MCQMediumJEE 2023Cross Product

JEE Mathematics 2023 Question with Solution

Let a=2i^7j^+5k^\vec{a} = 2\hat{i} - 7\hat{j} + 5\hat{k}, b=i^+k^\vec{b} = \hat{i} + \hat{k}, and c=i^+2j^3k^\vec{c} = \hat{i} + 2\hat{j} - 3\hat{k} be three given vectors. If r\vec{r} is a vector such that r×a=c×a\vec{r} \times \vec{a} = \vec{c} \times \vec{a} and rb=0\vec{r} \cdot \vec{b} = 0, then r|\vec{r}| is equal to:

  • A

    1172\frac{11}{7} \sqrt{2}

  • B

    117\frac{11}{7}

  • C

    1152\frac{11}{5} \sqrt{2}

  • D

    9147\frac{\sqrt{914}}{7}

Answer

Correct answer:A

Step-by-step solution

Standard Method

Given: a=2i^7j^+5k^\vec{a} = 2\hat{i} - 7\hat{j} + 5\hat{k}, b=i^+k^\vec{b} = \hat{i} + \hat{k}, c=i^+2j^3k^\vec{c} = \hat{i} + 2\hat{j} - 3\hat{k}.

Find: r|\vec{r}|, given that r×a=c×a\vec{r} \times \vec{a} = \vec{c} \times \vec{a} and rb=0\vec{r} \cdot \vec{b} = 0.

From

r×a=c×a\vec{r} \times \vec{a} = \vec{c} \times \vec{a}

we get

(rc)×a=0.(\vec{r} - \vec{c}) \times \vec{a} = 0.

This implies that rc\vec{r} - \vec{c} is parallel to a\vec{a}, so

r=c+λa\vec{r} = \vec{c} + \lambda \vec{a}

for some scalar λ\lambda.

Using rb=0\vec{r} \cdot \vec{b} = 0,

(c+λa)b=0(\vec{c} + \lambda \vec{a}) \cdot \vec{b} = 0

which gives

cb+λ(ab)=0.\vec{c} \cdot \vec{b} + \lambda (\vec{a} \cdot \vec{b}) = 0.

Now,

cb=(i^+2j^3k^)(i^+k^)=1+03=2\vec{c} \cdot \vec{b} = (\hat{i} + 2\hat{j} - 3\hat{k}) \cdot (\hat{i} + \hat{k}) = 1 + 0 - 3 = -2

and

ab=(2i^7j^+5k^)(i^+k^)=2+0+5=7.\vec{a} \cdot \vec{b} = (2\hat{i} - 7\hat{j} + 5\hat{k}) \cdot (\hat{i} + \hat{k}) = 2 + 0 + 5 = 7.

So,

2+7λ=0-2 + 7\lambda = 0

which gives

λ=27.\lambda = \frac{2}{7}.

Hence,

r=(i^+2j^3k^)+27(2i^7j^+5k^).\vec{r} = (\hat{i} + 2\hat{j} - 3\hat{k}) + \frac{2}{7}(2\hat{i} - 7\hat{j} + 5\hat{k}).

Expanding,

r=i^+2j^3k^+47i^2j^+107k^.\vec{r} = \hat{i} + 2\hat{j} - 3\hat{k} + \frac{4}{7}\hat{i} - 2\hat{j} + \frac{10}{7}\hat{k}.

Therefore,

r=(1+47)i^+(22)j^+(3+107)k^\vec{r} = \left(1 + \frac{4}{7}\right)\hat{i} + (2 - 2)\hat{j} + \left(-3 + \frac{10}{7}\right)\hat{k}

so

r=117i^117k^.\vec{r} = \frac{11}{7}\hat{i} - \frac{11}{7}\hat{k}.

Now,

r=(117)2+(117)2|\vec{r}| = \sqrt{\left(\frac{11}{7}\right)^2 + \left(-\frac{11}{7}\right)^2}

which becomes

r=12149+12149=24249=1172.|\vec{r}| = \sqrt{\frac{121}{49} + \frac{121}{49}} = \sqrt{\frac{242}{49}} = \frac{11}{7}\sqrt{2}.

Therefore, the magnitude of r\vec{r} is 1172\frac{11}{7}\sqrt{2}, so the correct option is A.

Use parallel vector idea quickly

Given: r×a=c×a\vec{r} \times \vec{a} = \vec{c} \times \vec{a} and rb=0\vec{r} \cdot \vec{b} = 0.

Find: r|\vec{r}|.

Since

(rc)×a=0,(\vec{r} - \vec{c}) \times \vec{a} = 0,

vector rc\vec{r} - \vec{c} must be parallel to a\vec{a}. So write directly

r=c+λa.\vec{r} = \vec{c} + \lambda \vec{a}.

Now enforce the perpendicularity condition with b\vec{b}:

(c+λa)b=0.(\vec{c} + \lambda \vec{a}) \cdot \vec{b} = 0.

That gives

λ=cbab=27=27.\lambda = -\frac{\vec{c} \cdot \vec{b}}{\vec{a} \cdot \vec{b}} = -\frac{-2}{7} = \frac{2}{7}.

Hence,

r=c+27a=117i^117k^.\vec{r} = \vec{c} + \frac{2}{7}\vec{a} = \frac{11}{7}\hat{i} - \frac{11}{7}\hat{k}.

So,

r=(117)2+(117)2=1172.|\vec{r}| = \sqrt{\left(\frac{11}{7}\right)^2 + \left(\frac{11}{7}\right)^2} = \frac{11}{7}\sqrt{2}.

This shortcut works because the cross product condition immediately restricts r\vec{r} to a line parallel to a\vec{a} through c\vec{c}, and the dot product condition then determines the scalar uniquely. Therefore, the correct option is A.

Common mistakes

  • Assuming r=c\vec{r} = \vec{c} from r×a=c×a\vec{r} \times \vec{a} = \vec{c} \times \vec{a} is incorrect. Equal cross products with the same vector only imply that (rc)×a=0(\vec{r} - \vec{c}) \times \vec{a} = 0, so rc\vec{r} - \vec{c} is parallel to a\vec{a}. Always write r=c+λa\vec{r} = \vec{c} + \lambda \vec{a}.

  • Computing the dot products incorrectly is a common error. In particular, cb=1+03=2\vec{c} \cdot \vec{b} = 1 + 0 - 3 = -2 and ab=2+0+5=7\vec{a} \cdot \vec{b} = 2 + 0 + 5 = 7. Match coefficients of i^\hat{i}, j^\hat{j}, and k^\hat{k} carefully before solving for λ\lambda.

  • While finding the magnitude, students sometimes forget to square both nonzero components or mishandle the negative sign. Since magnitude uses squares, (117)2=(117)2\left(-\frac{11}{7}\right)^2 = \left(\frac{11}{7}\right)^2. Use r=x2+y2+z2|\vec{r}| = \sqrt{x^2 + y^2 + z^2} correctly.

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