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Biorheology is an international interdisciplinary journal that publishes research on the deformation and flow properties of biological systems or materials. It is the aim of the editors and publishers of
Biorheology to bring together contributions from those working in various fields of biorheological research from all over the world. A diverse editorial board with broad international representation provides guidance and expertise in wide-ranging applications of rheological methods to biological systems and materials.
The aim of biorheological research is to determine and characterize the dynamics of physiological processes at all levels of organization. Manuscripts should report original theoretical and/or experimental research promoting the scientific and technological advances in a broad field that ranges from the rheology of macromolecules and macromolecular arrays to cell, tissue and organ rheology. In all these areas, the interrelationships of rheological properties of the systems or materials investigated and their structural and functional aspects are stressed.
The scope of papers solicited by
Biorheology extends to systems at different levels of organization that have never been studied before, or, if studied previously, have either never been analyzed in terms of their rheological properties or have not been studied from the point of view of the rheological matching between their structural and functional properties. This biorheological approach applies in particular to molecular studies where changes of physical properties and conformation are investigated without reference to how the process actually takes place, how the forces generated are matched to the properties of the structures and environment concerned, proper time scales, or what structures or strength of structures are required.
Biorheology invites papers in which such 'molecular biorheological' aspects, whether in animal or plant systems, are examined and discussed. While we emphasize the biorheology of physiological function in organs and systems, the biorheology of disease is of equal interest. Biorheological analyses of pathological processes and their clinical implications are encouraged, including basic clinical research on hemodynamics and hemorheology.
In keeping with the rapidly developing fields of mechanobiology and regenerative medicine,
Biorheology aims to include studies of the rheological aspects of these fields by focusing on the dynamics of mechanical stress formation and the response of biological materials at the molecular and cellular level resulting from fluid-solid interactions. With increasing focus on new applications of nanotechnology to biological systems, rheological studies of the behavior of biological materials in therapeutic or diagnostic medical devices operating at the micro and nano scales are most welcome.
Abstract: A theory for the rheological behavior and fluid flux in swelling tissues under small deformations is presented. Tissues are considered as bicomponent solid-fluid mixtures. Concentration effects are included. The driving forces (body, surface and interactive), are discussed and their constitutive relationships to the tissue’s deformation are specified. Mass and momentum balance equations are developed for each component and for the tissue as a whole. The concept of swelling stress emerges from the theory as an anisotropic generalization of the commonly used swelling pressure. It is shown to be a measure of the total chemical potential combining both mechanical and concentration…effects. The theory shows that concentration effects modify the tissue’s bulk stiffness in a manner consistent with experimental observations.
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Abstract: The response of a cartilage disc to unconfined compressive loading under small deformations is analyzed. The cartilage is considered as a transversely isotropic bicomponent (solid-fluid) tissue. Concentration effects (commonly termed osmotic pressure) are accounted for. The tissue’s permeability is taken to be isotropic. Its concentration force is assumed to vary linearly with volume. The analysis shows that if the tissue’s fibrous structure is taken into consideration, then the instantaneous response to a step loading depends on the tissue’s elasticity and on its concentration force. The subsequent creep response, under commonly used experimental conditions, has a time constant which depends…on the concentration force and permeability, but independent of its elastic response. The equilibrium volume is predicted to depend only on the concentration force. Where data is available it confirms the model’s predictions. It is concluded from the present analysis that inclusion of concentration effects and the tissue’s fibrous structure has significant consequences in terms of the relative roles of the collagen fibers (solid) vs. the ground substance (fluid) in the response of the cartilage to compressive loading.
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Abstract: Measurements were made of the viscosity of suspensions of synthetic erythrocytes composed of hemoglobin solutions encapsulated in liposomes, as a function of shear rate, temperature, suspension concentration, lipid membrane composition, and the viscosity of the suspending medium. It was found that the viscous behavior of the synthetic erythrocyte suspensions was non-Newtonian and nearly the same as that of suspensions of natural erythrocytes prepared similarly, with the major difference being that synthetic erythrocyte suspensions are somewhat more viscous. Suspensions of Fluosol FC-43 prepared similarly were found to be essentially Newtonian fluids, and substantially different and more viscous than either erythrocyte suspension.…The higher viscosity of synthetic erythrocyte suspensions probably accounts for the ability of these suspensions to maintain normal systemic vascular resistance in transfusion experiments, in spite of the fact that synthetic erythrocytes are smaller than natural erythrocytes.
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Abstract: The bulk modulus of a dilutely dispersed system of spherical shell structures is obtained taking into account interfacial tensions at both the interfaces of the shell as follows: κ ∗ = κ Q + 4 3 c μ Q ′ Q − c Q ′ where Q = K ′ K m − Δ K ′ Δ MA 3 , Q…′ = K ′ Δ K − Δ K ′ KA 3 , K m = 3 κ m + 4 μ − 2 γ / a , Δ K = 3 κ m − 3 κ − 2 γ / a , Δ M = 4 μ m − 4 μ + 2 γ / a , K = 4 μ m + 3 κ + 2 γ / a , K ′ = 3 κ ′ + 4 μ m − 2 γ ′ / a ′ , Δ K ′ = 3 κ m − 3 κ ′ + 2 γ ′ / a ′ , A = a′/a, a and a′ are the outer and the inner radii of the shell, γ and γ ′ the interfacial tensions at r = a and r = a′, in which r is the radial distance from the origin at the center of the shell structure, κ and μ the bulk modulus and the rigidity of the medium, in which the prime and the subscripts m denote the quantities for the inside (r<a′) and the shell (a′<r<a) regions, respectively, and c the volume concentration of shell structures.
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Abstract: The following paper is a brief presentation of problems related to the concepts of diffusion coefficient D and so-called viscosity η used to characterize the cohesion of biological membranes. The first approach to this problem is a recall of the definition of D and η in liquids. It appears that the models developed with exogenous probes to account for the diffusion-viscosity relationship are not verified in membranes. The existence of complex diffusional mechanisms, the influence of the size of the probe are presented. The results of a model calculation suggest that there is no direct correlation other than…great simplifications, between the diffusion coefficient and viscosity. The calculations are then extended to actual biological assemblies and the influence of proteins on the motion of the probe considered. The limitations of the methods involving exogeneous probes for determining the cohesion of biological membranes are discussed.
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