Sphere Inscribed in Two Cones

Calculus Level 5

Shown to the right is a sphere inscribed in two congruent cones attached by their bases.

If the volume of the two cones combined is V , V, the maximum possible volume of the sphere can be expressed as a b c V , \frac{a\sqrt b}{c}V, where a , b , a, b, and c c are positive integers such that the root and fraction are in their simplest forms.

Find a + b + c . a+b+c.


The answer is 16.

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1 solution

Joseph Newton
Dec 30, 2017

In this proof, I will refer to:

  • the volume of the sphere as v v ,
  • the radius of the sphere as r r ,
  • the volume of the two cones as V V as given in the question,
  • the radius of the base of the cones as s s (because r r is already taken), and
  • the height of each cone as h h .

First, we will get the dimensions of the sphere in terms of a single variable s s .

From the formula for the volume of a cone: V = 2 × ( 1 3 π s 2 h ) h = 3 V 2 π s 2 V=2\times\left(\frac{1}{3}\pi s^2 h\right)\\ h=\frac{3V}{2\pi s^2} Shown here is a cross-section of part of the sphere and cones: We can easily prove that A B D \triangle ABD is similar to A D C \triangle ADC , because of the right angle and that C A D \angle CAD is common.

A C = s 2 + h 2 AC=\sqrt{s^2+h^2} from the Pythagorean theorem, and we can now use the rule that corresponding sides in similar triangles are in the same ratio: B D A D = D C A C r h = s s 2 + h 2 r = s h s 2 + h 2 r = s 3 V 2 π s 2 s 2 + ( 3 V 2 π s 2 ) 2 r = 3 V s 4 π 2 s 6 + 9 V 2 \begin{aligned}\frac{BD}{AD}&=\frac{DC}{AC}\\ \frac{r}{h}&=\frac{s}{\sqrt{s^2+h^2}}\\ r&=\frac{sh}{\sqrt{s^2+h^2}}\\ r&=\frac{s\frac{3V}{2\pi s^2}}{\sqrt{s^2+\left(\frac{3V}{2\pi s^2}\right)^2}}\\ r&=\frac{3Vs}{\sqrt{4\pi^2s^6+9V^2}}\end{aligned} Intuitively, the maximum possible radius of the sphere would give the maximum possible volume as well, so we can now do calculus to our r r variable. and substitute it into the formula for the volume of a sphere later. To do maxima and minima, we have to take the derivative, using the quotient and chain rules: d r d s = 3 V ( 4 π 2 s 6 + 9 V 2 s 1 2 1 4 π 2 s 6 + 9 V 2 ( 24 π 2 s 5 ) 4 π 2 s 6 + 9 V 2 ) = 3 V ( ( 4 π 2 s 6 + 9 V 2 ) s 1 2 ( 24 π 2 s 5 ) ( 4 π 2 s 6 + 9 V 2 ) 4 π 2 s 6 + 9 V 2 ) = 3 V ( 4 π 2 s 6 + 9 V 2 12 π 2 s 6 ( 4 π 2 s 6 + 9 V 2 ) 3 ) = 3 V ( 9 V 2 8 π 2 s 6 ( 4 π 2 s 6 + 9 V 2 ) 3 ) \begin{aligned}\frac{dr}{ds}&=3V\left(\frac{\sqrt{4\pi^2s^6+9V^2}-s\frac{1}{2}\frac{1}{\sqrt{4\pi^2s^6+9V^2}}\left(24\pi^2s^5\right)}{4\pi^2s^6+9V^2}\right)\\ &=3V\left(\frac{\left(4\pi^2s^6+9V^2\right)-s\frac{1}{2}\left(24\pi^2s^5\right)}{\left(4\pi^2s^6+9V^2\right)\sqrt{4\pi^2s^6+9V^2}}\right)\\ &=3V\left(\frac{4\pi^2s^6+9V^2-12\pi^2s^6}{\sqrt{\left(4\pi^2s^6+9V^2\right)^3}}\right)\\ &=3V\left(\frac{9V^2-8\pi^2s^6}{\sqrt{\left(4\pi^2s^6+9V^2\right)^3}}\right)\end{aligned} Now we let the derivative equal zero to find a maximum or minimum turning point. The bottom of the fraction is irrelevant for this: 3 V ( 9 V 2 8 π 2 s 6 ( 4 π 2 s 6 + 9 V 2 ) 3 ) = 0 9 V 2 8 π 2 s 6 = 0 s 6 = 9 V 2 8 π 2 s 3 = 3 V 2 2 π s = 3 V 2 2 π 3 \begin{aligned}3V\left(\frac{9V^2-8\pi^2s^6}{\sqrt{\left(4\pi^2s^6+9V^2\right)^3}}\right)&=0\\ 9V^2-8\pi^2s^6&=0\\ s^6&=\frac{9V^2}{8\pi^2}\\ s^3&=\frac{3V}{2\sqrt2\pi}\\ s&=\sqrt[3]{\frac{3V}{2\sqrt2\pi}}\end{aligned} If we let V V equal a manageable number like 1 1 , We can now check whether this is a maximum or minimum by doing a first derivative test:

Let V = 1 V=1 , s = 3 2 2 π 3 = 0.6963 ∴s=\sqrt[3]{\frac{3}{2\sqrt2\pi}}=0.6963\dots

s s 0.6000 0.6963 0.7000
d r d s \frac{dr}{ds} 0.4467 0.0000 -0.0172

Since the function is increasing when s < 3 V 2 2 π 3 s<\sqrt[3]{\frac{3V}{2\sqrt2\pi}} and decreasing when s > 3 V 2 2 π 3 s>\sqrt[3]{\frac{3V}{2\sqrt2\pi}} , we can conclude that s = 3 V 2 2 π 3 s=\sqrt[3]{\frac{3V}{2\sqrt2\pi}} is a maximum turning point.

Now that we know that s = 3 V 2 2 π 3 s=\sqrt[3]{\frac{3V}{2\sqrt2\pi}} gives us the maximum radius of the sphere, we can now substitute this into our radius formula: r = 3 V s 4 π 2 s 6 + 9 V 2 = 3 V 3 V 2 2 π 3 4 π 2 ( 3 V 2 2 π 3 ) 6 + 9 V 2 = 3 V 3 V 2 2 π 3 4 π 2 ( 9 V 2 8 π 2 ) + 9 V 2 = 3 V 3 V 2 2 π 3 3 V 1 2 + 1 = 3 V 2 2 π 3 3 2 = 3 V 2 2 π 3 × 2 2 3 3 3 r = V π 3 3 \begin{aligned}r&=\frac{3Vs}{\sqrt{4\pi^2s^6+9V^2}}\\ &=\frac{3V\sqrt[3]{\frac{3V}{2\sqrt2\pi}}}{\sqrt{4\pi^2\left(\sqrt[3]{\frac{3V}{2\sqrt2\pi}}\right)^6+9V^2}}\\ &=\frac{3V\sqrt[3]{\frac{3V}{2\sqrt2\pi}}}{\sqrt{4\pi^2\left(\frac{9V^2}{8\pi^2}\right)+9V^2}}\\ &=\frac{3V\sqrt[3]{\frac{3V}{2\sqrt2\pi}}}{3V\sqrt{\frac{1}{2}+1}}\\ &=\frac{\sqrt[3]{\frac{3V}{2\sqrt2\pi}}}{\sqrt{\frac{3}{2}}}\\ &=\sqrt[3]{\frac{3V}{2\sqrt2\pi}}\times\sqrt[3]{\frac{2\sqrt2}{3\sqrt3}}\\ r&=\sqrt[3]{\frac{V}{\pi\sqrt3}}\end{aligned} Finally, we can use the formula for the volume of a sphere: v = 4 3 π r 3 = 4 3 π ( V π 3 3 ) 3 = 4 3 π V π 3 = 4 3 3 V = 4 3 9 V \begin{aligned}v&=\frac{4}{3}\pi r^3\\ &=\frac{4}{3}\pi\left(\sqrt[3]{\frac{V}{\pi\sqrt3}}\right)^3\\ &=\frac{4}{3}\pi\frac{V}{\pi\sqrt3}\\ &=\frac{4}{3\sqrt3}V\\ &=\frac{4\sqrt3}{9}V\end{aligned} So a = 4 a=4 , b = 3 b=3 and c = 9 c=9 , so the answer is 4 + 3 + 9 = 16 4+3+9=\boxed{16}

It's much simpler if you eliminate the constant V V in your working from the start.

Here's how I would have done it:

Without the loss of generality, let V = 2 3 π V = \dfrac23 \pi , then we can get s 2 h = 1 s^2 h = 1 \qquad \bigstar .

And from your line: r h = s s 2 + h 2 \dfrac rh = \dfrac s{\sqrt{s^2 + h^2}} , we can get

r h = s 1 / h + h 2 r 2 h 2 = s 2 1 / h + h 2 = s 2 h h 3 + 1 = 1 h 3 + 1 r 2 = h 2 h 3 + 1 . \dfrac rh = \dfrac s{ \sqrt{1/h + h^2} } \quad \Leftrightarrow \quad \dfrac{r^2}{h^2} = \dfrac{s^2}{1/h + h^2} = \dfrac{s^2 h}{h^3 + 1} = \dfrac1{h^3 + 1} \quad \Leftrightarrow \quad r^2 = \dfrac{h^2}{h^3 + 1} .

Then differentiating r = ( h 2 h 3 + 1 ) 1 / 2 r= \left(\dfrac{h^2}{h^3 + 1} \right)^{1/2} gives d r d h h ( h 3 2 ) 2 h 2 / ( h 3 + 1 ) ( h 3 + 1 ) 2 \dfrac{dr}{dh} - \dfrac{h(h^3 - 2)}{2 \sqrt{h^2/(h^3+1)} (h^3 + 1)^2} .

When at critical point, d r d h = 0 \dfrac{dr}{dh} = 0 , so h = 2 1 / 3 h = 2^{1/3} .

The rest should follow.

Pi Han Goh - 3 years, 5 months ago

Another approach could be to parametrise this problem in terms of the angle CAD (let it be denoted as θ \theta ) in your diagram. Letting the radius of the sphere be r r , we have CD is r cos θ \frac{r}{\cos\theta} and AD is r sin θ \frac{r}{\sin\theta} . Then the volume of the two cones combined is V = 2 π r 3 3 cos 2 θ sin θ V = \frac{2 \pi r^3}{3\cos^2\theta \sin\theta} . Since the volume of the sphere is V s p h e r e = 4 3 π r 3 V_{sphere} = \frac{4}{3} \pi r^3 , we can substitute in the expression for V to obtain V s p h e r e = 2 V cos 2 θ sin θ V_{sphere} = 2V\cos^2\theta \sin\theta and we can differentiate with respect to θ \theta to obtain the answer. (Remembering that 0 < θ < π / 2 0<\theta<\pi/2 )

John Frank - 3 years ago

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