Publications
ПУБЛИКАЦИИ
Selective transport of ions through bimolecular phospholipid membranes
Selective transport of ions through bimolecular phospholipid membranes
Selective transport of ions through bimolecular phospholipid membranes
1968
Biochimica et Biophysica Acta (BBA) - Biomembranes
1968
Biochimica et Biophysica Acta (BBA) - Biomembranes
1968
Biochimica et Biophysica Acta (BBA) - Biomembranes
V. 163, № 2, 125-136
V. 163, № 2, 125-136
doi.org
Abstract
Abstract
АННОТАЦИЯ
АННОТАЦИЯ
1. The mechanism of ion transport through bimolecular phospholipid membranes in the presence of a number of lipid-soluble substances was studied.
2. Membrane conductance sharply increases on adding these substances to a lipid solution in heptane, or to aqueous solutions separated by a membrane, if transported ions are present in these solutions. The conductance increases linearly, or with the square of the concentration of carriers.
3. At constant concentration of the carrier, the bimolecular membrane conductance depends non-linearly on the concentration of the transported ion. Conductance reaches a maximum in the region of concentrations of transported ion corresponding to the binding of approximately one-half of the carriers on the membrane surface.
4. Current-voltage curves of bimolecular phospholipid membranes in the presence of the carriers are non-linear. In solutions of low buffer capacity effects connected with the diffusion overpotential near the membrane surface are observed.
5. In the presence of certain carriers the current-voltage curves show a region with negative resistance.
6. A potential difference arises from a transmembrane concentration gradient of penetrating ions or from the carrier-charged species. This potential difference has its maximum in the same region of concentration of transported ions as the conductance.
7. Direct passage of the charged form of the carrier through the membrane and the comparatively slow increase of conductance with the concentration of carrier indicate that the ions do not pass through the “pores” in bimolecular phospholipid membrane or by “relay-race” mechanism, but are transported by mobile carriers.
8. When an osmotic pressure gradient is created by sucrose in the presence of tetrachloro-2-trifluoromethylbenzimidazole, a potential difference arises which corresponds to the charged form being carried along by water flow.
9. The conductance of thick layers of non-polar solvent is changed insignificantly on adding the carrier to aqueous solution. This is connected with the rise of spacial charge. The presence in aqueous solutions of two carrier—one of which is charged positively and the second one negatively—results in a significant increase of conductance of such layers. This effect is also observe on bimolecular membranes.
10. An hypothesis is suggested whereby the selective transport of ions (X=) through bimolecular phospholipid membranes is performed by charged (C±) or uncharged (C) carriers. Ions are bound with the carrier by a chemical reaction on a membrane surface. The current through the membrane is carried by a charged form (C± or CX±. The uncharged form (C or CX) diffuses along the concentration gradient. In some cases one carrier molecule and in other cases two molecules participate in the transport of one ion.
1. The mechanism of ion transport through bimolecular phospholipid membranes in the presence of a number of lipid-soluble substances was studied.
2. Membrane conductance sharply increases on adding these substances to a lipid solution in heptane, or to aqueous solutions separated by a membrane, if transported ions are present in these solutions. The conductance increases linearly, or with the square of the concentration of carriers.
3. At constant concentration of the carrier, the bimolecular membrane conductance depends non-linearly on the concentration of the transported ion. Conductance reaches a maximum in the region of concentrations of transported ion corresponding to the binding of approximately one-half of the carriers on the membrane surface.
4. Current-voltage curves of bimolecular phospholipid membranes in the presence of the carriers are non-linear. In solutions of low buffer capacity effects connected with the diffusion overpotential near the membrane surface are observed.
5. In the presence of certain carriers the current-voltage curves show a region with negative resistance.
6. A potential difference arises from a transmembrane concentration gradient of penetrating ions or from the carrier-charged species. This potential difference has its maximum in the same region of concentration of transported ions as the conductance.
7. Direct passage of the charged form of the carrier through the membrane and the comparatively slow increase of conductance with the concentration of carrier indicate that the ions do not pass through the “pores” in bimolecular phospholipid membrane or by “relay-race” mechanism, but are transported by mobile carriers.
8. When an osmotic pressure gradient is created by sucrose in the presence of tetrachloro-2-trifluoromethylbenzimidazole, a potential difference arises which corresponds to the charged form being carried along by water flow.
9. The conductance of thick layers of non-polar solvent is changed insignificantly on adding the carrier to aqueous solution. This is connected with the rise of spacial charge. The presence in aqueous solutions of two carrier—one of which is charged positively and the second one negatively—results in a significant increase of conductance of such layers. This effect is also observe on bimolecular membranes.
10. An hypothesis is suggested whereby the selective transport of ions (X=) through bimolecular phospholipid membranes is performed by charged (C±) or uncharged (C) carriers. Ions are bound with the carrier by a chemical reaction on a membrane surface. The current through the membrane is carried by a charged form (C± or CX±. The uncharged form (C or CX) diffuses along the concentration gradient. In some cases one carrier molecule and in other cases two molecules participate in the transport of one ion.
chaimatics
Chaimatics
Discovery of links between the biology, physics and mathematics, and founding a new area of studies focused on computations in living systems are his life achievements. Efim Liberman gave the name of “Chaimatics” to this new area of science
I
DNA is the text of a code written for molecular computers of living cells. The notion of “Text” is intrinsically opposite to a random sequence of symbols, and it can exist only inside the system of language. In this case, it is a genetic language, which is isomorphic to a natural language
II
Computations conducted in a living cell are real physical actions, and free energy and time must be spent for completing them. As all living organisms are comprised of cells, this statement is applicable to any control processes implemented in the biosphere
III
Molecular computations are limited by the microscopic scale of a cell and inevitable impact of the computations on formulation of a problem begin solved. The Chaimatics grew from the recognition of the computation reality as the quantum mechanics grew from the recognition of the measurement reality.
IV
A cell creates а quantum computing tool for solving complex problems. This tool utilizes hypersound quanta, and uses the cell cytoskeleton as the computing environment. In such a computer, a price of elementary computation converges to the physical limit, which is Planck’s constant
Chaimatic's statements are simple, but they require a change in the traditional vision, rooted in scientific practice
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Chapter I
The journey of life in science
chaimatics
хаиматика
хаиматика
Итогом жизни в науке стало установление связей между биологией, физикой, математикой и новая область исследования, посвященная вычислениям в живых системах. Ефим Либерман дал имя новой науке: «Хаиматика»
I
ДНК – это текст программы для молекулярных компьютеров клеток. «Текст» по определению не случайная последовательность знаков и может существовать только внутри языковой системы. В данном случае это генетический язык, изоморфный естественному языку
II
Вычисление в живой клетке является реальным физическим действием и требует затрат свободной энергии и времени. Поскольку все живые организмы состоят из клеток, это относится ко всему управлению, которое осуществляется в биосфере
III
Молекулярные вычисления ограничены микроскопическим объемом клетки и принципиальной возможностью влияния вычисления на условия решаемой задачи: квантовая механика возникла из осознания реальности измерения, Хаиматика - из реальности вычисления
IV
Для решения сложных задач клетка создает устройство квантового вычисления, использующего кванты гиперзвука и клеточный цитоскелет, как вычисляющую среду. Цена вычисления в таком компьютере стремится к физическому пределу – постоянной Планка
Утверждения Хаиматики просты, но они требуют изменения традиционных представлений, принятых в научной практике
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Глава I
Как все начиналось
хаиматика