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Lecture notes • Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian, Ning. (1995) Essentials of neural Science and Behavior. Study guide and practice problems . Appleton & Lange Davson, H. (1970) A Textbook of General Physiology, 4 th Ed., Williams and Wilkins Hille, B. (1992) Ionic Channels of Excitable Membranes, 2ed., Sinauer. Levitan, I. B. & Kaczmarek, L. K. (1991) The Neuron: Cell and Molecular biology, Oxford. Mathews, G. G. (1998) Cellular Physiology of Nerve and Muscle, Blackwell Science

Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

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Page 1: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Lecture notes

• Taken in part from:• Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed.• Calabrese, R. C., Gordon, J., Hawkins, R., & Qian, Ning. (1995) Essentials of neural Science and Behavior.

Study guide and practice problems. Appleton & Lange• Davson, H. (1970) A Textbook of General Physiology, 4th Ed., Williams and Wilkins • Hille, B. (1992) Ionic Channels of Excitable Membranes, 2ed., Sinauer.• Levitan, I. B. & Kaczmarek, L. K. (1991) The Neuron: Cell and Molecular biology, Oxford.• Mathews, G. G. (1998) Cellular Physiology of Nerve and Muscle, Blackwell Science

Page 2: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

CELLMEMBRANE

• 1) KEEPS THE CELL INTACKT (IN PART)

• 2) PERMEABLE TO SMALL MOLECULES

• 3) IMPERMEABLE TO LARGE MOLECULES.

Page 3: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

DIFFUSION

PHYSICAL PROCESS THAT EQUILIBRATES FREELY MOVING SUBSTANCES

Page 4: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

CELLULAR COMPARTMENTS

• INTRACELLULAR SPACE – The fluid space surrounded by the plasma membrane or cell wall.

• EXTRACELLULAR SPACE – The fluid space surrounding the outside of a plasma membrane of a cell or cell wall.

Page 5: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

COMPOSITIONS OF PARTICLAS WITHIN AND OUTSIDE PLASMA

MEBRANES

Page 6: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

PLASMA MEMBRANE

Page 7: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

FREEZE FRACTURE TECHNIQUE

Page 8: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,
Page 9: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

FRACTURE IS NOT ALONG CRYSTAL PLANES

Page 10: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,
Page 11: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

OSMOLARITY

• CONCENTRATION OF WATER IN SOLUTIONS CONTAINING DIFFERENT DISSOLVED SUBSTANCES.

Page 12: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Osmolarity (cont.)

• THE HIGHER THE OSMOLARITY OF A SOLUTION THE LOWER THE CONCENTRATION OF WATER IN THAT SOLUTION.

Page 13: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

MOLARITY

• THE MOLECULAR WEIGHT, IN GRAMS, OF A SUBSTANCE DISOLVED IN 1 LITER OF SOLUTION. (1 M)

Page 14: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Molarity (cont.)

• 1 MOLE OF DISOLVED PARTICLES PER LITER IS SAID TO HAVE 1 OSMAL

Page 15: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

MOLALITY

• MOLES OF SOLUTION PER KILOGRAM OF SOLVENT

• Takes into account that large dissolved molecules (protein of high molecular weight) displace a greater volume of water than small molecules

Page 16: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Example• Glucose, sucrose do not greatly dissolve

in water. Number of water molecules does not change.

Page 17: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Osmolarity

• Osmolarity takes into account how many dissolved particles result from each molecule of the dissolved substance.

• 0.1 M glucose solution is 0.1 Osm solution.

Page 18: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

• Glucose, sucrose and urea molecules do not dissociate when dissolved in water.

• 0.1M glucose is a 0.1 Osm solution

Page 19: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Osmolarity for dissociated substances

0.1 M NaCl = 0.1 M Na + 0.1M Cl = 0.2 Osm

Page 20: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

300 Osm

• 300 mM glucose

• 150 mM NaCl

• 100 mM NaCl + 100 mM Sucrose

• 75 mM NaCl + 75 mM KCl

Page 21: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Mixing

• The mixing is caused by the random independent motion of individual molecules (temperature dependent).

Page 22: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Two separate actions

• Random movement of the solute (glucose)

• Random movement of the solvent (water).

Page 23: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Osmosis

• WHEN SOLUTIONS OF DIFFERENT OSMOLARITY ARE PLACED IN CONTACT WITH A BARRIER THROUGH WHICH WATER WILL MOVE ACROSS THE BARRIER, WATER WILL MOVE FROM THAT SIDE WITH THE GREATER NUMBER OF WATER MOLECULES PER UNIT VOLUME (Higher Osmolarity) TO THAT SIDE WITH THE LESSER WATER MOLECULES PER UNIT VOLUME (Lower Osmolarity).

Page 24: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Home experiment

• Mason or Kerr quart jar.

• Dark Molasses

• Large Carrot

• Glass Tube

Page 25: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Observable change

• Mechanism is the same mechanism as diffusion, but observable with water for its causes observable changes in the volume of liquid of chamber into which the water moves.

Page 26: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Work done by osmosis moves piston from left to right

compartment

Page 27: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Osmotic Pressure

• Suppose that one could measure the force necessary to just keep the water from moving into compartment A.

• That force devided by the cross sectional area of the piston would be the osmotic pressure of the system.

Page 28: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Aquapores

• Pores have now been found that transfer only water and not ions.

Page 29: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

OSMOTIC CHANGE IN VOL.

Page 30: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,
Page 31: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

OSMOTIC BALALANCE VS CELL VOLUME

• [S]in = [S]out

• [S]in + [P]in = [S]out

Page 32: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

NO NET CHANGE WHEN IN BALANCE

• IF A SUBSTANCE IS AT DIFFUSION EQUILIBRIUM ACROSS THE CELL MEMBARANE, THERE IS NO NET MOVEMENT OF THAT SUBSTANCE ACROSS THAT MEMBRANE.

Page 33: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Osm vs. cell volume (cont.)

• REQUIRES THAT:

• [S]in = [S]out

• and

• [S]in + [P]in = [S]out

• BE SIMULATENEOUSLY TRUE AT EQUILIBRIUM.

Page 34: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

• How do cells in nature solve the simultaneous condition?

Page 35: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Solution 1

• MAKE THE CELL IMPERMEANT TO WATER

• Certain epithelial cells (skin) are impermanent to water

Page 36: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Solution 2

• PUT THE CONTENTS OF THE CELL WITHIN AN INELASTIC WALL

• Plant cell’s solution

Page 37: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Solution 3

• MAKE THE CELL MEMBRANE IMPERMEANT TO SELECTED EXTRACELLULAR SOLUTES

Page 38: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Impermeant sucrose & protein

Page 39: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

ECF Osm. Lower than ICF

Page 40: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

ECF has permeant solute, ECF & ICF initially equal

Page 41: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

ECF contains a mixture of permeant and impermeant solutes

Page 42: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

• [UREA]in + [P]in = [UREA]out +

[SUCROSE]out

Page 43: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

IONS IN SOLUTION (WATER)

• Ions in solution behave much like particles in solution.

Page 44: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Na+, K+, Cl-, Ca2+

• When they move they carry their charge with them.

Page 45: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

• Some channels are non selective as to the type of cation.

Page 46: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

• The movement of ions down their gradient can do work.

Page 47: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Size of ion depends on it ability to hold a water “cloud”

Page 48: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Most channels only allow one species of ion to pass

Page 49: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Na+ channel. Water cloud must be stripped away

Page 50: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,
Page 51: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Current through channels follows Ohm’s law

Page 52: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,
Page 53: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

CATION & ANIONS

• Positively charged particles in solution tend to congregate near the negative pole of a battery.

• Negatively charged particles tend to congregate near the positive poles.

Page 54: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

DIFFUSION POTENTIAL

• DIFFERENTIAL DISTRIBUTION OF IONS IN SOLUTION BETWEEN TWO DIFFERENT COMAPARTMENTS, WITH A COMUNICATING CHANNEL, GIVE RISE TO A VOLTAGE GRADIANT IN THE SOLUTION.

Page 55: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Concentration Cell• Different concentration of electrolyte XY in

solution.

• Membrane permeable to only X+

Page 56: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Diffusion

• Concentration in 1 is greater than 2 by twice as much

Page 57: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Diffusion

• If the barrier is moved, twice as many X+ moves down its gradient from compartment 1 to compartment 2, carrying a positive charge.

Page 58: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Charge separation

• Movement of charges from 1 to 2 sets up a potential difference between the two compartments.

• This charge separation is in the direction of 2 to 1, opposite to the diffusion gradient.

Page 59: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

• As the potential difference grows it will become increasing harder to move X+ from 1 to 2.

• More and more X+ will move from 2 to 1

Page 60: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Equilibrium Potential

• An equilibrium position is reached at which the electrical (tending to move X+ from 2 to 1) just balances the chemical or concentration gradient (tending to move X+ from 1 to 2).

Page 61: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Voltage

1) The potential difference that builds up in the above system is expressed as voltage (in mVolts).

Page 62: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Voltage (cont.)

Voltage should be thought of as a gradient. A gradient implies looking at two places or states with respect to one another.

Page 63: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Electrical conventions 1

If Compartment 1 is the reference chamber, Compartment 2 is said to be positive with respect to compartment 1. (A volt meter will point toward the positive pole).

Page 64: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Electrical conventions 2

• If the compartment 2 is the reference chamber, compartment 2 is negative with respect to compartment 1. (The voltmeter will point to the left chamber).

Page 65: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Voltage (cont.)

2) This can be thought of as an electromotive force.

Page 66: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Voltage (cont.)

3) Think of this voltage as a driving force for the movement of charges in space.

Page 67: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Equilibrium Potential

• A potential can be calculated for each species of ions which represents the balance between the electromotive force (separation of charge) and diffusion (differential concentration gradient) for a given species of ion across a selectively permeable membrane.

Page 68: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Temperature effect

• There is a temperature coefficient that is implied in the Nernst equation. Increasing the temperature increases the random motion of the molecules in solution. This increase will increase the probability of a given ion to go through the channel.

Page 69: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Nernst Equation

• If one wants to know the dynamic value of the diffusion flow one would have to do work to stop the flow.

• Assume an increment of work is done to just stop the flow of K down its gradient but no greater work.

Page 70: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Sources of energy driving the Nernst equation

• Diffusion gradient.

• The generated electrical field (Separation of Charge)

Page 71: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

• The differential concentrations (Diffusion)

Page 72: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Diffusion gradient of K

Page 73: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,
Page 74: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Work opposing diffusion

• δWc = δn(R)(T) ln([x]out/[x]in)

Where δW = increment of work

δn = increment of number of moles moved.R = gas constant (8.314 J deg-1 mole-1)

T = absolute temperature X = molar concentrations of solute in compartment 1 an 2

Page 75: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Work of opposing electromotive force

• Work of electromotive force opposing diffusion

δWe = δn (zFE)

δWe = increment of work. δn = moles moved against an electrical gradient. Z = valence of the ion moved. F = Faraday’s constant (96,500). E = the potential difference between the two compartments.

Page 76: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

At Equilibrium, no net movement of X

• δWe = δWc

or

• δn (z) (FE) = δn (R)(T)ln([X]1/[X]2)

• Solving for E

Page 77: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Nernst Equation

• E = (RT/zF)ln([X]1/[X]2)• or • E = (25/z)ln([X]1/[X]2)• or • enumerating the constants• E = (58/z)log10([X1/X]2)• at 18o C• E is in millivolts.

Page 78: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

CRITICAL PROPERTIES OF THE NERNST EQUATION

• Applies to only one ion at a time. Each ion will have its own equilibrium potential.

Page 79: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Property 1

• Applies only to those ions that can cross the membrane.

Page 80: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Property 2

• At equilibrium ions move across the membrane, but there is no net change in the number of ions that move per unit time.

Page 81: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Nernst equation (cont)

• If you exceed the equilibrium potential in excitable cells, the direction of current flow will be reversed and ions will flow in the opposite direction up hill (more on this later).

Page 82: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

Implications

• If the concentration in one of the two chambers is changed, the voltage E must change.

• If the voltage changes, the ratio of the two compartments change and the concentrations must change with respect to each other.

Page 83: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

The Effect External Δ Potassium Ion Concentrations on Membrane

Potentials

Page 84: Lecture notes Taken in part from: Adley, D. J. (1991) The Physiology of Excitable Cells, Cambridge,3ed. Calabrese, R. C., Gordon, J., Hawkins, R., & Qian,

The Resting Membrane Potential

• There is a resting membrane potential for all cells.

• Requires: Selectively permeable membrane, diffusion gradient, separation of charge