A two-step method is proposed for solving this problem. At the first step, using the Dulac–Cherkas test, we find nested closed curves that have no common points and split the simply connected domain into doubly connected subdomains, with each curve being transversal to the vector field of ...
Conformal transformation of the circles through the origin in the (x, y)-plane (left) into lines in the (u, v)-plane (right) Full size image 5.1.2 Hough Transform The Hough transform [2] is a technique that finds clusters of points that lie on or close to a parametric curve such ...
Let $P$ be a polygonal curve in $\mathbb{R}^D$ of length $n$, and $S$ be a point set of size $k$. The Curve/Point Set Matching problem consists of finding a polygonal curve $Q$ on $S$ such that its Fr\'echet distance from $P$ is less than a given $\varep
the sEMD’s preferred direction velocity tuning curve is similar but peaks at 5 Hz. This suggests that the reported parameter set of the sEMD tunes it to slightly higher relative velocities. The model performs in a robust way for a wide range of illuminations (from 5 lux to 5000 lux)...
Find the length of the curve e^t \sin t\vec i - e^t\vec j + e^t \cos t\vec k from t = 0 to t = 1. Find \frac{d}{dx} [\int_0^{x^3} \sin t \,dt ] Find ds/dt for s = (1 - sin t ) / (2 +...
(habitable planets) per planetary system, fl = the fraction of habitable planets that develop primitive life, fi = the fraction of planets with life that evolve intelligent life and civilizations, fc = the fraction of civilizations that become ACCs, L = the length of time ...
This measurement reflects the usefulness of the module for a given a design goal. Using modules with high utility values should result in superior designs. We propose a heuristic which iteratively perturbs module utility values until they lead to good module selections. Our experiments show that ...
%a zero crossing area, so its the middlest value of the zero crossing area z = find(diff(sign(array))); a = 1; b = 1; fori=2:1:length(z) ifz(i) > z(i-1)+round((samplerate/10000))+1 a = 1; ifi == 2 zci(b,a) = z(i-1); ...
Self-shaping systems offer a promising approach for making complex 3D geometries from the material-driven transformation of 2D sheets. However, current res
We compare our results for P (k⊥) in weakly coupled quark-gluon plasma to expectations from holographic calculations that assume a plasma that is strongly coupled at all length scales. We find that the shape of P (k⊥) at modest k⊥ may not be very different in weakly coupled and ...