Life at the Cell and Below-Cell Level. The Hidden History of a Fundamental Revolution in Biology
Gilbert N. Ling, Ph.D.
Pacific Press
ISBN 0-9707322-0-1

"Dr. Ling is one of the most inventive biochemist I have ever met."
Prof. Albert Szent-Györgyi,
Nobel Laureate

Chapter 15.

Physiological Activities: Electronic Mechanisms and Their Control by ATP, Drugs, Hormones and Other Cardinal Adsorbents
(p. 179-232)

The membrane theory once gained world-wide acceptance for its success in explaining four major physiological manifestations of the living cells: solute distribution, permeability, swelling and shrinkage and resting potential. The demonstration that the cell membrane is in fact permeable to sucrose and Na+ made the original membrane theory difficult to defend. In response, the sodium pump hypothesis was installed. In time, this subsidiary hypothesis also met serious contradictions, even harder to defend. And with it, the paradigm of cells as membrane-enclosed dilute solutions is, in my opinion, coming to an end.

In presenting the LFCH and the PM theory, we focused primarily on two basic cell physiological phenomena: selective K+ adsorption and Na+ exclusion on one hand; multilayer polarization and orientation of cell water on the other. Both are static manifestations of the resting living state. The first part of the present chapter offers new interpretations of the four classic static physiological manifestations mentioned above: solute distribution, permeability, swelling and shrinkage and resting potential in the light of the AI Hypothesis. We then examine how these physiological manifestations are controlled by ATP, drugs, hormones or other cardinal adsorbents through the operation of the electronic control mechanism described in the preceding chapter. In addition, I shall also tackle two dynamic cell physiological activities: the action potential and true active transport.


Figure 54. Equilibrium distribution of Na+ in frog muscle cells at 0°C in the presence of 2.5, 5.0 or 15 mM of К+. in the bathing medium after a correction was made for Na+ trapped in the extracellular space of 10%. (Later work revised this figure to 9%, but no attempt was made to revise this graph, which is reproduced as it was published in 1969.) The ordinate is in units of μmoles/gram of fresh muscle cells. The straight line going through or near most experimental points at the two higher K+ concentrations has a slope of 0.14. A q-value of 0.18 was obtained for Na+ (mostly as chloride) by dividing 0.14 by the percentage of water in the muscle cells (80%). In this estimate, no correction was made for Na+ associated with "connective tissue elements" (etc.). Using existing information on hand, 1 estimated later that the q-value of Na+ (as chloride) in the water of frog muscle cells is probably between 0.14 and 0.18. 0.15 would be a good estimate. (Ling173 from the International Review of Cytology by permission of Academic Press)


15.1 Selective solute distribution in living cells; cooperativity and control

In this section, we resume our discourse on the distribution of Na+ and K+ (and Mg2+) in frog muscle cells. More specifically, we focus attention on the influence of ATP on the state of cell water and K+; and the influence of the cardiac glycoside, ouabain, on the accumulation of this and other alkali-metal ions in frog muscles.

After that, I shall discuss the accumulation in frog muscle cells of D-glucose and the free amino acid, glycine; and their respective control by the hormone, insulin. In addition, I shall also touch upon lactose accumulation in the bacteria, Escherichia coli (E. coli).

(1) K+, Na+ and Mg2+ accumulation in living cells

In a preceding section [10.2], I have devoted much space establishing the adsorbed state of cell K+. We now turn our attention to Na+ and Mg2+ which so far have been kept on a back burner.

Figure 54 shows the equilibrium distribution of Na+ in frog muscle at 0°C in the presence of a normal external K+ concentration (2.5 mM) and higher ones.173 The data show general obedience to the Troshin equation (Equation Al in Appendix 1), which describes a free fraction of Na+ in the cell water and another fraction of adsorbed Na+.

After the adsorbed fraction of Na+ is chased away by K+ at the higher concentrations, a straight-line plot of the remaining Na+ in the tissue water against external Na+ concentration is obtained with a slope of 0.14. After corrections for Na+ trapped in the extracellular space and adsorbed on "connective tissue elements," one obtains a q-value of 0.15 for Na+ (as chloride) in frog muscle cell water. The q-value for sucrose in frog muscle cell water at the same temperature (0°C) is, as seen in Figure 27, 0.13.156 p 191

While the distribution of (univalent) Na+ in frog muscle depends strongly upon the concentration of (univalent) K+, the distribution of (divalent) Mg2+ in both frog muscle and frog ovarian eggs is indifferent to the concentration of (univalent) K+ as the studies of Ling, Walton and Ling have revealed.502 Similarly, the distribution of K+ is also indifferent to the concentration of Mg2+ in the bathing medium. This mutual indifference is in conflict with the membrane theory as expounded by Donnan [4.3] where the same Donnan ratio governs the distribution of all permeant ions 98 p 216; 15 p 28; 107 p 17 as  well as the resting potential (Figure 4B). By the same token, it is in harmony with the AI Hypothesis, according to which there is no causal relationship between the resting potential and bulk phase ionic distribution, nor obligatory relationship between monovalent and divalent ion distribution as they adsorb in the cells on separate and different types of sites.

In frog muscle there are about 12 mmoles of Mg2+ adsorbing sites with strong affinity for this ion—reaching full saturation at an external Mg2+ of 1 mM (or less) (1 mM is the lowest concentration we studied). The q-value of Mg2+ (as chloride) is 0.21 at 25°C. To a first approximation, the data can also be described by the Troshin equation.

The Troshin equation is a special case of Ling's general equation for solute distribution in living cells and model systems156 (presented as Equation A3 in Appendix 1). In the theory, which the Troshin equation stands for, there is no cooperative interaction among the adsorption sites. In the Al Hypothesis, on the other hand, cooperativity among the β- and γ-carboxyl and other proximal functional groups is a universal feature. But it may be undetectable under some conditions.

Autocooperativity becomes detectable when the nearest neighbor interaction energy is much larger than zero (-γ/2 >> 0). -γ/2 is much larger than zero, when the alternative adsorbents have widely different adsorption energies (for details, see Reference 107 p 139-140), as in the case when frog muscles are in an environment containing a high concentration of Na+ and very low K+ concentration. Autocooperativity is evident in the (sigmoid) uptake curve of K+ in Figure 55, which resembles the oxygen uptake curve of human erythrocytes shown in the inset. In contrast, oxygen uptake of myoglobin—shown on the left of the inset—does not exhibit autocooperativity. Instead, it follows a "hyperbolic" uptake curve characteristic of Langmuir adsorption (with no discernible near-neighbor interaction).


 Figure 55. Equilibrium K+ concentration in frog sartorius muscles at 25°C in Ringer's solution containing an unvarying high concentration of Na+ concentration (100 mM) but varying (low) K+ concentration (abscissa). The sigmoid profile resembles that of oxygen uptake by human erythrocytes shown in the inset as the line going through or near the filled circles. The solid line to the left in the inset shows oxygen uptake of isolated myoglobin. (Inset from Eastman et al.440) (Ling439 by permission of Federation Proceedings)

Parenthetically, I may add that a straight-line distribution curve with a slope significantly lower than unity—like that shown for Na+ in the presence of higher K+ concentration in Figure 54, and that shown for Mg2+ above an external Mg2+ concentration of 1 mM, as well as those of the many larger nonelectrolytes shown in Figures 26 and 27—is theoretically incompatible with a pump-mechanism. An outward pumping mechanism needed to maintain a low intracellular concentration of a solute would inevitably predict not a straight line but a concave-upward distribution curve as a result of the increasing saturation of pumping sites with rising concentration of the solute being pumped, represented on the abscissa.174

To be continued

Разделы книги
"Life at the Cell and Below-Cell Level.
The Hidden History of a Fundamental Revolution in Biology":

Contents (PDF 218 Kb)
Preface (
PDF 155 Kb)
Answers to Reader's Queries (Read First!) (
PDF 120 Kb)

1. How It Began on the Wrong Foot---Perhaps Inescapably
2. The Same Mistake Repeated in Cell Physiology
3. How the Membrane Theory Began
4. Evidence for a Cell Membrane Covering All Living Cells
5. Evidence for the Cell Content as a Dilute Solution
6. Colloid, the Brain Child of a Chemist
7. Legacy of the Nearly Forgotten Pioneers
8. Aftermath of the Rout
9. Troshin's Sorption Theory for Solute Distribution
10. Ling's Fixed Charge Hypothesis (LFCH)
11. The Polarized Multilayer Theory of Cell Water
12. The Membrane-Pump Theory and Grave Contradictions
13. The Physico-chemical Makeup of the Cell Membrane
14. The Living State: Electronic Mechanisms for its Maintenance and Control
15. Physiological Activities: Electronic Mechanisms and Their Control by ATP, Drugs, Hormones and Other Cardinal Adsorbents
16. Summary Plus
17. Epilogue 

A Super-Glossary
List of Abbreviations
List of Figures, Tables and Equations
References (
PDF 193 Kb)
Subject Index
About the Author

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