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According to (3), the rotor motion equation of multi-machine power systems can be derived as below [20, 21].
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Consequently, the CSE of the core is derived as below, {mathrm{CSE}}_C r)=frac{ cosh left(frac{r}{L_C}right)}{ cosh left(frac{R_C}{L_C}right)}=frac{ cosh left(frac{r}{L_C}right)}{ cosh left({k}_Cright)},kern0.5em 0le r<{R}_C.
The wave vectors of P and S wave, ( l_{text{p}} ) and ( l_{text{S}} ), are derived as shown below.
The DRM was derived as described below.
This result is derived as follows.
Assuming that all the carriers diffuse along the radial direction, namely, minority-carrier diffusion in the vertical direction is negligible [17], the steady-state Eq. (1) can be then derived as below, {D}_hfrac{partial^2varDelta h(r)}{partial {r}^2}-frac{varDelta h}{tau_h}+{g}_h=0, (2).
These components can be derived from Young's equation as given below (2).
There were limitations as to what could be derived from the studies, which we discuss below.
G, Δ G, and I are not directly available but can be derived from CGM and subcutaneous insulin delivery as detailed below.
MSCs will be derived from the lipoharvest and isolated and expanded as detailed below.
Thus, the conservation of the LRL vector must be derived directly, e.g., by the method of Poisson brackets, as described below.
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