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Vector Algebra question

2023 · 11 Apr · Shift 1 · Q37
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  5. /2023 · 11 Apr · Shift 1 · Q37

Vector Algebra question

2023 · 11 Apr · Shift 1 · Q37

JEE MainMathematicsVector AlgebraMCQ+4 / −1
Let a⃗\vec{a}a be a non-zero vector parallel to the line of intersection of the two planes described by i^+j^,i^+k^\hat{i}+\hat{j}, \hat{i}+\hat{k}i^+j^​,i^+k^ and i^−j^,j^−k^\hat{i}-\hat{j}, \hat{j}-\hat{k}i^−j^​,j^​−k^. If θ\thetaθ is the angle between the vector a⃗\vec{a}a and the vector b⃗=2i^−2j^+k^\vec{b}=2 \hat{i}-2 \hat{j}+\hat{k}b=2i^−2j^​+k^ and a⃗⋅b⃗=6\vec{a} \cdot \vec{b}=6a⋅b=6, then the ordered pair (θ,∣a⃗×b⃗∣)(\theta,|\vec{a} \times \vec{b}|)(θ,∣a×b∣) is equal to :
  1. A
    (π3,36)\left(\frac{\pi}{3}, 3 \sqrt{6}\right)(3π​,36​)
  2. B
    (π3,6)\left(\frac{\pi}{3}, 6\right)(3π​,6)
  3. C
    (π4,36)\left(\frac{\pi}{4}, 3 \sqrt{6}\right)(4π​,36​)
  4. D
    (π4,6)\left(\frac{\pi}{4}, 6\right)(4π​,6)
View written solutionFree

Correct answer: D

  1. Interpret the planes from their spanning vectors

A plane described by two non-parallel vectors has those vectors lying in the plane, so its normal vector is their cross product.

  • First plane contains vectors i^+j^=(1,1,0)\hat i+\hat j=(1,1,0)i^+j^​=(1,1,0) and i^+k^=(1,0,1)\hat i+\hat k=(1,0,1)i^+k^=(1,0,1).
  • Second plane contains vectors i^−j^=(1,−1,0)\hat i-\hat j=(1,-1,0)i^−j^​=(1,−1,0) and j^−k^=(0,1,−1)\hat j-\hat k=(0,1,-1)j^​−k^=(0,1,−1).

The line of intersection of two planes is parallel to the cross product of their normals.


  1. Find normal to the first plane
n⃗1=(i^+j^)×(i^+k^)\vec n_1=(\hat i+\hat j)\times(\hat i+\hat k)n1​=(i^+j^​)×(i^+k^)

Using coordinates:

(1,1,0)×(1,0,1)=∣i^j^k^110101∣=i^(1)−j^(1)+k^(−1)(1,1,0)\times(1,0,1) =\begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & 1 & 0\\ 1 & 0 & 1 \end{vmatrix} =\hat i(1)-\hat j(1)+\hat k(-1)(1,1,0)×(1,0,1)=​i^11​j^​10​k^01​​=i^(1)−j^​(1)+k^(−1)

So,

n⃗1=i^−j^−k^=(1,−1,−1)\vec n_1=\hat i-\hat j-\hat k=(1,-1,-1)n1​=i^−j^​−k^=(1,−1,−1)
  1. Find normal to the second plane
n⃗2=(i^−j^)×(j^−k^)\vec n_2=(\hat i-\hat j)\times(\hat j-\hat k)n2​=(i^−j^​)×(j^​−k^)

Using coordinates:

(1,−1,0)×(0,1,−1)=∣i^j^k^1−1001−1∣=i^(1)−j^(−1)+k^(1)(1,-1,0)\times(0,1,-1) =\begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & -1 & 0\\ 0 & 1 & -1 \end{vmatrix} =\hat i(1)-\hat j(-1)+\hat k(1)(1,−1,0)×(0,1,−1)=​i^10​j^​−11​k^0−1​​=i^(1)−j^​(−1)+k^(1)

Thus,

n⃗2=i^+j^+k^=(1,1,1)\vec n_2=\hat i+\hat j+\hat k=(1,1,1)n2​=i^+j^​+k^=(1,1,1)
  1. Direction of line of intersection

A vector parallel to the line of intersection is

d⃗=n⃗1×n⃗2\vec d=\vec n_1\times \vec n_2d=n1​×n2​

So,

(1,−1,−1)×(1,1,1)=∣i^j^k^1−1−1111∣(1,-1,-1)\times(1,1,1) =\begin{vmatrix} \hat i & \hat j & \hat k\\ 1 & -1 & -1\\ 1 & 1 & 1 \end{vmatrix}(1,−1,−1)×(1,1,1)=​i^11​j^​−11​k^−11​​ =i^((−1)(1)−(−1)(1))−j^((1)(1)−(−1)(1))+k^((1)(1)−(−1)(1))=\hat i((-1)(1)-(-1)(1))- \hat j((1)(1)-(-1)(1))+ \hat k((1)(1)-(-1)(1))=i^((−1)(1)−(−1)(1))−j^​((1)(1)−(−1)(1))+k^((1)(1)−(−1)(1)) =i^(0)−j^(2)+k^(2)=(0,−2,2)=\hat i(0)-\hat j(2)+\hat k(2) =(0,-2,2)=i^(0)−j^​(2)+k^(2)=(0,−2,2)

Hence the line of intersection is parallel to

(0,−1,1)=−j^+k^(0,-1,1)= -\hat j+\hat k(0,−1,1)=−j^​+k^

Therefore, since a⃗\vec aa is non-zero and parallel to this line,

a⃗=λ(0,−1,1)\vec a=\lambda(0,-1,1)a=λ(0,−1,1)

for some non-zero scalar λ\lambdaλ.


  1. Use the condition a⃗⋅b⃗=6\vec a\cdot \vec b=6a⋅b=6

Given

b⃗=2i^−2j^+k^=(2,−2,1)\vec b=2\hat i-2\hat j+\hat k=(2,-2,1)b=2i^−2j^​+k^=(2,−2,1)

Now,

a⃗⋅b⃗=λ(0,−1,1)⋅(2,−2,1)\vec a\cdot \vec b=\lambda(0,-1,1)\cdot(2,-2,1)a⋅b=λ(0,−1,1)⋅(2,−2,1) =λ (0+2+1)=3λ=\lambda\,(0+2+1)=3\lambda=λ(0+2+1)=3λ

Given a⃗⋅b⃗=6\vec a\cdot \vec b=6a⋅b=6, so

3λ=6  ⟹  λ=23\lambda=6 \implies \lambda=23λ=6⟹λ=2

Thus,

a⃗=(0,−2,2)\vec a=(0,-2,2)a=(0,−2,2)
  1. Find the angle θ\thetaθ between a⃗\vec aa and b⃗\vec bb

First compute magnitudes:

∣a⃗∣=02+(−2)2+22=8=22|\vec a|=\sqrt{0^2+(-2)^2+2^2}=\sqrt{8}=2\sqrt2∣a∣=02+(−2)2+22​=8​=22​ ∣b⃗∣=22+(−2)2+12=9=3|\vec b|=\sqrt{2^2+(-2)^2+1^2}=\sqrt9=3∣b∣=22+(−2)2+12​=9​=3

Using dot product formula,

cos⁡θ=a⃗⋅b⃗∣a⃗∣∣b⃗∣=6(22)(3)=12\cos\theta=\frac{\vec a\cdot\vec b}{|\vec a||\vec b|} =\frac{6}{(2\sqrt2)(3)}=\frac{1}{\sqrt2}cosθ=∣a∣∣b∣a⋅b​=(22​)(3)6​=2​1​

Hence,

θ=π4\theta=\frac{\pi}{4}θ=4π​
  1. Find ∣a⃗×b⃗∣|\vec a\times \vec b|∣a×b∣

Using

∣a⃗×b⃗∣=∣a⃗∣∣b⃗∣sin⁡θ|\vec a\times \vec b|=|\vec a||\vec b|\sin\theta∣a×b∣=∣a∣∣b∣sinθ =(22)(3)(12)=6= (2\sqrt2)(3)\left(\frac{1}{\sqrt2}\right)=6=(22​)(3)(2​1​)=6

since for θ=π/4\theta=\pi/4θ=π/4, sin⁡θ=1/2\sin\theta=1/\sqrt2sinθ=1/2​.

So,

∣a⃗×b⃗∣=6|\vec a\times \vec b|=6∣a×b∣=6
  1. Final ordered pair
(θ,∣a⃗×b⃗∣)=(π4,6)(\theta,|\vec a\times \vec b|)=\left(\frac{\pi}{4},6\right)(θ,∣a×b∣)=(4π​,6)

This corresponds to Option D.

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