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Charged and neutral ion carriers through bimolecular phospholipid membranes
Charged and neutral ion carriers through bimolecular phospholipid membranes
1970
Biochimica et Biophysica Acta (BBA) - Biomembranes
1970
1970
Biochimica et Biophysica Acta (BBA) - Biomembranes
V. 196, № 2, 221-234
V. 196, № 2, 221-234
doi.org
Abstract
Abstract
АННОТАЦИЯ
АННОТАЦИЯ
1. In order to clarify the influence of configuration of molecules on their motion within bimolecular phospholipid membranes the electrical properties of these membranes in the presence of “spherical” lipid-soluble molecules of 1,2-dicarbadodecaborane (barene) derivatives were investigated. Decachlorobarene in the pH region 2 13 is an effective carrier of H+ through bimolecular membranes, and as well as other proton carriers, is an uncoupler of oxidative phosphorylation. The mercury derivatives of barene are carriers of the halogenn and rhodanide anions. Phenyldicarbaundecaborane anions easily penetrate bimolecular membranes.
2. In the presence of decachlorobarene at pH higher than the pK of decachlorobarene (pH > 12), and at sufficiency high concentrations of I−, Br− and Cl− in the presence of dibarenylmercuryl, the bimolecular membranes have stationary current-voltage characteristics with negative resistance. This confirms the supposition that such characteristics should be observed when the two forms of ion carrier have a charge of the same sign.
3. The N-type current-voltage curves of bimolecular membranes in the presence of tetrachloro-2-trifluoromethylbenzimidazole, copper ions and hydroxyammonium may also be accounted for within the framework of this hypothesis.
4. On the curves of dependence of current on the time after the rapid change of the fixed membrane voltage the carrier current is observed which is followed by the time dependent current of penetrating ions, the initial membrane potential difference, and the value of the potential change. In the presence of a transmembrane concentration gradient of penetrating ions the time course of these currents also depends on the direction of the electric field applied and the charge sign of the carriers and ions carried. This dependence can be accounted for by the assumption that the direction of the field determines the side of the membrane to which the charged carriers are “pressed” before the change of the fixed voltage.
5. When the carriers are introduced only into the bimolecular membranes, the current-voltage curves change with time owing to carrier leaving the membrane for the solutions. This process is accelerated by the mixing of the water solutions. When only one solution is mixed, the time course of current-voltage curves depends on the value and direction of the electric field. Such experiments enable the charge sign of the carriers in the membrane to be determined. With decachlorobarene at pH > 12 the two forms of H− carriers are negatively charged. The I−, Br− and Cl− carriers — the complexes of dibarenylmercury with these ions — are also negatively charged. With tetrachloro-2-trifluoromethylbenzimidazole, copper ions and hydroxyammonium (pH 6.0) the two forms of the carrier are positively charged. In the absence of penetrating ions, carriers of the dibarenylmercury type are not charged.
6. A hypothesis is suggested on the nature of the carriers which can be responsible for the properties of excitable cell membranes. An assumption is made that K+ and Na+ carriers of the valinomycin or gramicidin type can serve as excitability inducing substances if the molecules of these carriers contain one positive or two negative chemically linked charges, or if two or more similar molecules are linked together by flexible bonds which do not hinder the complexing with cations. Such an effect should also be observed if the mobile lipid-soluble molecules complex with two or more cations.
1. In order to clarify the influence of configuration of molecules on their motion within bimolecular phospholipid membranes the electrical properties of these membranes in the presence of “spherical” lipid-soluble molecules of 1,2-dicarbadodecaborane (barene) derivatives were investigated. Decachlorobarene in the pH region 2 13 is an effective carrier of H+ through bimolecular membranes, and as well as other proton carriers, is an uncoupler of oxidative phosphorylation. The mercury derivatives of barene are carriers of the halogenn and rhodanide anions. Phenyldicarbaundecaborane anions easily penetrate bimolecular membranes.
2. In the presence of decachlorobarene at pH higher than the pK of decachlorobarene (pH > 12), and at sufficiency high concentrations of I−, Br− and Cl− in the presence of dibarenylmercuryl, the bimolecular membranes have stationary current-voltage characteristics with negative resistance. This confirms the supposition that such characteristics should be observed when the two forms of ion carrier have a charge of the same sign.
3. The N-type current-voltage curves of bimolecular membranes in the presence of tetrachloro-2-trifluoromethylbenzimidazole, copper ions and hydroxyammonium may also be accounted for within the framework of this hypothesis.
4. On the curves of dependence of current on the time after the rapid change of the fixed membrane voltage the carrier current is observed which is followed by the time dependent current of penetrating ions, the initial membrane potential difference, and the value of the potential change. In the presence of a transmembrane concentration gradient of penetrating ions the time course of these currents also depends on the direction of the electric field applied and the charge sign of the carriers and ions carried. This dependence can be accounted for by the assumption that the direction of the field determines the side of the membrane to which the charged carriers are “pressed” before the change of the fixed voltage.
5. When the carriers are introduced only into the bimolecular membranes, the current-voltage curves change with time owing to carrier leaving the membrane for the solutions. This process is accelerated by the mixing of the water solutions. When only one solution is mixed, the time course of current-voltage curves depends on the value and direction of the electric field. Such experiments enable the charge sign of the carriers in the membrane to be determined. With decachlorobarene at pH > 12 the two forms of H− carriers are negatively charged. The I−, Br− and Cl− carriers — the complexes of dibarenylmercury with these ions — are also negatively charged. With tetrachloro-2-trifluoromethylbenzimidazole, copper ions and hydroxyammonium (pH 6.0) the two forms of the carrier are positively charged. In the absence of penetrating ions, carriers of the dibarenylmercury type are not charged.
6. A hypothesis is suggested on the nature of the carriers which can be responsible for the properties of excitable cell membranes. An assumption is made that K+ and Na+ carriers of the valinomycin or gramicidin type can serve as excitability inducing substances if the molecules of these carriers contain one positive or two negative chemically linked charges, or if two or more similar molecules are linked together by flexible bonds which do not hinder the complexing with cations. Such an effect should also be observed if the mobile lipid-soluble molecules complex with two or more cations.
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