lectures 1,2,3 rachel a. kaplan and elbert heng 2.3.14

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Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

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Page 1: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Lectures 1,2,3Rachel A. Kaplan and Elbert Heng

2.3.14

Page 2: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Announcements

• Detailed Answers for PS1 are on wiki

• Contacting TAso please use piazza, you’ll get the fastest

responseo if you don’t want to, email (not canvas

message) uso if you’re emailing Rachel

her email is [email protected]• or [email protected], either one is fine

• Tell us what you want us to cover! That’s what we’re here for!

Page 3: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Lecture 1: Intro to Electrophysiology

Page 4: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Background

● Neuron Doctrine● Cajal vs. Golgi● Graded vs. Discrete Signals● Lipid bilayer - hydrophobic; need ion channels● Properties of ion channels● Definitions: ions, voltage, membrane potential,

current, depolarization, hyperpolarization

Page 5: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Studying Ion Channels

● Driving force● Current vs. Voltage clamp● Hodgkin & Huxley: squid giant axon● Neher & Sakman: patch clamp

○ inside out patch○ outside out patch

Page 6: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

aka On Cell

Cell Attached

Page 7: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Whole Cell

Page 8: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Inside-Out

Page 9: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Outside-Out

Page 10: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Lecture 2: Ion Channel Function

Page 11: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Current Clamp

Page 12: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Voltage Clamp

Page 13: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Single Channel i/V plots

• Shows relationship between (direction and amount of) current (i) flowing through a channel given various membrane potentials (that you have clamped the membrane at to experimentally determine current)• If it’s OHMIC, it’s just a linear relationship

• not so scary, you learned this in middle school!

Page 14: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Drawing i/V Curves

• If a channel is ohmic, relationship between i and V is defined by Ohm’s law

• i = g V• In voltage clamp, we are manipulating the

independent variable: V• And we are measuring the dependent

variable: i• g is the slope

Page 15: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Drawing i/V Curves

If you want to draw a linear curve, what do you need?

Page 16: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Drawing i/V Curves

• That’s right, a slope and a point.• We can find a slope and a point • Slope: conductance• Point: where the curve crosses the x-axis (the

potential axis) – Eion or Vrev

• (these two are the same for channels that pass only one type of ion)

Page 17: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Drawing i/V Curves

• How do I find conductance?• Don’t worry about it, it will be given to you.

• How do I calculate the Eion?• Nernst Equation, duh

Page 18: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14
Page 19: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

What’s all this talk about driving force?

• Driving force = (Vm-Eion)• This is the potential difference that will

actually be doing the work of moving the current through the channel. • This allows you to use your i/V plot,

evaluate the relationship given a certain membrane potential, see how much current is flowing.

• Essentially normalizes the curve so that it’s like Eion was at the origin. • i = (Vm-Eion)g

Page 20: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14
Page 21: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Questions about this part of the homework?

Page 22: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Macroscopic currents

(Elbert)

Page 23: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Channel Gating on Macroscopic Currents

(Elbert)

Page 24: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Lecture 3: Ion Channel Structure

Page 25: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Basics

• Ion channels are proteins• Can be made of more than one protein (more

than one subunit)

• Ion channels do things• Need special machinery to do things –

domains• If the university was an ion channel, what

would be an example of a subunit and a domain?

Page 26: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

What do ion channels need to do?

• Pass ions from the outside (extracellular space) to the inside (intracellular)• Why can’t ions pass by themselves?• Thus, ion channels need to be able to

associate water and lipids• They do because of their amino acid

sequence.

Page 27: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

How do we deduce the structure?

• Hydrophobicity Plot – shows regions of the aa sequence that likely are in the membrane, so they likely are the membrane spanning regions.

• Glycosylation – will be on the extracellular part of the protein.

• Immunostaining – will show you if a terminus (the end of the protein) is intra or extracellular• FROM ALL OF THIS DATA, YOU CAN DRAW A

PUTATIVE STRUCTURE.

Page 28: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14
Page 29: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Other ways you can deduce structure:

• Imaging – really hard, but super cool! EM

• X-Ray Crystallography – also really hard, but that’s how Rod MacKinnon figured out what the Drosophilia Shaker K+ Channel looks like.

Page 30: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Function of ion channels

• Expression systems allow you to selectively express one channel and then measure the properties of that one type of channel. • Frog egg = your canvas• cDNA = your paint, with which you express

your feelings channels

Page 31: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Selectivity of Channels

Most Selective Less Selective Least Selective

VG Ligand Gated Gap Junctions

Calcium Activated K+ Channels

Non-specific cation/anion channels

Cyclic Nucleotide

Page 32: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Determination of Selectivity

• S5-S6 Region – Pore Forming Region• Residues here form an environment

for the ion that is as energetically favorable (comfortable) as it’s sphere of hydration (the water molecules that normally surround an ion)

Page 33: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Gating

• S4 is the voltage sensor• Like charges repel, so this is how it

moves!• The S4 alpha helix has a lot of positively

charged residues• So when the membrane becomes

depolarized enough (there is enough + charge on the intracellular side) it is repelled from that positive charge and moves up/out of the way

Page 34: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Inactivation

• This is the ball and chain model – ball will plug up channel and not let it pass more ions, and then eventually fall out so the channel can close (and then open again)• Remember, this is why we have the absolute

refractory period!

Page 35: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Modulation

• Modulation: changes the open probability of the channel• You are all experts at macroscopic I/V plots,

so you can reason how a modulator would affect the plot.

• MODULATORS:

Page 36: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

Modulation

• Modulation: changes the open probability of the channel• You are all experts at macroscopic I/V plots,

so you can reason how a modulator would affect the plot.

• MODULATORS:• Other subunits of the protein (beta

subunits)• Second messengers• Changes in gene expression• Phosphorylation• Allosteric regulators

Page 37: Lectures 1,2,3 Rachel A. Kaplan and Elbert Heng 2.3.14

HAVE A GREAT WEEK!

Questions?