Titlebook: Geometry of Surfaces; John Stillwell Textbook 1992 Springer Science+Business Media New York 1992 Area.Fractal.curvature.differential geome

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書目名稱Geometry of Surfaces影響因子(影響力)




書目名稱Geometry of Surfaces影響因子(影響力)學(xué)科排名




書目名稱Geometry of Surfaces網(wǎng)絡(luò)公開度




書目名稱Geometry of Surfaces網(wǎng)絡(luò)公開度學(xué)科排名




書目名稱Geometry of Surfaces被引頻次




書目名稱Geometry of Surfaces被引頻次學(xué)科排名




書目名稱Geometry of Surfaces年度引用




書目名稱Geometry of Surfaces年度引用學(xué)科排名




書目名稱Geometry of Surfaces讀者反饋




書目名稱Geometry of Surfaces讀者反饋學(xué)科排名

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隱士

Injunction

Von der Zerlegung der Zahlen in Teile,s intended to model “flat” surfaces in the real world; yet all physical flat surfaces are of finite extent and have boundaries. It is not clear that such a surface would resemble ?. when extended indefinitely, even if small parts of it matched small parts of ?. with absolute precision. Indeed, we ma

牢騷

適宜

Di- und triklinometrisches System,t . ? ., more than one line through . which does not meet . Such a surface departs from the euclidean plane in the opposite way to the sphere, and the hyperbolic plane, in fact, emerged from the study of surfaces which “curve” in the opposite way to the sphere. The train of thought, in brief, was th

適宜

,Die Gr??enordnung der Kardinalzahlen, function . such that each . ∈ . has an ε-neighborhood isometric to a disc of ?.. The proof of the Killing-Hopf theorem (Section 2.9) carries over word-for-word (provided “l(fā)ine”, “distance” etc., are understood in the hyperbolic sense), showing that any complete, connected hyperbolic surface is of t

Fallibility

Besondere Behandlung des Falles , = 3, problem of classifying groups Γ. In the spherical and euclidean cases this problem is easy to solve, as we have seen in Chapters 2 and 3, because there are only a small number of possibilities. However, in the hyperbolic case the number of possibilities is infinite, and the problem is best clarifie

有毛就脫毛

污點

Einleitung in die griechische Philologie sides of II according to the side pairing, is also an orbit space .Γ. Here . = . is S., ?., or ?.—the surface from which II originates—and Γ is the group generated by the side-pairing transformations of II. Because of its interpretation as an orbit space, . is also called an