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Exercise 11.2 · Q4

Q.Find the equation of the line which passes through the point (1,2,3)(1, 2, 3) and is parallel to the vector 3i^+2j^−2k^3\hat{i} + 2\hat{j} - 2\hat{k}.

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The vector equation of a line is r⃗=a⃗+λb⃗\vec{r} = \vec{a} + \lambda \vec{b}. Here a⃗=i^+2j^+3k^\vec{a} = \hat{i} + 2\hat{j} + 3\hat{k} and b⃗=3i^+2j^−2k^\vec{b} = 3\hat{i} + 2\hat{j} - 2\hat{k}, so the required equation is r⃗=(i^+2j^+3k^)+λ(3i^+2j^−2k^)\vec{r} = (\hat{i} + 2\hat{j} + 3\hat{k}) + \lambda (3\hat{i} + 2\hat{j} - 2\hat{k}).

The core idea is beautifully simple: a line is just a straight path. If you know one point on it and the direction you're heading, you can describe every other point by starting at that known point and taking some number of steps in that direction.

Think of it like this. You're standing at a fixed location — that's your given point (1,2,3)(1, 2, 3). You have a compass that always points in the same direction — that's the vector 3i^+2j^−2k^3\hat{i} + 2\hat{j} - 2\hat{k}. If you take one step forward in that direction, you reach a new point. If you take two steps, you go further. If you step backward (a negative number of steps), you go the other way along the same line. Every possible point on the line corresponds to some number of steps, which we call a parameter.

This is exactly what the vector equation of a line captures.

The vector equation of a line through point with position vector a⃗\vec{a} and parallel to vector b⃗\vec{b} is:

r⃗=a⃗+λb⃗,λ∈R\vec{r} = \vec{a} + \lambda \vec{b}, \quad \lambda \in \mathbb{R}

Now let's apply this to the given problem.

  1. Identify the position vector of the given point. The point is (1,2,3)(1, 2, 3). Its position vector (the vector from the origin to the point) is:

a⃗=i^+2j^+3k^\vec{a} = \hat{i} + 2\hat{j} + 3\hat{k}

  1. Identify the direction vector. The line is parallel to 3i^+2j^−2k^3\hat{i} + 2\hat{j} - 2\hat{k}, so this is our direction vector:

b⃗=3i^+2j^−2k^\vec{b} = 3\hat{i} + 2\hat{j} - 2\hat{k}

  1. Write the vector equation. Substitute a⃗\vec{a} and b⃗\vec{b} into the formula: r⃗=(i^+2j^+3k^)+λ(3i^+2j^−2k^)\vec{r} = (\hat{i} + 2\hat{j} + 3\hat{k}) + \lambda (3\hat{i} + 2\hat{j} - 2\hat{k}) …

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