Stochastic Narrow Escape in Molecular and Cellular Biology by David Holcman & Zeev Schuss

Stochastic Narrow Escape in Molecular and Cellular Biology by David Holcman & Zeev Schuss

Author:David Holcman & Zeev Schuss
Language: eng
Format: epub
Publisher: Springer New York, New York, NY


(4.11)

where D is the diffusion coefficient of a free glutamate molecule. The partial absorption rate constant κ accounts not only for the fraction of AMPARs inside the PSD, but also for the activation barrier of a single glutamate to a glutamate receptor binding site. The rate constant

(4.12)

The absorption rate constant κ e in (4.12) is obtained by calibration with the experimental value κ e  ≈ 1. 6 (see Sect. 4.7 below and Taflia and Holcman 2011). Here a and R PSD are the radii of a single receptor and the PSD, respectively, and N a is the number of AMPARs. The derivation starts by considering that the N a receptors are placed on the PSD, whose surface area is . The criterion for choosing κ is that the absorption flux be equal to the flux on the last line of (4.11) (see Schuss 2013, Sect. 2.​5). Here D is the diffusion constant of glutamate molecules in the cleft and κ e is the partial reflection rate constant of a single AMPAR on a glutamate molecule. This constant is calibrated from (patch-clamp) experimental data.

The probability that a glutamate molecule binds a receptor released at , is the total probability flux into the receptors, that is, into the absorbing boundary ,



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