What Fraction of The Volume was Removed?

Calculus Level 5

A right circular cone is cut into two pieces by a cutting plane that passes through the center of the base and is angled in such a way to generate a parabolic cut. The figure above shows the truncated cone. Find the ratio of the volume of the (smaller) piece that was removed (shown below), relative to the volume of the entire cone. If the ratio is F F , then enter 10000 F \lfloor 10000 F \rfloor . For example if the ratio is 0.23178391, the answer is 2317

2877 2516 2634 2793

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1 solution

Hosam Hajjir
Mar 26, 2018

Method 1:

Let the radius of the base be R R and the height be h h , then the semi-vertical angle θ c \theta_c is given by

θ c = tan 1 R h \theta_c = \tan^{-1} \dfrac{R}{h}

If the origin is at the apex of the cone, then we can take the cutting plane to be n ( r r 0 ) = 0 \vec{n} \cdot ( \vec{r} - \vec{r_0} ) = 0 where the normal vector n \vec{n} is

orthogonal to the cutting plane which is parallel to ( \sin \theta c, 0, \cos \theta c ), hence we can take

n = ( cos θ c , 0 , sin θ c ) \vec{n} = (-\cos \theta_c, 0, \sin \theta_c )

Now we'll slice the removed volume into slices parallel to the cutting plane, intersecting the base at x, and the volume will be

V = 0 t m a x A ( t ) d t V = \displaystyle \int_{0}^{t_{max}} A(t) dt

the parameter t t represents the distance of the slice from the cutting plane

such that it is zero at x = 0 x = 0 , and t = t m a x t = t_{max} at x = R x = -R .

With the definition of the normal vector above, we can represent the slice in vector form as

r = V u + r 0 r = V u + r_0 with

u = ( u 1 , u 2 ) u = (u_1, u_2) is the coordinate of r r with respect the two vectors in matrix V V which

are, respectively, (\sin \theta c, 0, \cos \theta c) and (0, 1, 0). And r 0 = ( x , 0 , h ) r_0 = (x, 0, h )

\( t is the distance of the slice plane from the cutting plane along the normal to the cutting plane,

hence, t = \vec{n} \cdot ( (x, 0, h) - (0, 0, h) ) = -( \cos \theta_c ) x

Next, we have to find the equation the parabola in the plane of the slice. For that we need the equation of

the cone, which is \( r^T Q r = 0 \), where Q = diag { cos 2 θ c , cos 2 θ c , s i n 2 θ c } Q = \text{diag} \{ \cos^2 \theta_c , \cos^2 \theta_c, -sin^2 \theta_c \} .

Substituting r = V u + r 0 r = V u + r_0 into the equation of the cone, results in

( V u + r 0 ) T Q ( V u + r 0 ) = 0 (V u + r_0)^T Q (V u + r_0) = 0

which when expanded becomes,

u T V T Q V u + 2 u T V T Q r 0 + r 0 T Q r 0 = 0 u^T V^T Q V u + 2 u^T V^T Q r_0 + {r_0}^T Q r_0 = 0

If use the notation c = cos θ c c = \cos \theta_c and s = sin θ c s = \sin \theta_c , then

V T Q V = [ s 0 c 0 1 0 ] [ c 2 0 0 0 c 2 0 0 0 s 2 ] [ s 0 0 1 c 0 ] V^T Q V = \begin{bmatrix} s && 0 && c \\ 0 && 1 && 0 \end{bmatrix} \begin{bmatrix} c^2 && 0 && 0 \\ 0 && c^2 && 0 \\ 0 && 0 && -s&^2 \end{bmatrix} \begin{bmatrix} s && 0 \\ 0 && 1 \\ c && 0 \end{bmatrix}

Evaluating the right-hand side, results in

V T Q V = [ 0 0 0 c 2 ] V^T Q V = \begin{bmatrix} 0 && 0 \\ 0 && c^2 \end{bmatrix}

In a similar fashion, we have

V T Q r 0 = [ s c ( x c s h ) 0 ] V^T Q r_0 = \begin{bmatrix} sc(xc - sh) \\ 0 \end{bmatrix}

and

r 0 T Q r 0 = c 2 x 2 s 2 h 2 {r_0}^T Q r_0 = c^2 x^2 - s^2 h^2

Therefore, the equation of the parabola is

c 2 u 2 2 + 2 u 1 s c ( x c s h ) + c 2 x 2 s 2 h 2 = 0 c^2 {u_2}^2 + 2 u_1 s c (x c - s h) + c^2 x^2 - s^2 h^2 = 0

Solving for the independent variable ( u 1 u_1 ) in terms of the dependent variable ( u 2 u_2 ), we have

u 1 = x c + s h 2 s c + c 2 s ( s h x c ) u 2 2 u_1 = - \dfrac{xc + sh}{2 sc} + \dfrac{c}{2 s(sh - xc)} {u_2}^2

Note that ( s h x c ) = c ( h tan θ c x ) = c ( R x ) ( sh - xc) = c ( h \tan \theta_c - x ) = c ( R - x ) and similarly, (sh + xc) = c (x + R) )

Since R < x < 0 -R < x < 0 , both terms are positive. The end points of the parabola corresponds to u 1 = 0 u_1 = 0 and are at

u 2 = a u_2 = -a and u 2 = a u_2 = a , where a = ( s 2 h 2 c 2 x 2 ) c 2 = R 2 x 2 a =\sqrt{ \dfrac{(s^2 h^2 - c^2 x^2) }{c^2}} = \sqrt{ R^2 - x^2 } .

Since the parabola is below the u 2 u_2 axis, the area is the negative of the integral between a -a and a a .

Performing the integral, results in,

A = x + R s R 2 x 2 1 3 ( R 2 x 2 ) ( 3 / 2 ) s ( R x ) A = \dfrac{ x + R }{ s } \sqrt{R^2 - x^2} - \dfrac{1}{3} \dfrac{ (R^2 - x^2)^(3/2) }{ s(R - x) }

Simplifying,

A = 2 3 ( 1 s ) ( x + R ) R 2 x 2 A = \dfrac{2}{3} ( \dfrac{1}{s} ) (x + R) \sqrt{R^2 - x^2}

Recall that the perpendicular distance of the slice from the cut is t = ( cos θ c ) x t = (-\cos \theta_c) x , hence we can substitute for

t t in the volume integral, and integrate with respect to x instead.

V = t = 0 t = ( cos θ c ) R A ( t ) d t = cos θ c x = R x = 0 A ( x ) d x V = \displaystyle \int_{t = 0 }^{t = (\cos \theta_c) R} A(t) dt = \displaystyle \cos \theta_c \int_{x = -R}^{x = 0} A(x) dx

The last integral is easy to perform, and is given by

2 c 3 s ( 1 3 R 3 + R 3 π 4 ) = 1 3 π R 2 h ( 1 2 2 3 π ) \dfrac{2c}{3s} ( \dfrac{-1}{3} R^3 + R^3 \dfrac{\pi}{4} ) = \dfrac{1}{3} \pi R^2 h ( \dfrac{1}{2} - \dfrac{2}{3 \pi})

where in the last step we used the fact that R = h tan θ c R = h \tan \theta_c .

The factor we're looking for is ( 1 2 2 3 π ) ( \dfrac{1}{2} - \dfrac{2}{3 \pi}) which numerically evaluates to 0.28779341 0.28779341 , making the answer 2877 \boxed{2877} .

Method 2:

Here we will take the slices parallel to the base, one such slice is shown in the figure above with a red line segment. The slice take the shape of the red region with the circle on the bottom left.

The cut is at, x = ( tan θ c ) ( h z ) = R ( 1 z / h ) x = (\tan \theta_c) (h - z) = R (1 - z/h)

The radius of circle of cut, r = z tan θ c = z R / h r = z \tan \theta_c = z R / h

Area of cut, A = 1 / 2 r 2 ( 2 t sin 2 t ) A = 1/2 r^2 (2t - \sin 2 t)

where t = cos 1 ( x / r ) t = \cos^{-1} ( x / r )

Therefore,

A ( z ) = 1 / 2 ( z R / h ) 2 ( 2 cos 1 ( h z z ) sin ( 2 cos 1 ( h z z ) ) ) A(z) = 1/2 (z R / h)^2 ( 2 \cos^{-1}( \dfrac{h - z}{z} ) - \sin ( 2 \cos^{-1}(\dfrac{h-z}{z} ) ) )

The required volume, V = z = h / 2 h A ( z ) d z V = \displaystyle \int_{z = h/2}^{h} A(z) dz

To normalize the volume integral, we set u = z / h u = z / h , then

V = R 2 h u = 1 2 1 1 2 u 2 ( 2 cos 1 ( 1 u u ) sin ( 2 cos 1 ( 1 u u ) ) ) d u V = R^2 h \displaystyle \int_{u = \frac{1}{2}}^{1} \dfrac{1}{2} u^2 ( 2 \cos^{-1}( \dfrac{1 - u}{u} ) - \sin ( 2 \cos^{-1}(\dfrac{1-u}{u} ) ) ) du

Evaluating the integral numerically, it comes to, 0.3013765533760

Dividing by 1 3 π \dfrac{1}{3} \pi gives the required ratio, 0.28779341 0.28779341

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