By C. M. Rodkiewicz (eds.)

ISBN-10: 3211816356

ISBN-13: 9783211816356

ISBN-10: 370914342X

ISBN-13: 9783709143421

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Indeed, this validity can be observed using data from HARKNESS (1971), who studied the variations of viscosity of serum and of albumin, globulin and fibrinogen solutions. 20) with dif- [n]-values are shown in good agreement (Fig. 8). 17) with 2 ~ C~ 9 (gr/100 ml). 20) to more data, the importance of non-newtonian effects in blood rheology calls for studying now variations of a function of tion. y at constant ~ n r as , that is the subject of the next sec- D. Quemada 50 4. BLOOD AS A STRUCTURED (SHEAR THINNING) FLUID: (1) Effects of RBC Aggregation and Deformation .

4). No theoretical calculation of coefficients k. l exists and their determina- tion can be only carried out by data fitting (see later). 5) a + 1 D. Quemada 32 where '( is the Taylor's factor. With r as the drop interfacial tension, eq. 5) holds in the limit S =(~Fy a/r) << 1 , that is if particles undergo very small deformation. From eq. 5), Einstein's result is recovered with "rigid" particles suspension (ex » 1) , while gas bubble emulsion (ex<< 1) leads to k1 + 1 . 3. Viscosity of concentrated suspensions.

27a) P) 2 a -- 2 Eq. 5 a <1> + ... e. a= eff/<1> as expected. 7 were observed by PAPIR et KRIEGER (1970) for suspensions of monodisperse colloidal spheres. 61 ) calculated by Vand (1949) from hydrodynamic interactions between spheres. 4. Application to blood and RBC suspensions The models given above were extensively used to fit blood and RBC suspension data, obtained from artificially prepared samples*, since normal hematocrit is about 40 - 45 • As hematocrit is not the true volume concentration <1> , a difficulty arises for applying model equations to data.

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Arteries and Arterial Blood Flow by C. M. Rodkiewicz (eds.)


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