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Exercise 6.3 · Q23

Q.Prove that the volume of the largest cone that can be inscribed in a sphere of radius RR is 827\frac{8}{27} of the volume of the sphere.

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Appeared in past exams:AP EAPCET 2023· Set eng-2023-05-19-FN· 1mreworded
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The largest cone inscribed in a sphere has its height equal to 4R3\frac{4R}{3} and base radius 22R3\frac{2\sqrt{2}R}{3}, giving volume 3281πR3\frac{32}{81}\pi R^3, which is exactly 827\frac{8}{27} of the sphere’s volume 43πR3\frac{4}{3}\pi R^3.

This is a classic optimization problem: you have a fixed sphere, and you want to fit the biggest possible cone inside it. The cone must touch the sphere’s surface at its base circumference and at its apex. The key insight is that the cone’s dimensions are not independent — they are linked by the geometry of the sphere. Once you express the cone’s volume in terms of a single variable (like its height), you can use calculus to find the maximum.

Let’s work through it step by step.


1. Set up the geometry

Imagine a sphere of radius RR. Place the cone so that its apex is at the top of the sphere and its base is a circle somewhere below. The axis of the cone passes through the centre of the sphere. Let the height of the cone be hh, measured from the apex to the centre of the base. The centre of the sphere lies somewhere along this axis.

If the apex is at the top, the centre of the sphere is at a distance RR from the apex. The base of the cone is at a distance hh from the apex. So the distance from the sphere’s centre to the base plane is h−Rh - R (since h>Rh > R for a cone that fits inside).

2. Relate base radius to height

The base of the cone is a circle of radius rr. This circle lies on the sphere’s surface, so every point on its circumference is at distance RR from the sphere’s centre. The centre of the base is at a distance h−Rh - R from the sphere’s centre. By the Pythagorean theorem in the vertical cross-section:

r2+(h−R)2=R2r^2 + (h - R)^2 = R^2

So:

r2=R2−(h−R)2=R2−(h2−2hR+R2)=2hR−h2r^2 = R^2 - (h - R)^2 = R^2 - (h^2 - 2hR + R^2) = 2hR - h^2

Thus:

r=2hR−h2r = \sqrt{2hR - h^2}

This is valid only when 2hR−h2≥02hR - h^2 \ge 0, i.e. 0≤h≤2R0 \le h \le 2R. The cone’s height cannot exceed the sphere’s diameter.

3. Write the volume of the cone

Volume of a cone is V=13πr2hV = \frac{1}{3}\pi r^2 h. Substitute r2r^2:

V(h)=13π(2hR−h2)h=13π(2h2R−h3)V(h) = \frac{1}{3}\pi (2hR - h^2) h = \frac{1}{3}\pi (2h^2 R - h^3)

So:

V(h)=π3(2Rh2−h3)V(h) = \frac{\pi}{3} (2R h^2 - h^3)

We need to maximise this for hh in (0,2R)(0, 2R).

4. Differentiate and find critical points

Differentiate with respect to hh:

V′(h)=π3(4Rh−3h2)=π3h(4R−3h)V'(h) = \frac{\pi}{3} (4R h - 3h^2) = \frac{\pi}{3} h (4R - 3h)

Set V′(h)=0V'(h) = 0:

h(4R−3h)=0h (4R - 3h) = 0

So h=0h = 0 (minimum, degenerate cone) or h=4R3h = \frac{4R}{3}.

Since h=4R3h = \frac{4R}{3} lies in (0,2R)(0, 2R), it is a valid candidate.

5. Confirm it’s a maximum

Check the second derivative:

V′′(h)=π3(4R−6h)V''(h) = \frac{\pi}{3} (4R - 6h)

At h=4R3h = \frac{4R}{3}:

V′′(4R3)=π3(4R−6⋅4R3)=π3(4R−8R)=−4πR3<0V''\left(\frac{4R}{3}\right) = \frac{\pi}{3} \left(4R - 6\cdot\frac{4R}{3}\right) = \frac{\pi}{3} (4R - 8R) = -\frac{4\pi R}{3} < 0

So it is indeed a maximum. …

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