Electrochemical Gradients Ion Gradients Cell Membranes Ion Channels Topics ITopics II IntroductionSynaptic Transmission Electrochemical GradientsElectrophysiology.

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Presentation transcript:

Electrochemical Gradients Ion Gradients Cell Membranes Ion Channels Topics ITopics II IntroductionSynaptic Transmission Electrochemical GradientsElectrophysiology Techniques Passive Membrane Properties Basic Circuits (Spinal Cord) Action Potential ISensory Systems Overview Voltage-Gated Ion Channels Synaptic Plasticity Ligand-Gated Ion Channels Recapitulation

Study Material NEUROSCIENCE Third Edition – Dale Purves Chapter 2 pages 34-43

Aims for this Lecture Know the values of the main ion concentration gradients. Understand the interaction between diffusion gradients and electrical fields. Know and understand the Nernst equation. Understand the effect of multiple permeabilities (Goldman equation). Know the typical resting membrane potential.

Recapitulation L1 Diffusion is fast over short distances (organelles to small cells), but very slow over long distances (many cells to organs). Multicellular organisms need to communicate and need to do so quickly and efficiently. Electrical signals across cell membranes are the main signals in nervous systems.

Biophysical Basis … why did the ion cross the membrane? All the phenomena that we will be talking about in the next two hours are manifestations of ion flux across membranes. Which brings us to the central question…

Diffusion and Movement Wikimedia: Diffusion Really?

Diffusion X X X X X X X X X X X X X X X X X X X X lr

X X X X X X X X X X X X X X X X X X X X lr

Chemical Potential X X X X X X X X X X X X X X X X X X X X lr Constant pressure and temperature

Electrical Potential K+K+ Cl - K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+

Electrical Potential K+K+ Cl - K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+ K+K+

Equilibrium Electrical FieldChemical Energy nAmount (Mol) zValence (+1 for K) FFaraday‘s constant (charge of one Mole of Ions) EPotential RGas constant TTemperature (absolute K) [ ]Concentration in the respective compartment

Nernst Equation Describes equilibrium No net flux

Specific Equilibrium Potentials IntracellularExtracellularE Potassium Ions 155 mM4 mM-98 mV Sodium Ions 12 mM145 mM+67mV

Mixed Potentials Goldmann, Hodkin, Katz

Resting Membrane Potential Time (s) Potential (mV) Time (s) Potential (mV)

A simple calculation.. Spherical cell 25 μm radius Specific capacitance 1 μF/cm 2 Number of ions, needed to charge this capacitor to 100 mV Total number of ions in a saline solution of 300 mM Fraction of ions needing to cross the membrane Avogadro‘s number ^23 Elementary charge ^-19 C

Electrostatic Force 2 individuals (weighing 72 kg – made up of water for simplicity’s sake). At a distance of 10 m from each other Of all their charged particles (protons electrons..) they decide to exchange 0.5% such that person 1 is positively and person 2 negatively charged. What force do these two persons exert on each other.

Result Coulomb’s law Force = 5.35*10 25 N As a comparison: The gravitational attraction between moon and earth is around 1.98*10 20 N If the two individuals were as far apart from each other as earth and moon, the force would amount to about 3.6*10 10 N

Voltage? How does 70 mV over 8 nm compare to the breakdown voltage in air? Equivalent to 87.5 kV per cm!

Breakdown Voltages Wikipedia

Actively Maintained IntracellularExtracellular Potassium Ions 155 mM4 mM Sodium Ions 12 mM145 mM Na + K+K+ K+K+ 2 3

Na/K ATPase First description The influence of some cations on an adenosine triphosphatase from peripheral nerves. SKOU JC. Biochim Biophys Acta Feb;23(2):

The Simulators Please use the instructions file to unzip and install the simulation environments. For the moment focus on the diffusion simulator and the Goldmann simulator. me questions or even better ask them in class.