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Vector Algebra question

2023 · 25 Jan · Shift 1 · Q24
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  5. /2023 · 25 Jan · Shift 1 · Q24

Vector Algebra question

2023 · 25 Jan · Shift 1 · Q24

JEE MainMathematicsVector AlgebraMCQ+4 / −1
The vector a→=−i^+2j^+k^\overrightarrow a = - \widehat i + 2\widehat j + \widehat ka=−i+2j​+k is rotated through a right angle, passing through the y-axis in its way and the resulting vector is b→\overrightarrow bb. Then the projection of 3a→+2b→3\overrightarrow a + \sqrt 2 \overrightarrow b3a+2​b on c→=5i^+4j^+3k^\overrightarrow c = 5\widehat i + 4\widehat j + 3\widehat kc=5i+4j​+3k is :
  1. A
    6\sqrt66​
  2. B
    2 3\sqrt33​
  3. C
    1
  4. D
    3 2\sqrt22​
View written solutionFree

Correct answer: D

  1. Given vector

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

We are told that a⃗\vec aa is rotated through a right angle, and in doing so it passes through the y-axis. So the rotation is in the plane containing a⃗\vec aa and the yyy-axis, through 90∘90^\circ90∘, such that the final vector b⃗\vec bb lies on the other side of the yyy-axis.

  1. Find the magnitude of a⃗\vec aa

∣a⃗∣=(−1)2+22+12=1+4+1=6|\vec a|=\sqrt{(-1)^2+2^2+1^2}=\sqrt{1+4+1}=\sqrt6∣a∣=(−1)2+22+12​=1+4+1​=6​

Since rotation preserves magnitude,

∣b⃗∣=6|\vec b|=\sqrt6∣b∣=6​

  1. Use the y-axis as the intermediate direction

The unit vector along the yyy-axis is j^=(0,1,0)\hat j=(0,1,0)j^​=(0,1,0).

Now,

a⃗⋅j^=2\vec a\cdot \hat j = 2a⋅j^​=2

So the angle θ\thetaθ between a⃗\vec aa and the yyy-axis satisfies

cos⁡θ=26\cos\theta=\frac{2}{\sqrt6}cosθ=6​2​

Since the vector is rotated through 90∘90^\circ90∘ and passes through the yyy-axis in the process, the yyy-axis bisects the angle between a⃗\vec aa and b⃗\vec bb. Thus b⃗\vec bb is the reflection of a⃗\vec aa about the yyy-axis in the plane of rotation.

  1. Find b⃗\vec bb by reflection about the y-axis

Resolve a⃗\vec aa into components parallel and perpendicular to j^\hat jj^​:

  • Parallel component: a⃗∥=2j^=(0,2,0)\vec a_{\parallel} = 2\hat j = (0,2,0)a∥​=2j^​=(0,2,0)

  • Perpendicular component: a⃗⊥=a⃗−a⃗∥=(−1,0,1)\vec a_{\perp}=\vec a-\vec a_{\parallel}=(-1,0,1)a⊥​=a−a∥​=(−1,0,1)

Reflection about the yyy-axis keeps the parallel component same and reverses the perpendicular component:

b⃗=a⃗∥−a⃗⊥=(0,2,0)−(−1,0,1)=(1,2,−1)\vec b=\vec a_{\parallel}-\vec a_{\perp}=(0,2,0)-(-1,0,1)=(1,2,-1)b=a∥​−a⊥​=(0,2,0)−(−1,0,1)=(1,2,−1)

So,

b⃗=i^+2j^−k^\vec b=\hat i+2\hat j-\hat kb=i^+2j^​−k^

Check: a⃗⋅b⃗=(−1)(1)+2⋅2+1(−1)=−1+4−1=2\vec a\cdot \vec b = (-1)(1)+2\cdot2+1(-1)= -1+4-1=2a⋅b=(−1)(1)+2⋅2+1(−1)=−1+4−1=2

Also, ∣a⃗∣∣b⃗∣cos⁡90∘=0|\vec a||\vec b|\cos 90^\circ =0∣a∣∣b∣cos90∘=0

This seems inconsistent with a 90∘90^\circ90∘ angle between a⃗\vec aa and b⃗\vec bb, so let us interpret the statement more carefully.

  1. Correct interpretation of rotation through right angle

The vector is rotated by 90∘90^\circ90∘ in such a way that during rotation it passes through the yyy-axis. Hence the angle from a⃗\vec aa to the yyy-axis plus the angle from the yyy-axis to b⃗\vec bb is 90∘90^\circ90∘.

Let the angle between a⃗\vec aa and j^\hat jj^​ be θ\thetaθ, then angle between b⃗\vec bb and j^\hat jj^​ is 90∘−θ90^\circ-\theta90∘−θ.

Since rotation is in the plane of a⃗\vec aa and j^\hat jj^​, let us construct an orthonormal basis in that plane.

Take e^1=j^=(0,1,0)\hat e_1=\hat j=(0,1,0)e^1​=j^​=(0,1,0)

The component of a⃗\vec aa perpendicular to j^\hat jj^​ is (−1,0,1)(-1,0,1)(−1,0,1) with magnitude 2\sqrt22​, so e^2=12(−1,0,1)\hat e_2=\frac{1}{\sqrt2}(-1,0,1)e^2​=2​1​(−1,0,1)

Then a⃗=2e^1+2e^2\vec a=2\hat e_1+\sqrt2\hat e_2a=2e^1​+2​e^2​

Now rotating by 90∘90^\circ90∘ in this plane gives b⃗=−2e^1+2e^2\vec b=-\sqrt2\hat e_1+2\hat e_2b=−2​e^1​+2e^2​

or the opposite orientation b⃗=2e^1−2e^2\vec b=\sqrt2\hat e_1-2\hat e_2b=2​e^1​−2e^2​

We choose the one that passes through the positive yyy-axis while rotating from a⃗\vec aa; this is

b⃗=2e^1−2e^2\vec b=\sqrt2\hat e_1-2\hat e_2b=2​e^1​−2e^2​

So b⃗=2(0,1,0)−2⋅12(−1,0,1)\vec b=\sqrt2(0,1,0)-2\cdot \frac{1}{\sqrt2}(-1,0,1)b=2​(0,1,0)−2⋅2​1​(−1,0,1) b⃗=(2,2,−2)\vec b=(\sqrt2,\sqrt2,-\sqrt2)b=(2​,2​,−2​)

This gives a⃗⋅b⃗=(−1)(2)+2(2)+1(−2)=0\vec a\cdot \vec b = (-1)(\sqrt2)+2(\sqrt2)+1(-\sqrt2)=0a⋅b=(−1)(2​)+2(2​)+1(−2​)=0

So this is correct.

  1. Compute 3a⃗+2b⃗3\vec a+\sqrt2\vec b3a+2​b

First, 3a⃗=3(−1,2,1)=(−3,6,3)3\vec a=3(-1,2,1)=(-3,6,3)3a=3(−1,2,1)=(−3,6,3)

Also, 2b⃗=2(2,2,−2)=(2,2,−2)\sqrt2\vec b=\sqrt2(\sqrt2,\sqrt2,-\sqrt2)=(2,2,-2)2​b=2​(2​,2​,−2​)=(2,2,−2)

Thus, 3a⃗+2b⃗=(−3,6,3)+(2,2,−2)=(−1,8,1)3\vec a+\sqrt2\vec b = (-3,6,3)+(2,2,-2)=(-1,8,1)3a+2​b=(−3,6,3)+(2,2,−2)=(−1,8,1)

  1. Projection on c⃗=5i^+4j^+3k^=(5,4,3)\vec c=5\hat i+4\hat j+3\hat k=(5,4,3)c=5i^+4j^​+3k^=(5,4,3)

Scalar projection of vector v⃗\vec vv on c⃗\vec cc is

projc⃗(v⃗)=v⃗⋅c⃗∣c⃗∣\text{proj}_{\vec c}(\vec v)=\frac{\vec v\cdot \vec c}{|\vec c|}projc​(v)=∣c∣v⋅c​

Here v⃗=(−1,8,1)\vec v=(-1,8,1)v=(−1,8,1).

Compute dot product:

v⃗⋅c⃗=(−1)(5)+8(4)+1(3)=−5+32+3=30\vec v\cdot \vec c = (-1)(5)+8(4)+1(3)=-5+32+3=30v⋅c=(−1)(5)+8(4)+1(3)=−5+32+3=30

Now, ∣c⃗∣=52+42+32=25+16+9=50=52|\vec c|=\sqrt{5^2+4^2+3^2}=\sqrt{25+16+9}=\sqrt{50}=5\sqrt2∣c∣=52+42+32​=25+16+9​=50​=52​

Therefore projection is

3052=62=32\frac{30}{5\sqrt2}=\frac{6}{\sqrt2}=3\sqrt252​30​=2​6​=32​

  1. Compare with options

323\sqrt232​

So the correct option is D.

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