... It is sometimes called the `thermoelectric figure-of-merit,' although this name is more often given to the dimensionless combination ZT sS 2 T X K In the above formulas, s, S, and K are respectively the material electrical conductivity, thermopower (Seebeck coefficient), and thermal conductivity, and T is the operating temperature or the average temperature T1 T2 a2 of the converter, with T1 and T2 being the respective cold and hot end temperatures. ... We first consider the thermal conductivity. ...

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... In Chap. ... sign cos : By the theorem on the motion of the center of masses in the space in projections to the related axes .x ; y ; z/ and the theorem on the change of the kinematic moment with respect to these axes, we obtain the following complete system of differential equations in the dynamical quasi-velocity space R1 fvg S2 f; g C R3 fx ;y ;z g: v cos P v sin C y v sin sin P 2 2 z v sin cos C .y C z / D Fx =m; v sin cos C v cos ... I2 n0 d cos with variable coefficient....

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• http://shamolin2.imec.msu.ru/shamolin.pdf

... The SHG enhancement is attributed to the combined effects of the spatial localization of the fundamental field in the MC spacer and the fulfillment of the phase-matching conditions. ... AlGaAs,14 AlAs/AlGaAs,15 and ZnS/SrF2 (Ref. 16) layers, or alternating layers of porous silicon (PS) with different porosities.17,18 Several approaches are used for the calculation of SHG enhancement at the PBG edges of photonic crystals. ... For SHG enhancement at the PBG edge phase matching is even more important. ...

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• http://shg.phys.msu.ru/ruscon/articles/pdf/03_JMMM_258_96.pdf
• http://shg.phys.msu.ru/ruscon/articles/pdf/04_JAP95_7330.pdf

... The model was then employed to assess the dependence of the association rate constant on the dimensions of the lumen. ... This small (10.5 kDa) protein diffuses in the lumen, a relatively narrow closed space between the thylakoid membranes, oxidizing cytochrome f (Cyt f ) in the membrane complex and then reducing the PS I reaction center. ... However, these works did not consider the diffusion of Pc molecules in the thylakoid lumen or their interaction with the b6 f and PS I membrane-bound complexes...

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• МОДЕЛИРОВАНИЕ БИОМЕХАНИЧЕСКИХ ПРОЦЕССОВ

Introduction to PLASMA ASTROPHYSICS (Selected 10 lectures) Boris V. Somov Astronomical Institute and Faculty of Physics Moscow State University Pushino-na-Oke, 2008 Contents Ab out These Lectures 1 Particles and Fields: Exact Self-Consistent Description 1.1 Liouville's theorem . . . . . . . . . . . . . . . . . . . 1.1.1 Continuity in phase space . . . . . . . . . 1.1.2 The character of particle interactions 1.1.3 The Lorentz force, gravity . . . . . . . . . 1.1.4 Collisional friction . . . . . . . . . . . .

232. Концессионный механизм как эффективное средство модернизации аэропортовой

233. http://mailybaev.imec.msu.ru/papers/Mailybaev1999b.pdf

234. http://ecology.genebee.msu.ru/3_SOTR/CV_Terekhin_publ/2003_Envir_human_EER.pdf

235. http://www-hep.sinp.msu.ru/hep/open_docs/lehep_2010.doc