Abstract
In this paper, we formulate a thermodynamic model of hemoglobin that describes, by a physical point of view, phenomena favoring the binding of oxygen to the protein. Our study is based on theoretical methods extrapolated by experimental data. After some remarks on the non-equilibrium thermodynamic theory with internal variables, some thermodynamic functions are determined by the value of the complex dielectric constant. In previous papers, we determined the explicit expression of a dielectric constant as a function of a complex dielectric modulus and frequency. The knowledge of these functions allows a new characterization of the material and leads to the study of new phenomena that has yet to be studied. In detail, we introduce the concept of “hemoglobe”, a model that considers the hemoglobin molecule as a plane capacitor, the dielectric of which is almost entirely constituted by the quaternary structure of the protein. This model is suggested by considering a phenomenological coefficient of the non-equilibrium thermodynamic theory related to the displacement polarization current. The comparison of the capacity determined by the mean of this coefficient, and determined by geometrical considerations, gives similar results; although more thermodynamic information is derived by the capacity determined considering the aforementioned coefficient. This was applied to the normal human hemoglobin, homozygous sickle hemoglobin, and sickle cell hemoglobin C disease. Moreover, the energy of the capacitor of the three hemoglobin was determined. Through the identification of displacement currents, the introduction of this model presents new perspectives and helps to explain hemoglobin functionality through a physical point of view.
Highlights
From an evolutionary point of view, the respiratory pigment known as hemoglobin (Hb), appeared very early
We want to show this model as it is related to the non-equilibrium thermodynamics fundamental laws with internal variables and how it is a “consequence” of entropy production and of the phenomenological equations
If the perturbation is not constant and of the harmonic type like the perturbation used in the paper [23], dispersive phenomena can be observed and a complex dielectric function is introduced that will vary with the perturbation frequency
Summary
Francesco Farsaci 1 , Ester Tellone 2, * , Antonio Galtieri 2 and Silvana Ficarra 2.
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