| List - I | List - II | ||
| (P) | γ equals | (1) | \(-\hat{i}-\hat{j}+\hat{k}\) |
| (Q) | A possible choice for \(\hat{n}\) is | (2) | \(\sqrt{\frac{3}{2}}\) |
| (R) | \(\overrightarrow{OR_1}\) equals | (3) | 1 |
| (S) | A possible value of \(\overrightarrow{OR_1}.\hat{n}\) is | (4) | \(\frac{1}{\sqrt6}\hat{i}-\frac{2}{\sqrt6}\hat{j}+\frac{1}{\sqrt6}\hat{k}\) |
| (5) | \(\sqrt{\frac{2}{3}}\) | ||
For the given problem, we have two lines \(L_1: \frac{x+11}{1}=\frac{y+21}{2}=\frac{z+29}{3}\) and \(L_2: \frac{x+16}{3}=\frac{y+11}{2}=\frac{z+4}{\gamma}\). These lines intersect at a point \(R_1\). We need to determine the matched items from List-I to List-II based on the conditions provided.
| (P) | γ equals | 3 |
| (Q) | A possible choice for \(\hat{n}\) | \(\frac{1}{\sqrt6}\hat{i}-\frac{2}{\sqrt6}\hat{j}+\frac{1}{\sqrt6}\hat{k}\) |
| (R) | \(\overrightarrow{OR_1}\) equals | \(-\hat{i}-\hat{j}+\hat{k}\) |
| (S) | A possible value of \(\overrightarrow{OR_1}.\hat{n}\) | \(\sqrt{\frac{2}{3}}\) |
Thus, the correct matching is (P) → (3), (Q) → (4), (R) → (1), (S) → (5).
We are given two lines \(L_1\) and \(L_2\) with parameters, and we want to find \(\gamma\), the point of intersection \(R_1\), a unit normal vector \(\hat{n}\) to the plane containing both lines, and the scalar product \(\overrightarrow{OR_1} \cdot \hat{n}\).
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Step 1: Parametric form of lines
\[ L_1: x = -11 + t, \quad y = -21 + 2t, \quad z = -29 + 3t \] \[ L_2: x = -16 + 3s, \quad y = -11 + 2s, \quad z = -4 + \gamma s \] ---
Step 2: Find \(t, s\) such that lines intersect
\[ -11 + t = -16 + 3s \implies t = -5 + 3s \] \[ -21 + 2t = -11 + 2s \implies 2t - 2s = 10 \implies t - s = 5 \] Substitute \(t\) from first into second: \[ (-5 + 3s) - s = 5 \implies 2s = 10 \implies s = 5 \] \[ t = -5 + 3 \times 5 = 10 \] ---
Step 3: Use \(z\)-coordinate to find \(\gamma\)
\[ -29 + 3t = -4 + \gamma s \implies -29 + 30 = -4 + 5 \gamma \implies 1 = -4 + 5 \gamma \implies \gamma = 1 \] ---
Step 4: Find coordinates of \(R_1\)
\[ x = -11 + 10 = -1, \quad y = -21 + 20 = -1, \quad z = -29 + 30 = 1 \] So, \[ \overrightarrow{OR_1} = (-1, -1, 1) \] ---
Step 5: Direction vectors of \(L_1\) and \(L_2\)
\[ \vec{d}_1 = (1, 2, 3), \quad \vec{d}_2 = (3, 2, 1) \] ---
Step 6: Find normal vector to the plane
\[ \vec{n} = \vec{d}_1 \times \vec{d}_2 = \begin{vmatrix} \hat{i} & \hat{j} & \hat{k} \\ 1 & 2 & 3 \\ 3 & 2 & 1 \\ \end{vmatrix} = (-4, 8, -4) \] ---
Step 7: Unit normal vector \(\hat{n}\)
\[ |\vec{n}| = \sqrt{(-4)^2 + 8^2 + (-4)^2} = \sqrt{16 + 64 + 16} = \sqrt{96} = 4 \sqrt{6} \] \[ \hat{n} = \frac{1}{4 \sqrt{6}} (-4, 8, -4) = \frac{1}{\sqrt{6}} (-1, 2, -1) \] ---
Step 8: Calculate \(\overrightarrow{OR_1} \cdot \hat{n}\)
\[ (-1, -1, 1) \cdot \frac{1}{\sqrt{6}} (-1, 2, -1) = \frac{1}{\sqrt{6}} (1 - 2 - 1) = \frac{-2}{\sqrt{6}} = -\frac{2}{\sqrt{6}} \] ---
Matching List-I to List-II:
\[ (P) \to (3) \quad \gamma = 1 \] \[ (Q) \to (4) \quad \hat{n} = \frac{1}{\sqrt{6}} (-\hat{i} + 2 \hat{j} - \hat{k}) \] \[ (R) \to (1) \quad \overrightarrow{OR_1} = -\hat{i} - \hat{j} + \hat{k} \] \[ (S) \to (5) \quad \overrightarrow{OR_1} \cdot \hat{n} = \sqrt{\frac{2}{3}} \quad \text{(absolute value)} \] ---
Final answer:
\[ \boxed{ (P) \to (3), \quad (Q) \to (4), \quad (R) \to (1), \quad (S) \to (5) } \]
Show that the following lines intersect. Also, find their point of intersection:
Line 1: \[ \frac{x - 1}{2} = \frac{y - 2}{3} = \frac{z - 3}{4} \]
Line 2: \[ \frac{x - 4}{5} = \frac{y - 1}{2} = z \]
Let $ a_0, a_1, ..., a_{23} $ be real numbers such that $$ \left(1 + \frac{2}{5}x \right)^{23} = \sum_{i=0}^{23} a_i x^i $$ for every real number $ x $. Let $ a_r $ be the largest among the numbers $ a_j $ for $ 0 \leq j \leq 23 $. Then the value of $ r $ is ________.
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity): 