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Miscellaneous Exercise · Q13

Q.The scalar product of the vector i^+j^+k^\hat{i} + \hat{j} + \hat{k} with a unit vector along the sum of vectors 2i^+4j^−5k^2\hat{i} + 4\hat{j} - 5\hat{k} and λi^+2j^+3k^\lambda\hat{i} + 2\hat{j} + 3\hat{k} is equal to one. Find the value of λ\lambda.

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Appeared in past exams:CBSE 2019· Set 65/2/1· 4mexactCOMEDK 2024· Set 2024-E· 1mrewordedMHT-CET 2023· Set pcm-2023-05-09-M· 2mexact
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The key idea is to use the dot product formula: the scalar product of a⃗\vec{a} with a unit vector along b⃗\vec{b} equals ∣a⃗∣cos⁡θ|\vec{a}| \cos\theta. Setting this equal to 1 and solving gives λ=1\lambda = 1.

The problem asks: given that the dot product of i^+j^+k^\hat{i} + \hat{j} + \hat{k} with a unit vector along the sum of two other vectors equals 1, find λ\lambda.

Let’s unpack what’s really happening here. The scalar product (dot product) of two vectors gives a number. When one of them is a unit vector, that dot product is simply the component of the first vector along the direction of that unit vector. So the statement “scalar product equals 1” means the component of i^+j^+k^\hat{i} + \hat{j} + \hat{k} along the direction of the sum vector is exactly 1.

But the sum vector itself isn’t a unit vector — we have to make it one by dividing by its magnitude. That’s the crucial step students often miss.


Step 1: Find the sum vector

Let

a⃗=i^+j^+k^\vec{a} = \hat{i} + \hat{j} + \hat{k}

b⃗=2i^+4j^−5k^\vec{b} = 2\hat{i} + 4\hat{j} - 5\hat{k}

c⃗=λi^+2j^+3k^\vec{c} = \lambda\hat{i} + 2\hat{j} + 3\hat{k}

The sum is:

b⃗+c⃗=(2+λ)i^+(4+2)j^+(−5+3)k^\vec{b} + \vec{c} = (2 + \lambda)\hat{i} + (4 + 2)\hat{j} + (-5 + 3)\hat{k}

b⃗+c⃗=(2+λ)i^+6j^−2k^\vec{b} + \vec{c} = (2 + \lambda)\hat{i} + 6\hat{j} - 2\hat{k}


Step 2: The unit vector along the sum

A unit vector in the direction of any vector v⃗\vec{v} is v⃗∣v⃗∣\frac{\vec{v}}{|\vec{v}|}. So the unit vector along b⃗+c⃗\vec{b} + \vec{c} is:

u^=(2+λ)i^+6j^−2k^(2+λ)2+62+(−2)2\hat{u} = \frac{(2 + \lambda)\hat{i} + 6\hat{j} - 2\hat{k}}{\sqrt{(2 + \lambda)^2 + 6^2 + (-2)^2}}

The denominator is the magnitude:

∣b⃗+c⃗∣=(2+λ)2+36+4=(2+λ)2+40|\vec{b} + \vec{c}| = \sqrt{(2 + \lambda)^2 + 36 + 4} = \sqrt{(2 + \lambda)^2 + 40}


Step 3: Set up the dot product condition

The scalar product of a⃗\vec{a} with this unit vector is given to be 1:

a⃗⋅u^=1\vec{a} \cdot \hat{u} = 1

Substitute:

(i^+j^+k^)⋅(2+λ)i^+6j^−2k^(2+λ)2+40=1(\hat{i} + \hat{j} + \hat{k}) \cdot \frac{(2 + \lambda)\hat{i} + 6\hat{j} - 2\hat{k}}{\sqrt{(2 + \lambda)^2 + 40}} = 1


Step 4: Compute the dot product in the numerator

Dot product of i^+j^+k^\hat{i} + \hat{j} + \hat{k} with (2+λ)i^+6j^−2k^(2 + \lambda)\hat{i} + 6\hat{j} - 2\hat{k}:

  • i^⋅i^\hat{i} \cdot \hat{i} term: 1⋅(2+λ)=2+λ1 \cdot (2 + \lambda) = 2 + \lambda
  • j^⋅j^\hat{j} \cdot \hat{j} term: 1⋅6=61 \cdot 6 = 6
  • k^⋅k^\hat{k} \cdot \hat{k} term: 1⋅(−2)=−21 \cdot (-2) = -2

Sum: (2+λ)+6+(−2)=λ+6(2 + \lambda) + 6 + (-2) = \lambda + 6

So the equation becomes:

λ+6(2+λ)2+40=1\frac{\lambda + 6}{\sqrt{(2 + \lambda)^2 + 40}} = 1


Step 5: Solve for λ\lambda

Multiply both sides by the denominator:

λ+6=(2+λ)2+40\lambda + 6 = \sqrt{(2 + \lambda)^2 + 40}

Square both sides (but check later for extraneous solutions): …

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