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Exact(25)
Multiply the first equation of (1.4) by for and integrate by parts over to obtain (4.19).
We use to multiply the first equation in the system (4.9) and then integrate over.
We merely multiply the first equation of (33) by and integrate by parts over.
Multiply the first equation of u in (1.1) by (u^{p-1}) and integrate on Ω by parts.
Multiply the first equation of (2) by (v in H_{0}^{1}(0,T)), integrate it on the interval ([0,T]).
If we multiply the first equation by 2 and the second equation by x and combine these equations we have frac{3}{x}u_{2}^{prime}(x)=x biggl( lambda+ frac{2}{x}-q ( x ) biggr) y(x).
Similar(35)
Multiply the second equation of (2.10) by and integrate over.
Multiply the second equation of (1.4) by and integrate it over to obtain (4.15).
Therefore, to hold on the uniformity of vectors z and x, we need to multiply the second term by s.
For nonzero frequencies we may multiply the second block row by ω − 1 and introduce the new variable v ˆ = ω − 1 p ˆ.
Next, you'll multiply the second column before the break by the second column after the break.
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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