 + + + _ _ _ CM VM = 0 CM VM = EK + + EK EK - - What is the strength of the potassium battery EK ???

  9. [X]out 58 mV log EX = z [X]in THE NERNST EQUATION The cytoplasmic and extracellular concentrations of an ion determine the chemical driving force for that ion and the equilibrium membrane potential if this is the ONLY ion that is permeable through the membrane Nernst Equation Where EX is the chemical potential and z is the charge of ion X z = +1 [K+]in = 130 mM [K+]out = 5 mM For potassium: 5 58 mV log EK+ = = - 82 mV 1 130

  10. Cl- Na+ Cl- Na+ K+ K+ IK + - + - + + + + out out + - + - in - - - - in IK = 2 pA slope = gK = 25 pS K+ K+ A- A- Cl- Na+ Cl- Na+ Vm EK = - 82 mV out out gK = 25 pS IK = 0 IK = 2 pA gK = 25 pS + + EK = - 82 mV EK = - 82 mV - - in in VOLTAGE-CURRENT RELATION OF THE POTASSIUM BATTERY When Vm = 0, large K+ efflux IK = 2 pA When Vm = EK, zero net K+ flux IK = 0 pA Conductivity of single K channel gK = 25 pS Total K conductivity (gK ) gK = gKXNK where NKis # K channels IK= gKx( Vm - EK ) Vm= EK+IK RK

  11. Cl- Na+ K+ + - + - out + - + - in K+ A- Cl- Na+ gK and Cm DETERMINE HOW FAST Vm CHANGES TO EK Vm (mV) channels open 0 - 82 T t T ~Cm/ gK The greater the value of gK , the greater the potassium current ( IK ) and the faster the transition to the potassium Nernst potential ( EK) The greater the value of Cm , the longer the potassium current ( IK ) and the slower the transition to the potassium Nernst potential ( EK)

  12. RESTING POTENTIAL SET BY RELATIVE PERMEABILITIES OF K+, Na+, & Cl- IONS Nernst Potential Relative Permeability (P) EK = - 82.1 mV 1.0 ENa = + 84.8 mV 0.05 ECl = - 63.6 mV 0.2 Resting membrane potential reflects the relative permeabilities of each ion and the Nernst potential of each ion gKEK + gNaENa + gClECl PKEK + PNaENa + PClECl ~ Vm = = gK+ gNa + gCl PK + PNa + PCl When the resting membrane potential is achieved, there is ongoing influx of sodium and a matching efflux of potassium. Na/K ATPase is continually needed to keep the ion gradients from running down over time

  13. [X]out 58 mV log EX = z [X]in ) ( PK[K+]o + PNa[Na+]o + PCl[Cl-]i PKEK + PNaENa + PClECl Vm = 58 mV log10 PK[K+]i + PNa[Na+]i + PCl[Cl-]o Vm = PK + PNa + PCl THE GOLDMAN EQUATION from before Nernst equatiion Goldman equation The greater an ion’s concentration and permeability, the more it contributes to the resting membrane potential When one ion is by far the most permeable, Goldman eq. reduces to Nernst eq.

  14. PKEK + PNaENa + PClECl Vm = PK + PNa + PCl RELATIVE PERMEABILITY & THE RESTING POTENTIAL [K+]o = 5 mM [Na+]o = 145 mM [Cl-]o = 100 mM [K+]i = 130 mM [Na+]i = 5 mM [Cl-]i = 8 mM EK = - 82.1 mV ENa = 84.8 mV ECl = - 63.6 mV PK = 1 PNa = 0.05 PCl = 0.2 Vm = - 72.4 mV

  15. K+ K+ K+ K+ K+ K+ AT STEADY STATE: Na+ IK + INa+ ICl= 0 out out gNa = 0.1 nS INa = - 15.7 pA RNa = 10 GW Na+ IK = 19.4 pA gK = 2 nS - - RK = 0.5 GW ENa = + 84.8 mV + + + EK = - 82.1 mV - in GRAPHIC AND CIRCUIT REPRESENTATIONS OF ION FLOWS ACROSS THE MEMBRANE AT THE RESTING POTENTIAL Cl- + + + + + + + + + + + + + + + + + + out Vm = - 72.4 mV - - - - - - - - - - - - - - - - - - in Cl- ENa = + 84.8 mV EK = - 82.1 mV out gCl = 0.4 nS out + + + RCl = 2.5 GW Vm = ICl = -3.5 pA - - - in -72.4 mV ECl = - 63.6 mV in EK + IKRK= Vm = ENa + INaRNa = ECl + IClRCl -82.1 mV + (19.4 pA)(0.5 GW) = -72.4 mV = +84.8 mV + (-15.7 pA)(10 GW) = -63.6 mV + (-3.5 pA)(2.5 GW)

  16. Nernst Potential Prest Paction-potential EK = -82 mV 1.0 1.0 ENa = +85 mV 0.05 5.0 ECl = -64 mV 0.2 0.2 INCREASING SODIUM PERMEABILITY UNDERLIES SODIUM INFLUX AND MEMBRANE DEPOLARIZATION DURING ACTION POTENTIAL During action potential, the number of open sodium channels increases dramatically Rest During Action Potential - 70 mV + 36 mV GOLDMAN EQUATION-PREDICTED Vm When sodium channels open, sodium ions flow in rapidly because of the negative membrane potential and the strong inward sodium battery Inward sodium current depolarizes membrane and moves it towards the positive potential predicted by Goldman’s equation (this positive potential is never fully achieved due to additional channel dynamics)

  17. Next Lecture: MEASURING MEMBRANE CONDUCTANCE AND CAPACITANCE & VOLTAGE-CLAMP RECORDING REQUIRED READING: Kandel text, Chapters 8, 9 (beginning), pgs 140-153

More Related