The line passes through the point \( \vec{A} = \vec{i} - 2\vec{j} \) and is parallel to the vector \( \vec{d} = 2\vec{i} + \vec{k} \). So, the parametric form of the line is: \[ \vec{r}(t) = (\vec{i} - 2\vec{j}) + t(2\vec{i} + \vec{k}) \Rightarrow \vec{r}(t) = (1 + 2t)\vec{i} - 2\vec{j} + t\vec{k} \] The plane passes through point \( \vec{B} = \vec{i} + 2\vec{j} \) and is parallel to the vectors: \[ \vec{v}_1 = 2\vec{j} - \vec{k}, \vec{v}_2 = \vec{i} + 2\vec{k} \] So, any point on the plane can be written as: \[ \vec{r}(u,v) = \vec{i} + 2\vec{j} + u(2\vec{j} - \vec{k}) + v(\vec{i} + 2\vec{k}) \] To find the intersection of the line and the plane, equate both expressions: \[ (1 + 2t)\vec{i} - 2\vec{j} + t\vec{k} = \vec{i} + 2\vec{j} + u(2\vec{j} - \vec{k}) + v(\vec{i} + 2\vec{k}) \] Equating components:

Substituting (i) and (ii) into (iii): \[ t = -(-2) + 2(2t) \Rightarrow t = 2 + 4t \Rightarrow -3t = 2 \Rightarrow t = -\frac{2}{3} \] Now substitute \( t = -\frac{2}{3} \) into the line equation: \[ \vec{r} = (1 + 2t)\vec{i} - 2\vec{j} + t\vec{k} = \left(1 - \frac{4}{3}\right)\vec{i} - 2\vec{j} - \frac{2}{3}\vec{k} = -\frac{1}{3}\vec{i} - 2\vec{j} - \frac{2}{3}\vec{k} \] Multiply by -1: \[ \vec{r} = \frac{1}{3} (\vec{i} + 6\vec{j} + 2\vec{k}) \]
| List-I | List-II | ||
|---|---|---|---|
| (A) | $f(x) = \frac{|x+2|}{x+2} , x \ne -2 $ | (I) | $[\frac{1}{3} , 1 ]$ |
| (B) | $(x)=|[x]|,x \in [R$ | (II) | Z |
| (C) | $h(x) = |x - [x]| , x \in [R$ | (III) | W |
| (D) | $f(x) = \frac{1}{2 - \sin 3x} , x \in [R$ | (IV) | [0, 1) |
| (V) | { -1, 1} | ||
| List I | List II | ||
|---|---|---|---|
| (A) | $\lambda=8, \mu \neq 15$ | 1. | Infinitely many solutions |
| (B) | $\lambda \neq 8, \mu \in R$ | 2. | No solution |
| (C) | $\lambda=8, \mu=15$ | 3. | Unique solution |
Let ABCD be a parallelogram and $ 2\bar{i} + \bar{j} $, $ 4\bar{i} + 5\bar{j} + 4\bar{k} $ and $ -\bar{i} - 4\bar{j} - 3\bar{k} $ be the position vectors of the vertices A, B, D respectively. Then the position vector of one of the points of trisection of the diagonal AC is