Alternative Equation Formats

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MathML

\begin{array}{rcl} q_{1} (y_{1, t}, y_{2, t}, \dots, y_{g, t}, x_{1, t}, x_{2, t}, \dots, x_{m, t}, θ_{1}, θ_{2}, \dots, θ_{p}) & = ϵ_{1, t} \\ q_{2} (y_{1, t}, y_{2, t}, \dots, y_{g, t}, x_{1, t}, x_{2, t}, \dots, x_{m, t}, θ_{1}, θ_{2}, \dots, θ_{p}) & = ϵ_{2, t} \\ ⋮ \\ q_{g} (y_{1, t}, y_{2, t}, \dots, y_{g, t}, x_{1, t}, x_{2, t}, \dots, x_{m, t}, θ_{1}, θ_{2}, \dots, θ_{p}) & = ϵ_{g, t} \end{array}

MathML rendered with MathJax

\begin{array}{rcl} q_{1} (y_{1, t}, y_{2, t}, \dots, y_{g, t}, x_{1, t}, x_{2, t}, \dots, x_{m, t}, θ_{1}, θ_{2}, \dots, θ_{p}) & = ϵ_{1, t} \\ q_{2} (y_{1, t}, y_{2, t}, \dots, y_{g, t}, x_{1, t}, x_{2, t}, \dots, x_{m, t}, θ_{1}, θ_{2}, \dots, θ_{p}) & = ϵ_{2, t} \\ ⋮ \\ q_{g} (y_{1, t}, y_{2, t}, \dots, y_{g, t}, x_{1, t}, x_{2, t}, \dots, x_{m, t}, θ_{1}, θ_{2}, \dots, θ_{p}) & = ϵ_{g, t} \end{array}

Math as LaTeX Source

\begin{eqnarray*} & q_{1}( y_{1,t}, y_{2,t}, \ldots , y_{g,t}, x_{1,t}, x_{2,t}, \ldots , x_{m,t}, {\theta }_{1}, {\theta }_{2}, \ldots , {\theta }_{p})& = {\epsilon }_{1,t} \\ & q_{2}( y_{1,t}, y_{2,t}, \ldots , y_{g,t}, x_{1,t}, x_{2,t}, \ldots , x_{m,t}, {\theta }_{1}, {\theta }_{2}, \ldots , {\theta }_{p})& = {\epsilon }_{2,t} \\ & {\vdots }& \\ & q_{g}( y_{1,t}, y_{2,t}, \ldots , y_{g,t}, x_{1,t}, x_{2,t}, \ldots , x_{m,t}, {\theta }_{1}, {\theta }_{2}, \ldots , {\theta }_{p})& = {\epsilon }_{g,t} \end{eqnarray*}