arthham

JEE Advanced 2024 · Introduction to Three Dimensional Geometry

Let OP⃗=α−1αi^+j^+k^\vec{OP} = \frac{\alpha - 1}{\alpha}\hat{i} + \hat{j} + \hat{k}, OQ⃗=i^+β−1βj^+k^\vec{OQ} = \hat{i} + \frac{\beta - 1}{\beta}\hat{j} + \hat{k} and OR‾=i^+j^+12k^\overline{OR} = \hat{i} + \hat{j} + \frac{1}{2}\hat{k} be three vectors, where a,b∈R−{0}a, b \in \mathbb{R} - \{0\} and O denotes the origin. If (OP⃗×OQ⃗)⋅OR⃗=0(\vec{OP} \times \vec{OQ}) \cdot \vec{OR} = 0 and the point (α,β,2)(\alpha, \beta, 2) lies on the plane 3x+3y−z+l=03x + 3y - z + l = 0 then the value of ll is ________.

Answer: 55

Watch this solved on the board The full walkthrough, written out a line at a time with narration explaining each step as it appears. Pause anywhere and ask why a line is there. Free to watch

Or read the worked solution below. Jump to the steps ↓

Written solution

OP⃗=α−1αi^+j^+k^,OQ⃗=i^+β−1βj^+k^\vec{OP} = \dfrac{\alpha-1}{\alpha}\hat{i} + \hat{j} + \hat{k},\quad \vec{OQ} = \hat{i} + \dfrac{\beta-1}{\beta}\hat{j} + \hat{k} OR⃗=i^+j^+12k^,a,b∈R−{0}\vec{OR} = \hat{i} + \hat{j} + \dfrac{1}{2}\hat{k},\quad a, b \in \mathbb{R} - \{0\} (OP⃗×OQ⃗)⋅OR⃗=0(\vec{OP} \times \vec{OQ}) \cdot \vec{OR} = 0 (α,β,2) lies on 3x+3y−z+l=0(\alpha, \beta, 2) \text{ lies on } 3x + 3y - z + l = 0 To find: l\text{To find: } l (OP⃗×OQ⃗)⋅OR⃗=0⇒OP⃗,OQ⃗,OR⃗ coplanar(\vec{OP} \times \vec{OQ}) \cdot \vec{OR} = 0 \Rightarrow \vec{OP}, \vec{OQ}, \vec{OR} \text{ coplanar} ⇔det⁡[OP⃗ OQ⃗ OR⃗]=0\Leftrightarrow \det[\vec{OP}\ \vec{OQ}\ \vec{OR}] = 0 ∣α−1α111β−1β11112∣=0\begin{vmatrix} \frac{\alpha-1}{\alpha} & 1 & 1 \\ 1 & \frac{\beta-1}{\beta} & 1 \\ 1 & 1 & \tfrac{1}{2} \end{vmatrix} = 0 Let a=1−1α,b=1−1β\text{Let } a = 1-\dfrac{1}{\alpha},\quad b = 1-\dfrac{1}{\beta} a(b2−1)−(12−1)+(1−b)=0a\left(\dfrac{b}{2}-1\right) - \left(\dfrac{1}{2}-1\right) + (1-b) = 0 a(b−2)2+32−b=0\dfrac{a(b-2)}{2} + \dfrac{3}{2} - b = 0 a(b−2)+3−2b=0⇒a(b−2)=2b−3a(b-2) + 3 - 2b = 0 \Rightarrow a(b-2) = 2b-3 b=1−1β⇒b−2=−β+1β,2b−3=−β+2βb = 1-\dfrac{1}{\beta} \Rightarrow b-2 = -\dfrac{\beta+1}{\beta},\quad 2b-3 = -\dfrac{\beta+2}{\beta} (1−1α)(β+1)=β+2\left(1-\dfrac{1}{\alpha}\right)(\beta+1) = \beta+2 1α=1−β+2β+1=−1β+1\dfrac{1}{\alpha} = 1 - \dfrac{\beta+2}{\beta+1} = \dfrac{-1}{\beta+1} α=−(β+1)⇒α+β=−1\alpha = -(\beta+1) \Rightarrow \alpha + \beta = -1 3α+3β−2+l=0⇒l=2−3(α+β)3\alpha + 3\beta - 2 + l = 0 \Rightarrow l = 2 - 3(\alpha+\beta) l=2−3(−1)=5l = 2 - 3(-1) = 5 l=5\boxed{l = 5}

More from Introduction to Three Dimensional Geometry

All 37 Introduction to Three Dimensional Geometry questions →