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Q.The value of λ\lambda for which the angle between the lines r⃗=i^+j^+k^+p(2i^+j^+2k^)\vec{r} = \hat{i} + \hat{j} + \hat{k} + p(2\hat{i} + \hat{j} + 2\hat{k}) and r⃗=(1+q)i^+(1+qλ)j^+(1+q)k^\vec{r} = (1+q)\hat{i} + (1+q\lambda)\hat{j} + (1+q)\hat{k} is π2\frac{\pi}{2} is :

(a) −4-4
(b) 44
(c) 22
(d) −2-2
CBSECBSE Class XII Board 2023MCQ· 1mImportance★★★★★
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The angle between two lines is π2\frac{\pi}{2} when their direction vectors are perpendicular (dot product = 0). For the given lines, this gives λ=−4\lambda = -4, so the correct option is (a).

Concept & Intuition

When two lines in space are perpendicular, the angle between them is 90∘90^\circ (π/2\pi/2 radians). The key idea is that the direction vectors of the lines determine this angle — not their position vectors. The constant terms (i^+j^+k^\hat{i} + \hat{j} + \hat{k} in the first line, and the qq-dependent position in the second) only tell us where the lines are located, not which way they point.

For two lines with direction vectors d⃗1\vec{d}_1 and d⃗2\vec{d}_2, the angle θ\theta between them satisfies:

cos⁡θ=d⃗1⋅d⃗2∣d⃗1∣ ∣d⃗2∣\cos\theta = \frac{\vec{d}_1 \cdot \vec{d}_2}{|\vec{d}_1|\,|\vec{d}_2|}

When θ=π2\theta = \frac{\pi}{2}, cos⁡θ=0\cos\theta = 0, so the numerator must be zero: d⃗1⋅d⃗2=0\vec{d}_1 \cdot \vec{d}_2 = 0. That's the entire condition — no need to compute magnitudes or worry about the constant terms.

Watch out

A common mistake is to include the constant position vectors (i^+j^+k^\hat{i} + \hat{j} + \hat{k} etc.) in the dot product. Those are just points on the line, not directions. Only the coefficients of pp and qq matter.

Step-by-step solution

  1. Extract the direction vectors from each line. The first line is r⃗=i^+j^+k^+p(2i^+j^+2k^)\vec{r} = \hat{i} + \hat{j} + \hat{k} + p(2\hat{i} + \hat{j} + 2\hat{k}). The coefficient of pp is the direction vector:

d⃗1=2i^+j^+2k^\vec{d}_1 = 2\hat{i} + \hat{j} + 2\hat{k}

The second line is r⃗=(1+q)i^+(1+qλ)j^+(1+q)k^\vec{r} = (1+q)\hat{i} + (1+q\lambda)\hat{j} + (1+q)\hat{k}.

Rewrite it in the standard form r⃗=(constant)+q(direction)\vec{r} = \text{(constant)} + q(\text{direction}):

r⃗=(i^+j^+k^)+q(i^+λj^+k^)\vec{r} = (\hat{i} + \hat{j} + \hat{k}) + q(\hat{i} + \lambda\hat{j} + \hat{k})

So the direction vector is: …

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