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QJEEAdv12Ma85c1: JEE Advanced 2012 Physics - Class 11 JEEAdv12Ma85c1 Solution: If and are vectors such that and then a possible value of is

If a→\overrightarrow a and b→\overrightarrow b are vectors such that ∣a→+b→∣=29\left| {\overrightarrow a + \overrightarrow b } \right| = \sqrt {29} and  a→×(2i^+3j^+4k^)=(2i^+3j^+4k^)×b^,\,\overrightarrow a \times \left( {2\widehat i + 3\widehat j + 4\widehat k} \right) = \left( {2\widehat i + 3\widehat j + 4\widehat k} \right) \times \widehat b, then a possible value of (a→+b→).(−7i^+2j^+3k^)\left( {\overrightarrow a + \overrightarrow b } \right).\left( { - 7\widehat i + 2\widehat j + 3\widehat k} \right) is

Multiple Choice Options

  • A 00
  • B 33
  • C 44
  • D 88

Step-by-Step Verified Solution

amp; Given, a⃗×(2i^+3j^+4k^)=(2i^+3j^+4k^)×b⃗amp;amp;⇒a⃗×(2i^+3j^+4k^)−(2i^+3j^+4k^)×b⃗=0amp;⇒a⃗×(2i^+3j^+4k^)+b⃗×(2i^+3j^+4k^)=0amp;∴(A→×B→=−B→×A→)amp;⇒(a⃗+b⃗)×(2i^+3j^+4k^)=0\begin{aligned}& \text { Given, } \vec{a} \times(2 \hat{i}+3 \hat{j}+4 \hat{k})=(2 \hat{i}+3 \hat{j}+4 \hat{k}) \times \vec{b} \\& \begin{aligned}& \Rightarrow \vec{a} \times(2 \hat{i}+3 \hat{j}+4 \hat{k})-(2 \hat{i}+3 \hat{j}+4 \hat{k}) \times \vec{b}=0 \\& \Rightarrow \vec{a} \times(2 \hat{i}+3 \hat{j}+4 \hat{k})+\vec{b} \times(2 \hat{i}+3 \hat{j}+4 \hat{k})=0 \\& \therefore(\overrightarrow{\mathrm{A}} \times \overrightarrow{\mathrm{B}}=-\overrightarrow{\mathrm{B}} \times \overrightarrow{\mathrm{A}}) \\& \Rightarrow \quad (\vec{a}+\vec{b}) \times(2 \hat{i}+3 \hat{j}+4 \hat{k})=0\end{aligned}\end{aligned}

Hence, a⃗+b⃗\vec{a}+\vec{b} is collinear to 2i^+3j^+4k^2 \hat{i}+3 \hat{j}+4 \hat{k}

Let a⃗+b⃗=λ(2i^+3j^+4k^)... (i)\vec{a}+\vec{b}=\lambda(2 \hat{i}+3 \hat{j}+4 \hat{k})\quad \text{... (i)}

⇒amp;∣a⃗+b⃗∣=∣λ∣22+32+42⇒amp;29=∣λ∣29 (Given, ∣a⃗+b⃗∣=29)⇒amp;∣λ∣=1⇒amp;∣λ∣=±1∴amp;a⃗+b⃗=±(2i^+3j^+4k^)\begin{array}{l}\Rightarrow & |\vec{a}+\vec{b}|=|\lambda| \sqrt{2^2+3^2+4^2} \\\Rightarrow & \sqrt{29}=|\lambda| \sqrt{29} \quad \text { (Given, }|\vec{a}+\vec{b}|=\sqrt{29}) \\\Rightarrow & |\lambda|=1 \\\Rightarrow & |\lambda|= \pm 1 \\\therefore & \vec{a}+\vec{b}= \pm(2 \hat{i}+3 \hat{j}+4 \hat{k})\end{array}

 Now, amp;(a⃗+b⃗)⋅(−7i^+2j^+3k^)amp;=±(2i^+3j^+4k^)⋅(−7i^+2j^+3k^)amp;=±(−14+6+12)amp;=±4\begin{aligned}\text { Now, } &(\vec{a}+\vec{b}) \cdot(-7 \hat{i}+2 \hat{j}+3 \hat{k}) \\&= \pm(2 \hat{i}+3 \hat{j}+4 \hat{k}) \cdot(-7 \hat{i}+2 \hat{j}+3 \hat{k}) \\&= \pm(-14+6+12) \\&= \pm 4\end{aligned}

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