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Moreover, all critical points of I in (overline{B_{alpha}(mathcal{K})}) belong to (mathcal{K}).
end{aligned} It is clear that all critical points of (I_{lambda}) must lie on (N_{lambda}).
We aim to employ Theorem 2.2 on T, where all critical points of T are solutions to (5).
Furthermore, when the relative error is not too large, the algorithm can capture almost all critical points.
A computational study is performed to examine the stress distribution at all critical points, maximum reach, natural frequencies and the corresponding mode shapes.
However, it is extremely complicated to identify all critical points and, therefore, it is not clear whether a chosen ({bf k} -point grid contains critical points or not.
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Note that (T in C^{1}(mathcal{B}, mathbb{R})), (T 0)=0), and that all the critical points of T are the solutions of (5).
end{aligned}Note that (Theta in C^1(mathcal {B}, mathbb {R}),, Theta (0)=0) and that all the critical points of (Theta) are the solutions of (12).
In particular, at points where ∇ρ(r ) vanishes (like all the critical points of ρ(r ), CP's): G r C P = 3 10 3 π 2 2 / 3 ρ 5 / 3 r C P + 1 6 ∇ 2 ρ r C P (2).
Now, let η = S ˜ n 4, we can therefore assume that | ε | is so small that all the critical points at infinity of J ε of two masses or more are above the level S ˜ n + 3 η, and the critical points at infinity of one mass are below S ˜ n + η.
Therefore, the opportunity of HCV transmission will remain substantial without implementing new prevention strategies that target all these critical points.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com