Металлообрабатывающий твердосплавный инструмент by В.С.Самойлов, Э.Ф.Эйхманс, В.А.Фальковский, А.Д.Локтев

By В.С.Самойлов, Э.Ф.Эйхманс, В.А.Фальковский, А.Д.Локтев

Металлообрабатывающий твердосплавный инструмент КНИГИ,ТЕХНИКА Название: Металлообрабатывающий твердосплавный инструментАвтор: В.С.Самойлов, Э.Ф.Эйхманс, В.А.Фальковский, А.Д.ЛоктевИздательство: МашиностроениеГод: 1988Страниц: 368Формат: djvuРазмер: 5.2 МбКачество: нормальное Приведены сведения об основных видах металлообрабатывающего твердосплавного инструмента. Большое внимание уделено инструменту с механическим креплением многогранных неперетачиваемых пластин, прогрессивным конструкциям инструмента, даны рекомендации по их применению. Рассмотрен инструмент из безвольфрамовых сплавов. Описаны современные методы обработки твердых сплавов и методы соединения твердого сплава со сталью.Для инженерно-технических работников машиностроительных предприятий. .com eighty five

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13) ^* ^ 0 0 0 0 that can be written in a closed form only if the aggregation kernel is independent from the internal coordinate; in fact, under this simplification hypothesis the equation becomes: J - 00 ( f \ ^ ^ 00 00 00 = ^ \ e \n{^-^'-,t)n{^'-,t)A^'A^-a,\en{^-t)\n{^'-t)A^'A^ . , (^ - ^' = u) is applied the set of equation for A: = 0, 1, and 2, becomes as follows: difir. 1 y dm. ^ dm. - = - T « o ^ o ; - ^ = 0; —2. , the evolution equation of each moment has a source term written in terms of known moments).

By using more quadrature nodes). , 2006). However, in bivariate problems it may be necessary to use A^ = 4 or 9 in order to capture all lower-order moments correctly (Fox, 2007). In any case, the total number of moment transport equations that must be solved is3N, and is much smaller than the number of degrees of freedoms required for a direct method. 32 Rodney O. Fox One-node closure Closure with A^ = 1 is usually not very accurate. However, it leads to simple-to-understand transport equations that will provide insight into why higher-order closures are needed.

R. Aris (1962). Vectors, Tensors, and the Basic Equations of Fluid Mechanics. Prentice-Hall, Englewood Cliffs, USA. G. A. Bird (1994). Molecular gas dynamics and the direct simulation of gas flows. Oxford Science Publications, 42. R. B. Bird, W. E. Stewart, and E. N. Lightfoot (2002). Transport Phenomena. John Wiley & Sons, New York, USA, second edition. F. Bouchut (1994). On zero pressure gas dynamics. In Advances in Kinetic Theory and Computing, pages 171-190. World Scientific Publishing, River Edge, USA.

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