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This equation is reproduced below [27].
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The complete set of equations is reproduced in Additional file 1.
In this paper, Lame equations are reproduced in terms of vessel outer and material cross-sectional areas and presented in a very simple format that enables hoop stress calculation without use of any approximation.
Considering the general SSLMS algorithm given in Equation 14 which is reproduced here for convenience: boldsymbol{hat{x}}[k] = boldsymbol{bar{x}}[k] + mu|boldsymbol{varepsilon}[k]|^{2L-2}boldsymbol{G}boldsymbol{C}^{T}[k]boldsymbol{varepsilon}[k] (16).
This latter property is reproduced by the scaling parameter S of the first equation of System (1) reported in Methods.
Mr. Lichtman's response is reproduced below.
The statement is reproduced in full below.
It is reproduced in full below.
The critical paragraph is reproduced below.
It is reproduced in its entirety below.
His equation may be reproduced using (1a)–(1c) as begin{array}{*{20}l} &frac{partial}{partial t^ underbrace{left(frac{p^ u^{{c^^{2}}-frac{{q^^{2}}{2beta^ right)}_{sf IB pseudomomentum} + nabla^cdot underbrace{ langle!langle E^-v^v^, v^ u^ rangle!rangle }_{sf IB flux} = 0, end{array} (27a).
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