If the latus rectum subtends a right angle at center of the hyperbola, then its eccentricity is
- $\frac{\sqrt{13}}{2}$
- $\frac{\sqrt{5}-1}{2}$
- $\frac{\sqrt{5}+1}{2}$
- $\frac{\sqrt{3}+1}{2}$
Solution

Centre = (0, 0) $ \because \quad \angle L C L^{\prime}=90^{\circ} $ Then, in $\Delta L C L^{\prime}$, by using Pythagoras theorem, $ \begin{aligned} (L C)^2+\left(L^{\prime} C\right)^2 & =\left(L L^{\prime}\right)^2 \\ (a e-0)^2 & +\left(\frac{b^2}{a}-0\right)^2+(a e-0)^2+\left(\frac{-b^2}{a}-0\right)^2 \\ & =\left(\frac{2 b^2}{a}\right)^2 \end{aligned} $ $ \begin{aligned} & 2\left(a^2 e^2+\frac{b^4}{a^2}\right)=\frac{4 b^4}{a^2} \Rightarrow \frac{2 b^4}{a^2}=2 a^2 e^2 \\ & \Rightarrow \quad b^4=a^4 e^2 \\ & {\left[a^2\left(e^2-1\right)\right]^2=a^4 e^2 \quad\left\{\because b^2=a^2\left(e^2-1\right)\right\}} \\ & a^4\left(e^2-1\right)^2=a^4 e^2 \\ & \Rightarrow \quad\left(e^2-1\right)^2=e^2 \Rightarrow e^2-1= \pm e \\ & \Rightarrow e^2 \pm e-1=0 \\ & \Rightarrow \quad e=\frac{ \pm 1 \pm \sqrt{1+4}}{2}=\frac{ \pm 1 \pm \sqrt{5}}{2} \\ & \end{aligned} $ $\because e$ can't be negative, hence $e=\frac{\sqrt{5}-1}{2}, \frac{\sqrt{5}+1}{2}$
Asked in: AP EAMCET 2021 (25 Aug Shift 2)