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Without expanding show that: `=|cos e c^2thetacot^2theta1cot^2thetacos e c^2theta-1 42 40 2|=0`

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Applying `C_{1} \rightarrow C_{1}-C_{2}-C_{3}`, we have $$ \Delta=\left|\begin{array}{ccc} \operatorname{cosec}^{2} \theta-\cot ^{2} \theta-1 & \cot ^{2} \theta & 1 \\ \cot ^{2} \theta-\operatorname{cosec}^{2} \theta+1 & \operatorname{cosec}^{2} \theta & -1 \\ 0 & 40 & 2 \end{array}\right|=\left|\begin{array}{ccc} 0 & \cot ^{2} \theta & 1 \\ ...
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