Read e-book online Science avec conscience PDF

By Edgar Morin

ISBN-10: 2020120887

ISBN-13: 9782020120883

Les sciences humaines n'ont pas moral sense des caractères physiques et biologiques des phénomènes humains. Les sciences naturelles n'ont pas moral sense de leur inscription dans une tradition, une société, une histoire. Les sciences n'ont pas judgment of right and wrong de leur rôle dans l. a. société. Les sciences n'ont pas moral sense qui leur manque une sense of right and wrong. Mais de partout naît le besoin d'une technology avec moral sense. Il est temps de prendre sense of right and wrong de l. a. complexité de toute réalité -physique, biologique, humaine, sociale, politique -et de los angeles réalité de los angeles complexité. Il est temps de prendre moral sense qu'une technology privée de réflexion et qu'une philosophie purement spéculative sont insuffisantes. sense of right and wrong sans technology et technological know-how sans sense of right and wrong sont mutilées et mutilantes.

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The discrete system that arises from this mimetic FDM is of the same form as (20). The only difference at the discrete level is that the entries in B and g are computed using the m(·, ·) inner-product instead of the L2 inner-product (u, λ −1 v) on H div (Ω ). Thus, for the mimetic FDM we have gkl = m(ρΞ , ψkl ) , where Ξ = ∑i j ξi j ψi j and ξi j = 1 |γi j | γi j bi j,kl = m(ψi j , ψkl ) , G · ni j ds. 22 J. E. –A. Lie, V. Kippe, S. Krogstad Fig. 7. Examples of deformed and degenerate hexahedral cells arising in corner-point grid models.

Sci. , 19(5):1717–1736, 1998. 8. T. Arbogast. Numerical subgrid upscaling of two-phase flow in porous media. In Z. Chen, R. E. -C. , pages 35–49. Springer-Verlag, Berlin, 2000. 9. T. Arbogast. Analysis of a two-scale, locally conservative subgrid upscaling for elliptic problems. SIAM J. Numer. , 42(2):576–598, 2004. 10. K. Aziz and A. Settari. Petroleum reservoir simulation. Elsevier, London and New York, 1979. 11. I. Babu˘ska, G. Caloz, and E. Osborn. Special finite element methods for a class of second order elliptic problems with rough coefficients.

The MsFEM was first introduced by Hou and Wu [33], but the basic idea goes back to earlier work by Babu˘ska and Osborn [12] for 1D problems and Babu˘ska, Caloz, and Osborn [11] for special 2D problems. The method is, like standard FEMs, based on a variational formulation. In the variational formulation of (27) we seek p ∈ H01 (Ω ) such that a(p, v) = ( f , v) for all v ∈ H01 (Ω ), where (·, ·) is the L2 inner-product and a(p, v) = Ω K(x)u (x)v (x) dx. (28) 30 J. E. –A. Lie, V. Kippe, S. Krogstad Now, let NB = {0 = x0 < x1 < .

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Science avec conscience by Edgar Morin


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