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Titlebook: Simulation in CIM; Manfred Weck (Leiter des Lehrstuhles für Werkzeugm Book 1991 Verlag TüV Rheinland GmbH, K?ln 1991 Anforderungen.Blechum

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31#
發(fā)表于 2025-3-26 22:24:30 | 只看該作者
Halftone Image Reconstruction Based on SLIC Superpixel Algorithmined by the linear smoothing filter and nonlinear smoothing filters. Finally, the vectored boundary and smooth background are combined together to get the reconstructed image. The boundary information is effectively retained during the reconstruction. The proposed method can effectively remove the halftone patterns and screen patterns.
32#
發(fā)表于 2025-3-27 03:19:17 | 只看該作者
Conclusion: Kingdoms of Romance in , and , narratives” that Fredric Jameson (1981) half welcomes as “a place of heterogeneity and of freedom from that reality principle to which a now oppressive realistic representation is the hostage,” even though they themselves may be hostage to the capitalist marketplace.
33#
發(fā)表于 2025-3-27 07:43:44 | 只看該作者
Christin Emrichends regularity properties of the cycle structure for general ., yielding tight bounds for the transposition distance of lonely permutations. The subset of lonely permutations that are 3-permutations is characterized and consequently an upper bound is obtained for their transposition distances.
34#
發(fā)表于 2025-3-27 09:38:16 | 只看該作者
Ulrich Natke,Anke Kohm?scherdere) und für die ?notorious obscurity of Chinese bookkeeping methods“.. Gemeinsame Herkunft, eigene Sprache und besondere Schrift (die etwa auf Lückenfüllung angelegt ist, z. B. wenn Vokale fehlen) schaffen ein für Au?enseiter undurchdringliches ?Dickicht“, weshalb wir Westler von chinesischen ?Geh
35#
發(fā)表于 2025-3-27 14:04:04 | 只看該作者
36#
發(fā)表于 2025-3-27 18:05:33 | 只看該作者
37#
發(fā)表于 2025-3-27 22:03:26 | 只看該作者
38#
發(fā)表于 2025-3-28 04:00:29 | 只看該作者
39#
發(fā)表于 2025-3-28 08:41:34 | 只看該作者
Vorticity generation in a nonpremixed flame sheet,ion included. The initial flame is straight and passes through the vortex core, but not through the center of the vortex as in Marble‘s work. During the first eddy turn-over time, the swirling flow forms a flame tip region, and the amount of tip rotation around the vortex depends on the diffusion co
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