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Exercise 11.2 · Q8

Q.Find the angle between the following pairs of lines:

(i) r⃗=2i^−5j^+k^+λ(3i^+2j^+6k^)\vec{r} = 2\hat{i} - 5\hat{j} + \hat{k} + \lambda(3\hat{i} + 2\hat{j} + 6\hat{k}) and r⃗=7i^−6k^+μ(i^+2j^+2k^)\vec{r} = 7\hat{i} - 6\hat{k} + \mu(\hat{i} + 2\hat{j} + 2\hat{k})
(ii) r⃗=3i^+j^−2k^+λ(i^−j^−2k^)\vec{r} = 3\hat{i} + \hat{j} - 2\hat{k} + \lambda(\hat{i} - \hat{j} - 2\hat{k}) and r⃗=2i^−j^−56k^+μ(3i^−5j^−4k^)\vec{r} = 2\hat{i} - \hat{j} - 56\hat{k} + \mu(3\hat{i} - 5\hat{j} - 4\hat{k})
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The angle between two lines in vector form is found using the dot product of their direction vectors. For (i) the angle is θ=cos⁡−1(1921)\theta = \cos^{-1}\left(\frac{19}{21}\right), and for (ii) the angle is θ=cos⁡−1(8315)\theta = \cos^{-1}\left(\frac{8\sqrt{3}}{15}\right).

The key idea is simple: a line in space is defined by a point and a direction. The direction vector tells you which way the line runs. When two lines are given in the form r⃗=a⃗+λb⃗\vec{r} = \vec{a} + \lambda \vec{b}, the angle between them is just the angle between their direction vectors b⃗1\vec{b}_1 and b⃗2\vec{b}_2. The position vectors a⃗\vec{a} don't matter at all for the angle — they only tell you where the lines are located, not how they're oriented.

Why does this work? Because the direction vector is like an arrow along the line. If you slide both arrows to the same starting point, the angle between them is exactly the angle between the lines. The dot product formula b⃗1⋅b⃗2=∣b⃗1∣∣b⃗2∣cos⁡θ\vec{b}_1 \cdot \vec{b}_2 = |\vec{b}_1| |\vec{b}_2| \cos \theta gives us cos⁡θ\cos \theta, and then we take the inverse cosine.

Watch out

A common mistake is to include the position vectors a⃗\vec{a} in the dot product. They are irrelevant for the angle — only the coefficients of λ\lambda and μ\mu matter.

Let's work through each part step by step.

Part (i)

  1. Identify the direction vectors.

    For the first line, r⃗=2i^−5j^+k^+λ(3i^+2j^+6k^)\vec{r} = 2\hat{i} - 5\hat{j} + \hat{k} + \lambda(3\hat{i} + 2\hat{j} + 6\hat{k}), the direction vector is b⃗1=3i^+2j^+6k^\vec{b}_1 = 3\hat{i} + 2\hat{j} + 6\hat{k}.

    For the second line, r⃗=7i^−6k^+μ(i^+2j^+2k^)\vec{r} = 7\hat{i} - 6\hat{k} + \mu(\hat{i} + 2\hat{j} + 2\hat{k}), the direction vector is b⃗2=i^+2j^+2k^\vec{b}_2 = \hat{i} + 2\hat{j} + 2\hat{k}.

  2. Compute the dot product.

    b⃗1⋅b⃗2=(3)(1)+(2)(2)+(6)(2)=3+4+12=19\vec{b}_1 \cdot \vec{b}_2 = (3)(1) + (2)(2) + (6)(2) = 3 + 4 + 12 = 19.

  3. Find the magnitudes.

    ∣b⃗1∣=32+22+62=9+4+36=49=7|\vec{b}_1| = \sqrt{3^2 + 2^2 + 6^2} = \sqrt{9 + 4 + 36} = \sqrt{49} = 7.

    ∣b⃗2∣=12+22+22=1+4+4=9=3|\vec{b}_2| = \sqrt{1^2 + 2^2 + 2^2} = \sqrt{1 + 4 + 4} = \sqrt{9} = 3.

  4. Apply the formula.

    cos⁡θ=b⃗1⋅b⃗2∣b⃗1∣∣b⃗2∣=197×3=1921\cos \theta = \frac{\vec{b}_1 \cdot \vec{b}_2}{|\vec{b}_1| |\vec{b}_2|} = \frac{19}{7 \times 3} = \frac{19}{21}.

    Therefore, θ=cos⁡−1(1921)\theta = \cos^{-1}\left(\frac{19}{21}\right).

Tip

Notice that 19/2119/21 is already in simplest form. If the dot product had been zero, the lines would be perpendicular. If the direction vectors were scalar multiples, the lines would be parallel.

Part (ii)

  1. Identify the direction vectors. First line: r⃗=3i^+j^−2k^+λ(i^−j^−2k^)\vec{r} = 3\hat{i} + \hat{j} - 2\hat{k} + \lambda(\hat{i} - \hat{j} - 2\hat{k}), so b⃗1=i^−j^−2k^\vec{b}_1 = \hat{i} - \hat{j} - 2\hat{k}. …

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