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Q.If two non-zero vectors a⃗\vec{a} and b⃗\vec{b} are such that (a⃗+b⃗)⊥a⃗(\vec{a} + \vec{b}) \perp \vec{a} and (2a⃗+b⃗)⊥b⃗(2\vec{a} + \vec{b}) \perp \vec{b}, then prove that ∣b⃗∣=2∣a⃗∣.|\vec{b}| = \sqrt{2} |\vec{a}|.

CBSECBSE Class XII Board 2024Subjective· 2mImportance★★★★★
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The condition that two vectors are perpendicular gives their dot product = 0. Using the two given perpendicular conditions, we form two equations in dot products, solve them, and directly obtain ∣b⃗∣=2∣a⃗∣|\vec{b}| = \sqrt{2} |\vec{a}|.

Why This Approach Works

When two vectors are perpendicular, their dot product is zero. That’s the single idea that unlocks the entire problem. We have two perpendicularity statements:

  1. (a⃗+b⃗)⊥a⃗(\vec{a} + \vec{b}) \perp \vec{a} means (a⃗+b⃗)⋅a⃗=0(\vec{a} + \vec{b}) \cdot \vec{a} = 0
  2. (2a⃗+b⃗)⊥b⃗(2\vec{a} + \vec{b}) \perp \vec{b} means (2a⃗+b⃗)⋅b⃗=0(2\vec{a} + \vec{b}) \cdot \vec{b} = 0

Each dot product expands using the distributive property. The unknowns are a⃗⋅a⃗=∣a⃗∣2\vec{a} \cdot \vec{a} = |\vec{a}|^2, b⃗⋅b⃗=∣b⃗∣2\vec{b} \cdot \vec{b} = |\vec{b}|^2, and a⃗⋅b⃗\vec{a} \cdot \vec{b}. We have two equations in these three unknowns — but we don’t need all three. We only need the relationship between ∣a⃗∣|\vec{a}| and ∣b⃗∣|\vec{b}|, and the equations will let us eliminate a⃗⋅b⃗\vec{a} \cdot \vec{b}.

Watch out

A common mistake is to assume a⃗⋅b⃗=0\vec{a} \cdot \vec{b} = 0 just because the vectors look “independent.” Nothing in the problem says a⃗\vec{a} and b⃗\vec{b} are perpendicular to each other — do not assume it.


Step-by-Step Solution

1. Write the first perpendicular condition

(a⃗+b⃗)⊥a⃗(\vec{a} + \vec{b}) \perp \vec{a} gives:

(a⃗+b⃗)⋅a⃗=0(\vec{a} + \vec{b}) \cdot \vec{a} = 0

Expand:

a⃗⋅a⃗+b⃗⋅a⃗=0\vec{a} \cdot \vec{a} + \vec{b} \cdot \vec{a} = 0

So:

∣a⃗∣2+a⃗⋅b⃗=0(1)|\vec{a}|^2 + \vec{a} \cdot \vec{b} = 0 \qquad(1)

2. Write the second perpendicular condition

(2a⃗+b⃗)⊥b⃗(2\vec{a} + \vec{b}) \perp \vec{b} gives:

(2a⃗+b⃗)⋅b⃗=0(2\vec{a} + \vec{b}) \cdot \vec{b} = 0

Expand:

2a⃗⋅b⃗+b⃗⋅b⃗=02\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{b} = 0

So:

2(a⃗⋅b⃗)+∣b⃗∣2=0(2)2(\vec{a} \cdot \vec{b}) + |\vec{b}|^2 = 0 \qquad(2) …

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