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NCERT Exemplar · Q21

Q.ABAB is a diameter of a circle and CC is any point on the circle. Show that the area of △ABC\triangle ABC is maximum when it is isosceles.

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Let the circle have radius rr, so AB=2rAB = 2r is fixed. Writing ∠CAB=θ\angle CAB = \theta, the right angle at CC (Thales' theorem) gives AC=2rcos⁡θAC = 2r\cos\theta and BC=2rsin⁡θBC = 2r\sin\theta, so the area is Δ(θ)=r2sin⁡2θ\Delta(\theta) = r^2\sin2\theta — a single-variable function of θ\theta. Differentiating and testing shows this is maximum at θ=π4\theta = \dfrac{\pi}{4}, where AC=BC=r2AC = BC = r\sqrt2, i.e. the triangle is isosceles.

Setting up

Let the circle have radius rr, so the diameter AB=2rAB = 2r is a fixed length (the circle itself doesn't change — only the position of CC on it does). Let CC be any point on the circle, and let ∠CAB=θ\angle CAB = \theta, where θ\theta can range over (0,π2)\left(0, \dfrac{\pi}{2}\right) as CC moves around the semicircle.

Since ABAB is a diameter and CC lies on the circle, the angle in a semicircle is a right angle (Thales' theorem):

∠ACB=90∘.\angle ACB = 90^\circ.

So △ABC\triangle ABC is always right-angled at CC, with the fixed segment ABAB as its hypotenuse.

Step 1 — Express the legs in terms of θ\theta

In this right triangle, with hypotenuse AB=2rAB = 2r and angle θ\theta at AA:

AC=ABcos⁡θ=2rcos⁡θ,BC=ABsin⁡θ=2rsin⁡θ.AC = AB\cos\theta = 2r\cos\theta, \qquad BC = AB\sin\theta = 2r\sin\theta.

This turns the problem into a single-variable optimization in θ\theta — no partial derivatives or multiple constraints are needed.

Step 2 — Write the area as a function of θ\theta

Δ(θ)=12⋅AC⋅BC=12(2rcos⁡θ)(2rsin⁡θ)=2r2sin⁡θcos⁡θ=r2sin⁡2θ.\Delta(\theta) = \frac{1}{2}\cdot AC \cdot BC = \frac{1}{2}(2r\cos\theta)(2r\sin\theta) = 2r^2\sin\theta\cos\theta = r^2\sin2\theta.

Step 3 — Differentiate and find the critical point

dΔdθ=r2⋅2cos⁡2θ=2r2cos⁡2θ.\frac{d\Delta}{d\theta} = r^2 \cdot 2\cos2\theta = 2r^2\cos2\theta.

Setting dΔdθ=0\dfrac{d\Delta}{d\theta} = 0:

cos⁡2θ=0⇒2θ=π2(since θ∈(0,π2)⇒2θ∈(0,π))\cos2\theta = 0 \quad\Rightarrow\quad 2\theta = \frac{\pi}{2} \quad (\text{since } \theta \in (0, \tfrac{\pi}{2}) \Rightarrow 2\theta \in (0,\pi))

⇒ θ=π4.\Rightarrow\ \theta = \frac{\pi}{4}.

Step 4 — Confirm it's a maximum

d2Δdθ2=−4r2sin⁡2θ.\frac{d^2\Delta}{d\theta^2} = -4r^2\sin2\theta. …

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