Alternative Equation Formats

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MathML

p o w e r = { Φ ( ( p 2 p 1 p 0 ) ( N w 1 w 2 ) 1 2 z 1 α [ ( w 1 p 1 + w 2 p 2 ) ( 1 w 1 p 1 w 2 p 2 ) ] 1 2 [ w 2 p 1 ( 1 p 1 ) + w 1 p 2 ( 1 p 2 ) ] 1 2 ) , upper one-sided Φ ( ( p 2 p 1 p 0 ) ( N w 1 w 2 ) 1 2 z 1 α [ ( w 1 p 1 + w 2 p 2 ) ( 1 w 1 p 1 w 2 p 2 ) ] 1 2 [ w 2 p 1 ( 1 p 1 ) + w 1 p 2 ( 1 p 2 ) ] 1 2 ) , lower one-sided Φ ( ( p 2 p 1 p 0 ) ( N w 1 w 2 ) 1 2 z 1 α 2 [ ( w 1 p 1 + w 2 p 2 ) ( 1 w 1 p 1 w 2 p 2 ) ] 1 2 [ w 2 p 1 ( 1 p 1 ) + w 1 p 2 ( 1 p 2 ) ] 1 2 ) + Φ ( ( p 2 p 1 p 0 ) ( N w 1 w 2 ) 1 2 z 1 α 2 [ ( w 1 p 1 + w 2 p 2 ) ( 1 w 1 p 1 w 2 p 2 ) ] 1 2 [ w 2 p 1 ( 1 p 1 ) + w 1 p 2 ( 1 p 2 ) ] 1 2 ) , two-sided

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Math as LaTeX Source

\[ \mr{power} = \left\{ \begin{array}{ll} \Phi \left( \frac{(p_2 - p_1 - p_0) (N w_1 w_2)^\frac {1}{2} - z_{1-\alpha } \left[ (w_1 p_1 + w_2 p_2) (1 - w_1 p_1 - w_2 p_2) \right]^\frac {1}{2}}{\left[ w_2 p_1 (1 - p_1) + w_1 p_2 (1 - p_2) \right]^\frac {1}{2}} \right), & \mbox{upper one-sided} \\ \Phi \left( \frac{-(p_2 - p_1 - p_0) (N w_1 w_2)^\frac {1}{2} - z_{1-\alpha } \left[ (w_1 p_1 + w_2 p_2) (1 - w_1 p_1 - w_2 p_2) \right]^\frac {1}{2}}{\left[ w_2 p_1 (1 - p_1) + w_1 p_2 (1 - p_2) \right]^\frac {1}{2}} \right), & \mbox{lower one-sided} \\ \Phi \left( \frac{(p_2 - p_1 - p_0) (N w_1 w_2)^\frac {1}{2} - z_{1-\frac{\alpha }{2}} \left[ (w_1 p_1 + w_2 p_2) (1 - w_1 p_1 - w_2 p_2) \right]^\frac {1}{2}}{\left[ w_2 p_1 (1 - p_1) + w_1 p_2 (1 - p_2) \right]^\frac {1}{2}} \right) + \\ \quad \Phi \left( \frac{-(p_2 - p_1 - p_0) (N w_1 w_2)^\frac {1}{2} - z_{1-\frac{\alpha }{2}} \left[ (w_1 p_1 + w_2 p_2) (1 - w_1 p_1 - w_2 p_2) \right]^\frac {1}{2}}{\left[ w_2 p_1 (1 - p_1) + w_1 p_2 (1 - p_2) \right]^\frac {1}{2}} \right), & \mbox{two-sided} \\ \end{array} \right. \]