Alternative Equation Formats

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MathML

nhi′=(nhi1,nhi2,…,nhiC)(1×C)nh′=(nh1′,nh2′,…,nhR′)(1×RC)phi⋅=nhi⋅ / nh(1×1)ph⋅j=nh⋅j / nh(1×1)Ph∗⋅′=(ph1⋅,ph2⋅,…,phR⋅)(1×R)Ph⋅∗′=(ph⋅1,ph⋅2,…,ph⋅C)(1×C)

MathML rendered with MathJax

nhi′=(nhi1,nhi2,…,nhiC)(1×C)nh′=(nh1′,nh2′,…,nhR′)(1×RC)phi⋅=nhi⋅ / nh(1×1)ph⋅j=nh⋅j / nh(1×1)Ph∗⋅′=(ph1⋅,ph2⋅,…,phR⋅)(1×R)Ph⋅∗′=(ph⋅1,ph⋅2,…,ph⋅C)(1×C)

Math as LaTeX Source

\[ \begin{array}{lllll} \mb{n}_{hi}^{\prime } & = & (n_{hi1},n_{hi2},\ldots ,n_{hiC}) & & (1 \times C) \\[0.10in] \mb{n}_ h^{\prime } & = & (\mb{n}_{h1}^{\prime },\mb{n}_{h2}^{\prime },\ldots , \mb{n}_{hR}^{\prime }) & & (1 \times RC) \\[0.10in] p_{hi \cdot } & = & n_{hi \cdot } ~ / ~ n_ h & & (1 \times 1) \\[0.10in] p_{h \cdot j} & = & n_{h \cdot j} ~ / ~ n_ h & & (1 \times 1) \\[0.10in] \mb{P}_{h* \cdot }^{\prime } & = & (p_{h1 \cdot },p_{h2 \cdot }, \ldots ,p_{hR \cdot }) & & (1 \times R) \\[0.10in] \mb{P}_{h \cdot *}^{\prime } & = & (p_{h \cdot 1},p_{h \cdot 2}, \ldots ,p_{h \cdot C}) & & (1 \times C) \\ \end{array} \]