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Exact(11)
The positive solution of this equation is given by (32).
The solution of this equation is given by ψ ( z ) = C exp ( − λ + 1 μ z ).
Using Lagrange multiplier technique, the weight vector that solves this equation is given by: (10).
This equation is given by Q_{text{urb}} = P - {text{ETa}} - {text{GR}} - Q_{text{sur}} pm Delta S.
Assuming A p to be non-singular, the solution of this equation is given by: mathbf{X}_{o,l}= mathbf{A}_{p}^{-1}mathbf{B}_{p} (33).
Writing slowness p = N/V, such that row matrix N satisfies NN T = 1, this equation is given by (8) where, and matrix Z N = Z(N, N), as defined in Appendix.
Similar(48)
Typical values of the quantities in this equation are given in the table.
The units of the terms in this equation are given below, expressed first in the centimetre-gram-second (cgs) system and then in the International System of Units (SI) system, with the conversion factor from the first to the second given between them.
Thus, The units of the terms in this equation are given below, expressed first in the centimetre-gram-second (cgs) system and then in the International System of Units (SI) system, with the conversion factor from the first to the second given between them.
The steps of the derivation of this equation are given below.
Applying the generalized Riccatitransformation, integral averaging technique of Philos type and Young'sinequality, a set of new criteria for oscillation or certain asymptoticbehavior of nonoscillatory solutions of this equations is given.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com