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Exercise 6.3 · Q25

Q.Show that the semi-vertical angle of the cone of the maximum volume and of given slant height is tan⁡−12\tan^{-1}\sqrt{2}.

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For a cone with fixed slant height ll, the volume is maximised when the semi-vertical angle θ\theta satisfies tan⁡θ=2\tan \theta = \sqrt{2}. This is found by expressing volume in terms of θ\theta, differentiating, and setting the derivative to zero.

We have a cone with a fixed slant height ll. The slant height is the distance from the apex to any point on the circular base, measured along the sloping surface. The semi-vertical angle θ\theta is the angle between the axis (height) and the slant height. Our job: find θ\theta that gives the largest possible volume.

Why does this work? In optimisation problems with a constraint (here, fixed ll), we express the quantity to be maximised — volume — in terms of a single variable. The slant height ties the radius rr and height hh together via l2=r2+h2l^2 = r^2 + h^2. So we can write rr and hh in terms of θ\theta and ll, then volume becomes a function of θ\theta alone. Differentiate, set to zero, and check it's a maximum.

Let's go step by step.


1. Relate the cone's dimensions to θ\theta and ll

In a right circular cone, the semi-vertical angle θ\theta is at the apex, between the axis (height hh) and the slant height ll. So:

  • sin⁡θ=rl\sin \theta = \frac{r}{l} → r=lsin⁡θr = l \sin \theta
  • cos⁡θ=hl\cos \theta = \frac{h}{l} → h=lcos⁡θh = l \cos \theta

These follow directly from the right triangle formed by rr, hh, and ll.


2. Write the volume in terms of θ\theta

Volume of a cone: V=13πr2hV = \frac{1}{3} \pi r^2 h

Substitute rr and hh:

V(θ)=13π(lsin⁡θ)2(lcos⁡θ)=13πl3sin⁡2θcos⁡θV(\theta) = \frac{1}{3} \pi (l \sin \theta)^2 (l \cos \theta) = \frac{1}{3} \pi l^3 \sin^2 \theta \cos \theta

Since ll is constant, maximising VV is equivalent to maximising f(θ)=sin⁡2θcos⁡θf(\theta) = \sin^2 \theta \cos \theta.

Tip

Ignoring constant factors (13πl3\frac{1}{3}\pi l^3) simplifies differentiation — the location of the maximum is unchanged.


3. Differentiate f(θ)f(\theta) and set to zero

Let f(θ)=sin⁡2θcos⁡θf(\theta) = \sin^2 \theta \cos \theta. Use the product rule:

f′(θ)=(2sin⁡θcos⁡θ)cos⁡θ+sin⁡2θ(−sin⁡θ)f'(\theta) = (2 \sin \theta \cos \theta) \cos \theta + \sin^2 \theta (-\sin \theta)

Simplify:

f′(θ)=2sin⁡θcos⁡2θ−sin⁡3θf'(\theta) = 2 \sin \theta \cos^2 \theta - \sin^3 \theta

Factor out sin⁡θ\sin \theta:

f′(θ)=sin⁡θ (2cos⁡2θ−sin⁡2θ)f'(\theta) = \sin \theta \, (2 \cos^2 \theta - \sin^2 \theta)

For a maximum in (0,π2)(0, \frac{\pi}{2}), set f′(θ)=0f'(\theta) = 0. sin⁡θ≠0\sin \theta \neq 0 (since θ>0\theta > 0), so:

2cos⁡2θ−sin⁡2θ=02 \cos^2 \theta - \sin^2 \theta = 0


4. Solve for θ\theta …

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