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Q.If a⃗,b⃗\vec{a}, \vec{b} and c⃗\vec{c} are unit vectors such that a⃗+b⃗+c⃗=0⃗\vec{a} + \vec{b} + \vec{c} = \vec{0}, then (a⃗⋅b⃗+b⃗⋅c⃗+c⃗⋅a⃗)(\vec{a} \cdot \vec{b} + \vec{b} \cdot \vec{c} + \vec{c} \cdot \vec{a}) is equal to :
(A) 32\frac{3}{2}
(B) 12\frac{1}{2}
(C) −12-\frac{1}{2}
(D) −32-\frac{3}{2}

CBSECBSE Class XII Board 2024MCQ· 1mImportance★★★★★
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The key idea is to square the given vector sum condition and use the fact that each vector is a unit vector. The sum of the dot products equals −32-\frac{3}{2}, which corresponds to option (D).

We have three unit vectors a⃗,b⃗,c⃗\vec{a}, \vec{b}, \vec{c} — each has magnitude 11. They satisfy a⃗+b⃗+c⃗=0⃗\vec{a} + \vec{b} + \vec{c} = \vec{0}. This means the three vectors form a closed triangle when placed head-to-tail. The question asks for the sum of their pairwise dot products.

The direct approach: take the dot product of the sum with itself. Since the sum is zero, its magnitude squared is zero. But the square of the sum expands into a sum of squares and cross terms — exactly what we need.

  1. Start with the given condition.

    a⃗+b⃗+c⃗=0⃗\vec{a} + \vec{b} + \vec{c} = \vec{0}.

  2. Take the dot product of both sides with itself.

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

  3. Expand the left-hand side.

    The dot product distributes:

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

Since dot product is commutative (a⃗⋅b⃗=b⃗⋅a⃗\vec{a}\cdot\vec{b} = \vec{b}\cdot\vec{a}), each cross term appears twice. So:

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

  1. Use the unit vector property. For any unit vector, a⃗⋅a⃗=∣a⃗∣2=1\vec{a}\cdot\vec{a} = |\vec{a}|^2 = 1. So:

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