- Timestamp:
- 2018-02-28T14:39:33+01:00 (6 years ago)
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branches/2017/dev_merge_2017/DOC/TexFiles/Chapters/Annex_ISO.tex
r9364 r9365 392 392 \quad {b_T}_{i+i_p+1/2}^k\left(\frac{\partial T}{\partial 393 393 t}T\right)_{i+i_p+1/2}^k \\ 394 \begin{ split}394 \begin{aligned} 395 395 &= -T_{i+i_p-1/2}^k{\;} _i^k{\mathbb{F}_u}_{i_p}^{k_p} (T) \quad + \quad T_{i+i_p+1/2}^k 396 396 {\;}_i^k{\mathbb{F}_u}_{i_p}^{k_p} (T) \\ 397 397 &={\;} _i^k{\mathbb{F}_u}_{i_p}^{k_p} (T)\,\delta_{i+ i_p}[T^k], \label{eq:triad:dvar_iso_i} 398 \end{ split}398 \end{aligned} 399 399 \end{multline} 400 400 while the vertical flux similarly drives a net rate of change of
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