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JEE Main 202228 JulyMorning Shift
Exam
JEE Main
Year
2022
Date
28 July
Shift
Morning Shift
Subject
Mathematics
Chapter
Vector Algebra

JEE Main 2022 · 28 July · Morning Shift · Mathematics · Vector Algebra

Let a vector → a has a magnitude 9 . Let a vector → b be such that...

Let a vector a→\overset{\to}{a} has a magnitude 99. Let a vector b→\overset{\to}{b} be such that for every \left(x, y\right)R \times R - \left\{\left(0, 0\right)\right\},thevector(xa→+yb→), the vector \left(x\overset{\to}{a} + y\overset{\to}{b}\right) is perpendicular to the vector \left(6y\overset{\to}{a} - 18x\overset{\to}{b}\right).Thenthevalueof∣a→×b→∣. Then the value of \left|\overset{\to}{a} \times \overset{\to}{b}\right| is equal to

Options

  1. A939\sqrt{3}
  2. B27327\sqrt{3}
  3. C99
  4. D8181

Correct answer

B. 27327\sqrt{3}

Step-by-step solution

Given, ∣a→∣=9\left|\overset{\to}{a}\right| = 9

And \left(x\overset{\to}{a} + y\overset{\to}{b}\right) \cdot \left(6y\overset{\to}{a} - 18x\overset{\to}{b}\right) = 0${as they are perpendicular}\left\{\text{as they are perpendicular}\right\}

⇒6xy∣a→∣2−18x2(a→⋅b→)+6y2(a→⋅b→)−18xy∣b→∣2=0⇒ 6xy{\left|\overset{\to}{a}\right|}^{2} - 18{x}^{2}\left(\overset{\to}{a} \cdot \overset{\to}{b}\right) + 6{y}^{2}\left(\overset{\to}{a} \cdot \overset{\to}{b}\right) - 18xy{\left|\overset{\to}{b}\right|}^{2} = 0

⇒6xy(∣a→∣2−3∣b→∣2)+(a→⋅b→)(y2−3x2)=0⇒ 6xy\left({\left|\overset{\to}{a}\right|}^{2} - 3{\left|\overset{\to}{b}\right|}^{2}\right) + \left(\overset{\to}{a} \cdot \overset{\to}{b}\right)\left({y}^{2} - 3{x}^{2}\right) = 0

This should hold ∀x,y∈R×R−{(0,0)}\forall x, y \in R \times R - \left\{\left(0, 0\right)\right\}

So, ∣a→∣2−3∣b→∣2=0 and (a→⋅b→)=0{\left|\overset{\to}{a}\right|}^{2} - 3{\left|\overset{\to}{b}\right|}^{2} = 0 \text{ and } \left(\overset{\to}{a} \cdot \overset{\to}{b}\right) = 0

∴∣a→∣2=3∣b→∣2 and (a→⋅b→)=0⇒cosθ=0⇒θ=90°∴ {\left|\overset{\to}{a}\right|}^{2} = 3{\left|\overset{\to}{b}\right|}^{2} \text{ and } \left(\overset{\to}{a} \cdot \overset{\to}{b}\right) = 0 ⇒ cos\theta = 0 ⇒ \theta = 90 °

Now ∣a→×b→∣2=∣a→∣2∣b→∣2sin⁡2θ=∣a→∣2∣b→∣2{asθ=90°}{\left|\overset{\to}{a} \times \overset{\to}{b}\right|}^{2} = {\left|\overset{\to}{a}\right|}^{2}{\left|\overset{\to}{b}\right|}^{2}\sin^{2}\theta = {\left|\overset{\to}{a}\right|}^{2}{\left|\overset{\to}{b}\right|}^{2}\left\{\text{as}\theta = {90}^{°}\right\}

=∣a→∣2⋅∣a→∣23= {\left|\overset{\to}{a}\right|}^{2} \cdot \dfrac{{\left|\overset{\to}{a}\right|}^{2}}{3} \left\{\text{as}{\left|\overset{\to}{b}\right|}^{2} = \dfrac{{\left|\overset{\to}{a}\right|}^{2}}{3}\right\}$

So, \left|\overset{\to}{a} \times \overset{\to}{b}\right| = \dfrac{{\left|\overset{\to}{a}\right|}^{2}}{\sqrt{3}} = \dfrac{81}{\sqrt{3}} = 27\sqrt{3}

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