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Titlebook: Hyperbolic Geometry; James W. Anderson Textbook 19991st edition Springer-Verlag London 1999 Hyperbolic geometry.Hyperbolic plane.Hyperboli

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ess in the left-ventricular wall may not be zero even if the intraventricular pressure is not present; such a stress is called the residual stress. The values of stresses must be obtained from the appropriate mathematial model, which should be as simple as possible. In the mathematical models propos
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James W. Anderson PhDthe integration of right and left ventricles as a low-pressure and a high-pressure pump, respectively. Both ventricles eject the same amount of blood to their respective peripheral circulation, but differ in intracavitary pressure, wall thickness, and shape. When coronary perfusion pressure is decre
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James W. Anderson PhDess in the left-ventricular wall may not be zero even if the intraventricular pressure is not present; such a stress is called the residual stress. The values of stresses must be obtained from the appropriate mathematial model, which should be as simple as possible. In the mathematical models propos
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James W. Anderson PhDal cells is defined as a tangential force produced by blood viscosity and a velocity gradient. There are many reports that endothelial cells respond to shear stress and change their morphology and functions. Blood flow characteristics have received special attention because atherogenesis is found ar
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James W. Anderson PhDes the nonlinearity of the stress—strain relationship and the existence of hysteresis. They also creep under constant stress and relax under constant strain. These mechanical properties have a structural basis. In Sec. 8.2 we consider the structure of the blood vessel wall. From Sec. 8.3 on, however
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James W. Anderson PhDes the nonlinearity of the stress—strain relationship and the existence of hysteresis. They also creep under constant stress and relax under constant strain. These mechanical properties have a structural basis. In Sec. 8.2 we consider the structure of the blood vessel wall. From Sec. 8.3 on, however
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The Basic Spaces,his book takes place. We define . and talk a bit about .. In order to aid our construction of a reasonable group of transformations of ℍ, we expand our horizons to consider the .., and close the chapter by considering how ℍ sits as a subset of ..
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,The General Möbius Group,ions, we spend this chapter by describing such a reasonable group of transformations of ℂ̅, namely the . Möb, which consists of compositions of . and . We close the chapter by restricting our attention to the transformations in Möb preserving ℍ.
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,Length and Distance in ℍ,o hyperbolic lines and preserve angles. In this chapter, we derive a means of measuring lengths of paths in ℍ which is invariant under the action of this group, expressed as an .. From this invariant element of arc-length, we construct an . on ℍ and explore some of its basic properties.
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