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and we define a subspace of as (2.6).
Now, we define a subspace of E T as follows: E ˜ T = { x ∈ E T ∣ x n is odd in n }.
From now on, we fix (alpha in 0,1)), and define a subspace of (C(A_{q,a}^)) by _{0}E_{a}^{alpha}= bigl{ yinmathcal{A}C bigl(A_{q,a}^bigr) : ^{mathrm {c}}D_{q,0^^{alpha }y in Cbigl(A_{q,a}^bigr) bigr}, and the space of variations (^{mathrm{c}}operatorname{Var}(0,a)) for the Caputo q-derivative by ^{mathrm{c}}operatorname{Var}(0,a)= bigl{ hin_{0}E_{a}^{alpha } : h(0)=h(a)=0 bigr}.
In order to define a subspace of R m we sought unit vectors vα.
Define a subspace of E P as follows: E ˜ P = { x n ∈ E P ∣ x n is odd in n }.
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While MFA defines a subspace of steady state flux distributions then EFMA restricts this subspace by taking into account of irreversibility of certain reactions.
We define a subspace H of L 2 as follows: H = { u ∈ L 2 | ∑ | λ k ( λ k − c ) | h k 2 < ∞ }.
Let us denote an element v, in E ′, as v = ∑ h m n ϕ m n, and we define a subspace E of E ′ as E = { v ∈ E ′ | ∑ | λ m n | h m n 2 < ∞ }.
We define a subspace W of (L^{2}(S^{1},R)) as follows: W=Bigl{ xin L^{2}bigl(S^{1},Rbigr bigm| sum vert mu_{k}vert h_{k}^{2}< inftyBigr}.
For practical use of the RKM method, it is necessary to define a closed subspace of (Pi_{w}^{m}[a,b]) by imposing required homogeneous boundary conditions on it.
For given positive integer is defined as a subspace of by (2.4).
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Since I tried Ludwig back in 2017, I have been constantly using it in both editing and translation. Ever since, I suggest it to my translators at ProSciEditing.

Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com