scholarly journals Alternating knots with large boundary slope diameter

Author(s):  
Masaharu Ishikawa ◽  
Thomas Mattman ◽  
Kazuya Namiki ◽  
Koya Shimokawa
Keyword(s):  
2009 ◽  
Vol 18 (12) ◽  
pp. 1623-1636
Author(s):  
SRIKANTH KUPPUM ◽  
XINGRU ZHANG

We found a family of infinitely many hyperbolic knot manifolds each member of which has a strongly detected boundary slope with associated root of unity of order 4.


Author(s):  
Cunfu Wang ◽  
Xiaoping Qian ◽  
William D. Gerstler ◽  
Jeff Shubrooks

This paper studies how to control boundary slope of optimized parts in density-based topology optimization for additive manufacturing (AM). Boundary slope of a part affects the amount of support structure required during its fabrication by additive processes. Boundary slope also has a direct relation with the resulting surface roughness from the AM processes, which in turn affects the heat transfer efficiency. By constraining the minimal boundary slope, support structures can be eliminated or reduced for AM, and thus, material and postprocessing costs are reduced; by constraining the maximal boundary slope, high-surface roughness can be attained, and thus, the heat transfer efficiency is increased. In this paper, the boundary slope is controlled through a constraint between the density gradient and the given build direction. This allows us to explicitly control the boundary slope through density gradient in the density-based topology optimization approach. We control the boundary slope through two single global constraints. An adaptive scheme is also proposed to select the thresholds of these two boundary slope constraints. Numerical examples of linear elastic problem, heat conduction problem, and thermoelastic problems demonstrate the effectiveness and efficiency of the proposed formulation in controlling boundary slopes for additive manufacturing. Experimental results from metal 3D printed parts confirm that our boundary slope-based formulation is effective for controlling part self-support during printing and for affecting surface roughness of the printed parts.


2013 ◽  
Vol 52 (9S1) ◽  
pp. 09KD11 ◽  
Author(s):  
Tomoaki Karaki ◽  
Tsunehiro Katayama ◽  
Kazuhiro Yoshida ◽  
Subaru Maruyama ◽  
Masatoshi Adachi

2004 ◽  
Vol 13 (05) ◽  
pp. 587-596
Author(s):  
ANNEKE BART

Given a Bianchi Group [Formula: see text], and a Hyperbolic manifold M, where π1(M) is of finite index in Γd, we show that all boundary slopes are realized as the boundary slope of an immersed totally geodesic surface and hence are virtually embedded boundary slopes.


1966 ◽  
Vol 70 (666) ◽  
pp. 676-676 ◽  
Author(s):  
J. C. Gibbings

The note by W. T. F. Lau upon the effective “length” of two-dimensional contracting ducts has raised further points of interest.Lau's paper presents three different criteria which can control a contraction length. Of these three, the second and third, that respectively are based upon the approach of the centre-line velocity to its asymptotic value and upon the approach of the flow to uniformity, were compared in ref. 1. The first criterion that is based upon the approach of the boundary slope to zero is not in general identical with the second.


2017 ◽  
Vol 833 ◽  
pp. 70-97 ◽  
Author(s):  
M. E. Negretti ◽  
J.-B. Flòr ◽  
E. J. Hopfinger

Gravity currents often occur on complex topographies and are therefore subject to spatial development. We present experimental results on continuously supplied gravity currents moving from a horizontal to a sloping boundary, which is either concave or straight. The change in boundary slope and the consequent acceleration give rise to a transition from a stable subcritical current with a large Richardson number to a Kelvin–Helmholtz (KH) unstable current. It is shown here that depending on the overall acceleration parameter$\overline{T_{a}}$, expressing the rate of velocity increase, the currents can adjust gradually to the slope conditions (small$\overline{T_{a}}$) or go through acceleration–deceleration cycles (large$\overline{T_{a}}$). In the latter case, the KH billows at the interface have a strong effect on the flow dynamics, and are observed to cause boundary layer separation. Comparison of currents on concave and straight slopes reveals that the downhill deceleration on concave slopes has no qualitative influence, i.e. the dynamics is entirely dominated by the initial acceleration and ensuing KH billows. Following the similarity theory of Turner 1973 (Buoyancy Effects in Fluids. Cambridge University Press), we derive a general equation for the depth-integrated velocity that exhibits all driving and retarding forces. Comparison of this equation with the experimental velocity data shows that when$\overline{T_{a}}$is large, bottom friction and entrainment are large in the region of appearance of KH billows. The large bottom friction is confirmed by the measured high Reynolds stresses in these regions. The head velocity does not exhibit the same behaviour as the layer velocity. It gradually approaches an equilibrium state even when the acceleration parameter of the layer is large.


1996 ◽  
Vol 26 (8) ◽  
pp. 1468-1479 ◽  
Author(s):  
Atsushi Kubokawa ◽  
James C. McWilliams

1966 ◽  
Vol 70 (666) ◽  
pp. 673-675 ◽  
Author(s):  
W. T. F. Lau

In a recent paper, Gibbings has made an interesting comparison of the length of two-dimensional contractions based on three criteria, namely:(1)the rapidity with which the boundary slope approaches its zero value;(2)the rapidity with which the centre-line velocity approaches its asymptotic value; and(3)the degree of uniformity of the velocity expressed as a percentage of its mean value.


Energy ◽  
2017 ◽  
Vol 119 ◽  
pp. 211-217 ◽  
Author(s):  
Wen Su ◽  
Li Zhao ◽  
Shuai Deng

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