Titlebook: Methods of Local and Global Differential Geometry in General Relativity; Proceedings of the R D. Farnsworth,J. Fink,A. Thompson Conference

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书目名称Methods of Local and Global Differential Geometry in General Relativity影响因子(影响力)

书目名称Methods of Local and Global Differential Geometry in General Relativity影响因子(影响力)学科排名

书目名称Methods of Local and Global Differential Geometry in General Relativity网络公开度

书目名称Methods of Local and Global Differential Geometry in General Relativity网络公开度学科排名

书目名称Methods of Local and Global Differential Geometry in General Relativity被引频次

书目名称Methods of Local and Global Differential Geometry in General Relativity被引频次学科排名

书目名称Methods of Local and Global Differential Geometry in General Relativity年度引用

书目名称Methods of Local and Global Differential Geometry in General Relativity年度引用学科排名

书目名称Methods of Local and Global Differential Geometry in General Relativity读者反馈

书目名称Methods of Local and Global Differential Geometry in General Relativity读者反馈学科排名

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A. P. Stonesed D-flip flop has a 23% decrease in cell count, a 50% decrease in area, a 40% decrease in latency when compared to the existing circuits. Further, there is a 27% decrease in cell count, 58% decrease in area, 17% decrease in latency in our design of edge-sensitive D-flip flop with asynchronous Set/

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M. Demianskiomfort and safety of the passengers in such vehicles are directly affected by the interaction between the subgrade and the slab. This article contains the dynamic analysis of a three-dimensional, modal bong graph model of the components of the high-speed track. In this paper, the concrete slab has b

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Lane P. Hughstonusing the data to identify the portion of flow through vegetation occupied by wakes. For this, a straightforward criterion, related to the incident flow conditions and generated vorticity, is proposed. Further refinements of this research can lead to applications in several branches of fluid mechani

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Pt. I. H. Dwivedi,R. Kantowskishow that electroviscous correction factor Y (ratio of apparent to physical viscosity) increases for no-slip (B. = 0) flow as surface charge density (S) varies from 4 to 16 at fixed K. It has been further observed that the surface charge-dependent slip at the walls plays a vital role on the hydrodyn

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Titlebook: Methods of Local and Global Differential Geometry in General Relativity; Proceedings of the R D. Farnsworth,J. Fink,A. Thompson Conference

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