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The sections in this article are: Theoretical Foundations of Water Transport in Epithelia Volume Absorption in the Proximal Tubule Water Permeability of the Proximal Tubule Measurement of Water Permeability Importance of the Osmotic Water Permeability Location of the Osmotic Gradient Luminal Hypotonicity Produced by Solute Absorption Absorbate Hypertonicity “Passive” Driving Forces for Volume Absorption NaCl Diffusion in Volume Absorption Reflection Coefficient Differences Models of Solute‐Solvent Coupling in Proximal Volume Absorption Routes of Volume Movement in the Proximal Nephron Measurement of Cell Membrane Osmotic Water Permeabilities Consequences of Transcellular Volume Flow The ADH ‐Sensitive Distal Nephron Measurement of Permeability Changes Produced by ADH Wafer Permeability of ADH ‐Sensitive Nephron Segments in Vivo and in Vitro Site of the Change in Water Permeability with ADH Evaluation of the P f / P Dw Ratio Large Pore Hypothesis Unstirred Layer Effects The Narrow Channel Hypothesis: Single‐File Diffusion Through Small Aqueous Channels ADH Increases the Number of Narrow Aqueous Channels in Apical Plasma Membranes The Apparent E A for Water Transport in Cortical Collecting Tubules The Raw Data Correction for Diffusion Constraints in Series with Apical Membranes The “True” E A for Water Transport Pseudo‐“Breaks” in E A Measurements Comparison of ADH ‐Dependent Apical Membrane Water Channels with Gramicidin A Channels Parallel Paths for Water and Solute Permeation Morphologic Studies Intracellular Mediators of ADH Action Modulation of ADH Action—α‐Adrenergic Agents Atrial Natriuretic Peptide Prostaglandins Calcium Protein Kinase C Summary
The sections in this article are: Theoretical Foundations of Water Transport in Epithelia Volume Absorption in the Proximal Tubule Water Permeability of the Proximal Tubule Measurement of Water Permeability Importance of the Osmotic Water Permeability Location of the Osmotic Gradient Luminal Hypotonicity Produced by Solute Absorption Absorbate Hypertonicity “Passive” Driving Forces for Volume Absorption NaCl Diffusion in Volume Absorption Reflection Coefficient Differences Models of Solute‐Solvent Coupling in Proximal Volume Absorption Routes of Volume Movement in the Proximal Nephron Measurement of Cell Membrane Osmotic Water Permeabilities Consequences of Transcellular Volume Flow The ADH ‐Sensitive Distal Nephron Measurement of Permeability Changes Produced by ADH Wafer Permeability of ADH ‐Sensitive Nephron Segments in Vivo and in Vitro Site of the Change in Water Permeability with ADH Evaluation of the P f / P Dw Ratio Large Pore Hypothesis Unstirred Layer Effects The Narrow Channel Hypothesis: Single‐File Diffusion Through Small Aqueous Channels ADH Increases the Number of Narrow Aqueous Channels in Apical Plasma Membranes The Apparent E A for Water Transport in Cortical Collecting Tubules The Raw Data Correction for Diffusion Constraints in Series with Apical Membranes The “True” E A for Water Transport Pseudo‐“Breaks” in E A Measurements Comparison of ADH ‐Dependent Apical Membrane Water Channels with Gramicidin A Channels Parallel Paths for Water and Solute Permeation Morphologic Studies Intracellular Mediators of ADH Action Modulation of ADH Action—α‐Adrenergic Agents Atrial Natriuretic Peptide Prostaglandins Calcium Protein Kinase C Summary
Asymmetrically etched ion-track membranes attract great interest for both fundamental and technical reasons because of a large variety of applications. So far, conductometric measurements during track etching provide only limited information about the complicated asymmetric etching process. In this paper, monitoring of osmotic phenomena is used to elucidate the initial phase of nanopore formation. It is shown that strong alkaline solutions generate a considerable osmotic flow of water through newborn conical pores. The interplay between diffusion and convection in the pore channel results in a substantially nonlinear alkali concentration gradient and a rapid change in the pore geometry after breakthrough. Similar phenomena are observed in experiments with cylindrical track-etched pores of 15-30 nm in radius. A theoretical description of the diffusion-convection processes in the pores is provided.
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