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Exercise 10.3 · Q11

Q.Show that ∣a⃗∣b⃗+∣b⃗∣a⃗|\vec{a}|\vec{b}+|\vec{b}|\vec{a} is perpendicular to ∣a⃗∣b⃗−∣b⃗∣a⃗,|\vec{a}|\vec{b}-|\vec{b}|\vec{a}, for any two nonzero vectors a⃗\vec{a} and b⃗.\vec{b}.

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The key idea is to use the dot product condition for perpendicular vectors: two vectors are perpendicular iff their dot product is zero. We compute the dot product of the given expressions and show it simplifies to zero using the fact that ∣a⃗∣2∣b⃗∣2−∣b⃗∣2∣a⃗∣2=0|\vec{a}|^2 |\vec{b}|^2 - |\vec{b}|^2 |\vec{a}|^2 = 0.

Why This Approach Works

For any two nonzero vectors a⃗\vec{a} and b⃗\vec{b}, we want to prove that the vectors u⃗=∣a⃗∣b⃗+∣b⃗∣a⃗\vec{u} = |\vec{a}|\vec{b} + |\vec{b}|\vec{a} and v⃗=∣a⃗∣b⃗−∣b⃗∣a⃗\vec{v} = |\vec{a}|\vec{b} - |\vec{b}|\vec{a} are perpendicular. The fundamental condition for perpendicularity (orthogonality) is that their dot product equals zero: u⃗⋅v⃗=0\vec{u} \cdot \vec{v} = 0.

The trick here is that the coefficients ∣a⃗∣|\vec{a}| and ∣b⃗∣|\vec{b}| are scalars (numbers), so they can be pulled out of dot products freely. The expression will simplify beautifully because the cross-terms cancel — a classic pattern where (A+B)⋅(A−B)=A⋅A−B⋅B(A+B)\cdot(A-B) = A\cdot A - B\cdot B.

Watch out

A common mistake is to treat ∣a⃗∣b⃗|\vec{a}|\vec{b} as a scalar times a vector, but then forget that ∣a⃗∣|\vec{a}| is just a number. When taking dot products, scalars factor out normally: (kx⃗)⋅(my⃗)=km(x⃗⋅y⃗)(k\vec{x})\cdot (m\vec{y}) = km (\vec{x}\cdot\vec{y}).

Step-by-Step Solution

1. Define the two vectors clearly.

Let:

u⃗=∣a⃗∣b⃗+∣b⃗∣a⃗\vec{u} = |\vec{a}|\vec{b} + |\vec{b}|\vec{a}

v⃗=∣a⃗∣b⃗−∣b⃗∣a⃗\vec{v} = |\vec{a}|\vec{b} - |\vec{b}|\vec{a}

We need to show u⃗⋅v⃗=0\vec{u} \cdot \vec{v} = 0.

2. Compute the dot product u⃗⋅v⃗\vec{u} \cdot \vec{v}.

Using the distributive property of the dot product:

u⃗⋅v⃗=(∣a⃗∣b⃗+∣b⃗∣a⃗)⋅(∣a⃗∣b⃗−∣b⃗∣a⃗)\vec{u} \cdot \vec{v} = \big(|\vec{a}|\vec{b} + |\vec{b}|\vec{a}\big) \cdot \big(|\vec{a}|\vec{b} - |\vec{b}|\vec{a}\big)

This expands as:

=(∣a⃗∣b⃗)⋅(∣a⃗∣b⃗)  −  (∣a⃗∣b⃗)⋅(∣b⃗∣a⃗)  +  (∣b⃗∣a⃗)⋅(∣a⃗∣b⃗)  −  (∣b⃗∣a⃗)⋅(∣b⃗∣a⃗)= (|\vec{a}|\vec{b})\cdot(|\vec{a}|\vec{b}) \;-\; (|\vec{a}|\vec{b})\cdot(|\vec{b}|\vec{a}) \;+\; (|\vec{b}|\vec{a})\cdot(|\vec{a}|\vec{b}) \;-\; (|\vec{b}|\vec{a})\cdot(|\vec{b}|\vec{a})

3. Factor out the scalar coefficients.

Remember that for any scalars p,qp, q and vectors x⃗,y⃗\vec{x}, \vec{y}, we have (px⃗)⋅(qy⃗)=pq(x⃗⋅y⃗)(p\vec{x})\cdot(q\vec{y}) = pq (\vec{x}\cdot\vec{y}). Applying this:

  • First term: (∣a⃗∣b⃗)⋅(∣a⃗∣b⃗)=∣a⃗∣2(b⃗⋅b⃗)=∣a⃗∣2∣b⃗∣2(|\vec{a}|\vec{b})\cdot(|\vec{a}|\vec{b}) = |\vec{a}|^2 (\vec{b}\cdot\vec{b}) = |\vec{a}|^2 |\vec{b}|^2
  • Second term: (∣a⃗∣b⃗)⋅(∣b⃗∣a⃗)=∣a⃗∣∣b⃗∣(b⃗⋅a⃗)(|\vec{a}|\vec{b})\cdot(|\vec{b}|\vec{a}) = |\vec{a}||\vec{b}| (\vec{b}\cdot\vec{a})
  • Third term: (∣b⃗∣a⃗)⋅(∣a⃗∣b⃗)=∣b⃗∣∣a⃗∣(a⃗⋅b⃗)(|\vec{b}|\vec{a})\cdot(|\vec{a}|\vec{b}) = |\vec{b}||\vec{a}| (\vec{a}\cdot\vec{b})
  • Fourth term: (∣b⃗∣a⃗)⋅(∣b⃗∣a⃗)=∣b⃗∣2(a⃗⋅a⃗)=∣b⃗∣2∣a⃗∣2(|\vec{b}|\vec{a})\cdot(|\vec{b}|\vec{a}) = |\vec{b}|^2 (\vec{a}\cdot\vec{a}) = |\vec{b}|^2 |\vec{a}|^2

So: …

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