Step 1: The direction ratios of the lines \( L_1 \) and \( L_2 \) can be extracted from their parametric equations. For \( L_1 \), the direction ratios are \( (1, -1, -1) \), and for \( L_2 \), the direction ratios are \( (1, 2, 2) \).
Step 2: The direction vector of the line \( L_3 \) is perpendicular to both \( L_1 \) and \( L_2 \), so we compute the cross product of the direction vectors of \( L_1 \) and \( L_2 \). \[ \mathbf{d_3} = \mathbf{d_1} \times \mathbf{d_2} \] After computing the cross product, we get the direction vector of \( L_3 \).
Step 3: The equation of the line \( L_3 \) is now known, and we substitute the parametric equations of \( L_3 \) into the plane equation \( 5x - 11y - 8z = 1 \) to find the value of \( 5x - 11y - 8z \). Thus, the final value of \( 5x - 11y - 8z \) is found.
If the domain of the function $ f(x) = \log_7(1 - \log_4(x^2 - 9x + 18)) $ is $ (\alpha, \beta) \cup (\gamma, \delta) $, then $ \alpha + \beta + \gamma + \delta $ is equal to
Let $ A = \{-2, -1, 0, 1, 2, 3\} $. Let $ R $ be a relation on $ A $ defined by $ (x, y) \in R $ if and only if $ |x| \le |y| $. Let $ m $ be the number of reflexive elements in $ R $ and $ n $ be the minimum number of elements required to be added in $ R $ to make it reflexive and symmetric relations, respectively. Then $ l + m + n $ is equal to
A conducting bar moves on two conducting rails as shown in the figure. A constant magnetic field \( B \) exists into the page. The bar starts to move from the vertex at time \( t = 0 \) with a constant velocity. If the induced EMF is \( E \propto t^n \), then the value of \( n \) is _____. 