Electron-Gated Ion Channels : With Amplification by NH3 by Wilson P. Ralston PDF

By Wilson P. Ralston

ISBN-10: 1891121413

ISBN-13: 9781891121418

With greater than a hundred billion (10^11) neurons in our apprehensive approach, each one having hundreds of thousands of ion channels, nature may most likely have advanced an easy, strong, low-energy gating approach to manage the circulate of ions into and out of the telephone. the sort of method, in line with electron tunneling and quantum mechanics, is the topic of this booklet documenting the author’s learn on electron gating. Electron tunneling in proteins is a much-studied phenomenon; although, for electrons to manage ion channel gates, a mechanism for amplification is needed. in the course of the study, it was once came across that NH3 teams on the finish of arginine and lysine facet chains are inverting and extending the sensitivity of electron move to adjustments within the electrical box. The inversion frequency for NH3, at the arginine aspect chain, was firm experimentally in Blue Fluorescent Protein utilizing a brand new microwave spectroscopy process built for this goal. The inversion frequency of NH3 in the fuel part happens at approximately 24 GHz and is used for amplification within the ammonia maser. This frequency, decreased by means of the attachment of NH3 to the part chain, is the foundation for amplification at arginine and lysine websites. The amplification resulted in improvement of electron gating versions for sodium and potassium ion channels and to a version for calcium oscillators. The electron gating versions fit and clarify, for the 1st time, the advanced expense curves, defined through the vintage (1952) Hodgkin-Huxley equations. Amplified electron tunneling and gating opens the door to figuring out nature’s mechanisms for timing, reminiscence, and calcium signaling.

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Extra info for Electron-Gated Ion Channels : With Amplification by NH3 Inversion Resonance

Sample text

Usually capacitors have a constant capacitance, with charge increasing linearly with voltage. Here, an exponential change in capacitance with voltage provides the necessary characteristic to model the charge displacement between tunneling sites with changes in membrane voltage. 1) where vn is the voltage across the capacitor, n is the site number, C0 is the capacitance with vn equal to zero, and H' is a sensitivity factor. With two THE SETCAP MODEL 39 capacitors connected in a series configuration, as in Fig.

E should be the same as the experimentally determined sensitivity for J3m. From this, the amplification can be determined by equating the sensitivity for fit with the corresponding 1/18 voltage sensitivity for the Hodgkin-Huxley rate constant J3m. 106 (Eq. m was used for matching, because (according to the model) the am sensitivity is reduced, due to the electron probability being spread over four or five arginine or lysine tunneling sites. The abovecalculated amplification is for a temperature of 6°C.

The more general form N-1 is used, instead of 3, to allow expansion of the equation for an N site model. 35) Substituting in terms from Eq. 1, gives (3 36) The rate constant at is equal to a/RCa and K0 is defined as G/RC0 (Eq. 5). 38) 48 ELECTRON-GATED ION CHANNELS Fig. 3-3. A SETCAP circuit model for four arginine electron-tunneling sites spaced every third residue. The potential v across adjacent tunneling sites is determined by the net electric field, which varies with the membrane voltage. With v = 0, the average negative charge on each capacitor is XA e.

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Electron-Gated Ion Channels : With Amplification by NH3 Inversion Resonance by Wilson P. Ralston


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