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Titlebook: Ion Transport through Biological Membranes; An Integrated Theore Michael C. Mackey Book 1975 Springer-Verlag Berlin · Heidelberg 1975 Bioma

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楼主: 深谋远虑
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Conservation and Field Equationsnd concentration gradients across the membrane. All of the derivations of the conservation equations in this chapter are to be found in Mackey and McNeel (1973), and also can be found in alternate forms in the literature. In Chapter 12 I illustrate how they arise naturally from a molecular formulation of ED theory.
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Admittance Properties of the Electrodiffusion Equationsof . and the excitable cell from .. Transverse impedance measurements on both of these systems in the resting state gave data that was interpreted as arising from a membrane capacity (C.) of approximately 1μ.F/cm. in parallel with a membrane resistance (R.) on the order of 10. ohm-cm. (Curtis and Cole 1938; Cole and Hodgkin, 1939).
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Relationship Between the Microscopic and Macroscopic Formulations of Electrodiffusion Theoryonservation equations. The same basic physical model was developed in the previous chapter, but from a microscopic basis. It is the purpose of this chapter to examine the connection between the two approaches.
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The Microscopic Model in a Steady State: No Concentration Gradientsgradients across the membrane. After some preliminary remarks on spatial gradients, I pass to considerations of predicted ionic chord conductance, interionic selectivity, and chord conductance temperature coefficients as functions of applied electric field strength, and ion-scatterer interactions and parameters.
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Steady State and Dynamical Properties of the Macroscopic Modelvement when t. ≪ t. and ionic energy is essentially unaltered by the presence of electric fields or concentration gradients. In Chapter 12 I connected the macroscopic model with the microscopic model developed in Chapter 11. In this chapter I examine some of the steady state and time dependent properties of the macroscopic model.
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