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Synaptic transmission Presynaptic release of neurotransmitter Quantal analysis Postsynaptic receptors Single channel transmission Models of AMPA and NMDA receptors Analysis of two state models Realistic models
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Synaptic transmission: CNS synapse PNS synapse
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Neuromuscular junction Much of what we know comes from the more accessible large synapses of the neuromuscular junction. This synapse never shows failures.
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Different sizes and shapes I. Presynaptic release II. Postsynaptic, channel openings.
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I. Presynaptic release: The Quantal Hypothesis A single spontaneous release event – mini. Mini amplitudes, recorded postsynaptically are variable. I. Presynaptic release
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Assumption: minis result from a release of a single ‘quanta’. The variability can come from recording noise or from variability in quantal size. Quanta = vesicle
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A single mini Induced release is multi-quantal
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Statistics of the quantal hypothesis: N available vesicles P r - prob. Of release Binomial statistics:
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N available vesicles P r - prob. Of release Binomial statistics: Examples mean: variance: Note – in real data, the variance is larger
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Yoshimura Y, Kimura F, Tsumoto T, 1999 Example of cortical quantal release
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Short term synaptic dynamics: depression facilitation
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Synaptic depression: N r - vesicles available for release. P r - probability of release. Upon a release event N r P r of the vesicles are moved to another pool, not immediately available (N u ). Used vesicles are recycled back to available pool, with a time constant τ u
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Therefore: And for many AP’s: NuNu NrNr 1/τ u
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Show examples of short term depression. How might facilitation work?
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There are two major types of excitatory glutamate receptors in the CNS: AMPA receptors And NMDA receptors II. Postsynaptic, channel openings.
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Openings, look like: but actually
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Openings, look like: How do we model this?
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A simple option: Assume for simplicity that: Furthermore, that glutamate is briefly at a high value G max and then goes back to zero.
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Assume for simplicity that: Examine two extreme cases: 1) Rising phase, kG max >>β s :
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Rising phase, time constant= 1/(k[Glu]) Where the time constant, τ rise = 1/(k[Glu]) τ rise
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2) Falling phase, [Glu]=0: rising phase combined
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Simple algebraic form of synaptic conductance: Where B is a normalization constant, and τ 1 > τ 2 is the fall time. Or the even simpler ‘alpha’ function: which peaks at t= τ s
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Variability of synaptic conductance through N receptors (do on board)
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A more realistic model of an AMPA receptor Closed Open Bound 1 Bound 2 Desensitized 1 Markov model as in Lester and Jahr, (1992), Franks et. al. (2003). K 1 [Glu] K 2 [Glu] K -2 K -1 K3K3 K -3 K -d KdKd
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NMDA receptors are also voltage dependent: Jahr and Stevens; 90 Can this also be done with a dynamical equation? Why is the use this algebraic form justified?
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NMDA model is both ligand and voltage dependent
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Homework 4. a.Implement a 2 state, stochastic, receptor Assume α=1, β=0.1, and glue is 1 between times 1 and 2. Run this stochastic model many times from time 0 to 30, show the average probability of being in an open state (proportional to current). b. Implement using an ODE a model to calculate the average current, compare to a. and to analytical curve
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c. Implement using an ODE the following 5-state receptor: Closed Open Bound 1 Bound 2 Desensitized 1 K 1 [Glu] K 2 [Glu] K -2 K -1 K3K3 K -3 K -d KdKd Assume there are two pulses of [Glu]= ?, for a duration of 0.2 ms each, 10 ms apart. Show the resulting currents K 1 =13; [mM/msec]; K -1 =5.9*(10^(-3)); [1/ms] K 2 =13; [mM/msec]; K -2 =86; [1/msec] K 3 =2.7; [1/msec]; K -3 =0.2; [ 1/msec] K d =0.9 [1/msec]; K -d =0.9
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Summary
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