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It is a singular point which holds potentially the rainwater.
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It is easy to see that x j is a singular point and we need to deal with it piecewisely.
Moreover, special attention is paid to the construction of propeller blades with a well-defined tangent plane at the tip, which is a singular point of the blade boundary surfaces.
This means that if x j ≠ 0 is a singular point of ν, so is g x j for each g ∈ G, and the mass of ν concentrated at g x j is the same for each g ∈ G.
If there is a singular point with only bound states, the leading term is (text {O}(t^{-1})) but when there are resonances there is only a bound by (text {O}(1/log t)).
It is clear that (lambda_{jn}=ialpha_{n} omega_{j}-omega)^{-1} omega_{j}-omegalar point of (f(x,lambda)) for any (j=1,2,ldots,m), (omega _{j}neqomega), (nin mathbb{N}).
Let x j be a singular point of the measures μ and ν.
Let x j ≠ 0 be a singular point of measures ς and ν.
Now, let x i be a singular point of the measures σ and ν.
for all ∈ Ω 2 and, thus, (52) is necessary and sufficient for to be a singular point of Φ m.
From the field distributions in Figure 4, each corner of the grating was a singular point of field and these scatting points became the sources of surface wave, as Figure 6 shown.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com