Tilted conical cup - new water depth

Geometry Level pending

A water cup is in the shape of a conical frustrum with bottom diameter 4 4 cm, and top diameter 8 8 cm, and slant height 10 10 cm. It is filled to half its height with water, then the cup is tilted by 3 0 30^{\circ} . Find the new depth (in centimeters) of water in the tilted cup (this is d 2 d_2 in the image above, drawn to scale). If the new depth is denoted by d d then find 1 0 3 d \lfloor 10^3 d \rfloor

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Details and Assumptions:

  • You may need the following formulas for the semi-minor and semi-major axes lengths of the water surface ellipse.

Semi-minor axis length = a = z 0 tan θ cos ϕ 1 sin 2 ϕ sec 2 θ \text{Semi-minor axis length } = a = \dfrac { z_0 \tan \theta \cos \phi}{\sqrt{1 - \sin^2 \phi \sec^2 \theta} }

Semi-major axis length = b = z 0 tan θ cos ϕ 1 sin 2 ϕ sec 2 θ \text{Semi-major axis length } = b = \dfrac { z_0 \tan \theta \cos \phi}{1 - \sin^2 \phi \sec^2 \theta}

Where z 0 z_0 is the distance between the apex and the intersection point of the axis with the intercepting plane. θ \theta is the semi-vertical angle of the cone, i.e. the angle between the axis of the cone and its surface. Finally, ϕ \phi is the acute angle between the axis of the cone and the normal vector to the intersecting plane. For completeness (although you won't need this in this problem), the distance between the center of the ellipse and the point where the axis of the cone meets the cutting plane is given by v 0 v_0 ,

v 0 = z 0 sin ϕ tan 2 θ 1 sin 2 ϕ sec 2 θ v_0 = \dfrac{z_0 \sin \phi \tan^2 \theta}{1 - \sin^2 \phi \sec^2 \theta}

These formulas were derived in the solution of this problem .


The answer is 5153.

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2 solutions

This is a follow-up of my solution of the previous problem . Refer to my previous solution to understand better the calculations in this solution.

First we find the volume of the half-filled water tumbler, V 1 2 = 2 6 π 3 ( 6 3 2 3 ) 97.47378709 V_\frac 12 = \frac {2\sqrt 6\pi}3(6^3-2^3) \approx 97.47378709 . Now we align the axis of the tumbler along the x x -axis with its bottom along the z z -axis. We note that the radius of the cross-section circle of the tumbler is given by r ( x ) = m x + 2 r(x) = mx + 2 , where m = 1 24 m=\frac 1{\sqrt{24}} . The volume of the water V ( x ) V(x) is the sum of the volume of a frustrum V 1 ( x ) V_1(x) and the volume of a "wedge" V 2 ( x ) V_2(x) . The volume of the frustrum is given by V 1 ( x ) = 2 6 π 3 ( r 1 ( x ) 3 2 3 ) V_1(x) = \frac {2\sqrt 6\pi}3(r_1(x)^3 - 2^3) , where r 1 ( x ) r_1(x) is the base radius of the frustrum.

For the volume of the wedge V 2 ( x ) V_2(x) , we can make use of the result of the previous problem. Using the farthest point of the wedge from the z z -axis as the reference for x x , at x = 4 6 x=4\sqrt 6 or at the brim of the tumbler, the water poured out when the tumbler is tilted at 3 0 30^\circ is found to be V o u t 98.1614004197936 V_{\rm out}\approx 98.1614004197936 . The width of the wedge l ( 4 6 ) = 16 6 1 + 6 2 l(4\sqrt 6) = \frac {16\sqrt 6}{1+6\sqrt 2} . This means that V 2 ( 4 6 ) = V 1 ( 4 6 ) V 1 ( 4 6 l ( 4 6 ) ) V o u t 68.81430502 V_2(4\sqrt 6) = V_1(4\sqrt 6) - V_1(4\sqrt 6 - l(4\sqrt 6)) - V_{\rm out} \approx 68.81430502 (volume of a frustrum with height l l minus the volume of water poured out). We note that the shape of the wedge does not change with x x , therefore V 2 ( x ) V_2(x) is directly proportional to r ( x ) 3 r(x)^3 . Therefore we can find V 2 ( x ) = ( r ( x ) 4 ) 3 V 2 ( 4 6 ) V_2(x) = \left(\frac {r(x)}4\right)^3 V_2(4\sqrt 6) .

Using the x x -coordinate of the wedge's farthest end from the z z -axis, the base radius of the frustrum r 1 ( x ) = m ( x l ( x ) ) + 2 r_1(x) = m(x-l(x))+2 , where l ( x ) = 4 r ( x ) 6 1 + 6 2 l(x) = \frac {4r(x)\sqrt 6}{1+6\sqrt 2} . And the final formula is

V ( x ) = 2 6 π ( x l ( x ) ) 3 8 ) 3 + r ( x ) 3 V 2 ( 4 6 ) 64 V(x) = \frac {2\sqrt 6\pi (x-l(x))^3 - 8)}3 + \frac {r(x)^3 V_2(4\sqrt 6)}{64}

We have to find the value of x x , when V ( x ) = V 1 2 V(x) = V_\frac 12 . As you can see the computation is very complex, I used a Microsoft Excel spreadsheet and manual iterations. The required x 1 6.746320373 x_1 \approx 6.746320373 and the required d = 5 2 6 ( 2 6 5 × 3 2 1 5 × 1 2 ) x 1 5.153941385 d = \frac 5{2\sqrt 6} \left(\frac {2\sqrt 6}5 \times \frac {\sqrt 3}2 - \frac 15 \times \frac 12 \right)x_1 \approx 5.153941385 . Therefore 1 0 3 d = 5153 \lfloor 10^3 d \rfloor = \boxed{5153} .

Hosam Hajjir
Oct 31, 2020

We are given that the bottom radius is r 1 = 2 r_1 = 2 and the top radius is r 2 = 4 r_2 = 4 and the slant height is s = 10 s = 10 , hence the height h = s 2 ( r 2 r 1 ) 2 = 96 h = \sqrt{s^2 - (r_2 - r_1)^2 } = \sqrt{96}

The radius of the water surface before tilting is r 0 = 1 2 ( r 1 + r 2 ) = 3 r_0 = \frac{1}{2} (r_1 + r_2) = 3 , And from similar triangles, we deduce that height of the cone underneath the water surface is 3 2 h \frac{3}{2} h .

Hence, the original volume of the whole cone underneath the water plane is

V 1 = 1 3 π r 0 2 3 2 h = 1 2 π r 0 2 h V_1 = \frac{1}{3} \pi r_0^2 \frac{3}{2} h = \frac{1}{2} \pi r_0^2 h

If we take the origin at the apex of the cone, then its equation is

z = a x 2 + y 2 = a r z = a \sqrt{x^2 + y^2} = a r

since r 1 = 2 r_1 = 2 at the bottom and r 2 = 4 r_2 = 4 at the top and the difference in z z is h = 96 h =\sqrt{96} , then 96 = a ( 4 2 ) \sqrt{96} = a (4 - 2) , so that a = 96 / 2 = 24 a = \sqrt{96}/2 = \sqrt{24}

Next, the water surface in the tilted cup will cross the axis of the cup at an elevation of z = z 0 z = z_0 . This is shown in the attached image which shows

the cup after untilting. We need the find the volume under the blue line (plane). If we assume the x-axis is pointing towards the reader, then the y-axis is pointing to the right and the z-axis is pointing vertically up.

The equation of the plane of the surface of the water is z = tan ( π 6 ) y + z 0 z = \tan(\dfrac{\pi}{6}) y + z_0 where z 0 z_0 is yet to be determined.

To find the volume of the cone under this plane, we'll find its intersection

with the plane. Let t = tan π 6 = 1 3 t = \tan \dfrac{\pi}{6} = \dfrac{1}{\sqrt{3}} , then

t y + z 0 = a x 2 + y 2 t y + z_0 = a \sqrt{x^2 + y^2}

t 2 y 2 + z 0 2 + 2 t y z 0 = a 2 ( x 2 + y 2 ) t^2 y^2 + z_0^2 + 2 t y z_0 =a^2( x^2 + y^2)

Re-arranging,

y 2 ( a 2 t 2 ) 2 t y z 0 + a 2 x 2 = z 0 2 y^2 (a^2 - t^2) - 2 t y z_0 + a^2 x^2 = z_0^2

Completing the square,

( a 2 t 2 ) ( y t z 0 / ( a 2 t 2 ) ) 2 + a 2 x 2 = z 0 2 + t 2 z 0 2 / ( a 2 t 2 ) = z 0 2 ( a 2 ) / ( a 2 t 2 ) (a^2 - t^2) (y - t z_0 /(a^2 - t^2) )^2 + a^2 x^2 = z_0^2 + t^2 z_0^2/ (a^2 - t^2) = z_0^2 ( a^2 )/(a^2 - t^2)

This can be written as

x 2 / A 2 + ( y y 0 ) 2 / B 2 = 1 x^2 / A^2 + (y - y_0)^2 / B^2 = 1

where

y 0 = t z 0 / ( a 2 t 2 ) y_0 = t z_0 / (a^2 - t^2)

A = z 0 / ( a 2 t 2 ) 1 / 2 A = z_0 / (a^2 - t^2)^{1/2}

B = z 0 a / ( a 2 t 2 ) B = z_0 a / (a^2 - t^2)

This is the equation of the projection of the elliptical surface of water onto the xy plane.

The area of this region is

A 1 = π A B = π z 0 2 a ( a 2 t 2 ) 3 / 2 A_1 = \pi A B = \pi z_0^2 \dfrac{a}{ (a^2 - t^2)^{3/2} }

Hence the area of the cone underneath the water surface is

A 2 = A 1 sin θ = 5 A 1 A_2 = \dfrac{A_1}{ \sin \theta } = 5 A_1

And finally the volume is V 2 = 1 3 d A 2 = 1 3 z 0 sin θ ( 5 A 1 ) = 1 3 π z 0 3 a ( a 2 t 2 ) 3 / 2 V_2 = \frac{1}{3} d A_2 = \frac{1}{3} z_0 \sin \theta (5 A_1) = \frac{1}{3} \pi z_0^3 \dfrac{a} { (a^2 - t^2)^{3/2} }

Setting V 2 V_2 equal to V 1 V_1 , gives us z 0 z_0 . Solving for z 0 z_0 , we get z 0 = 14.59451952 z_0 = 14.59451952

Hence the altitude of water at r = r 1 r = r_1 is z = z 0 + t r h = 15.74922006 96 = 5.951261087 z^* = z_0 + t r - h = 15.74922006 - \sqrt{96} = 5.951261087

And finally, the depth of water = z cos π 6 = 3 2 ( 5.951261087 ) = 5.153943286 = z^* \cos \dfrac{\pi}{6} = \dfrac{\sqrt{3}}{2} (5.951261087) = 5.153943286

which makes the answer 5153.943286 = 5153 \lfloor 5153.943286 \rfloor = \boxed{5153}

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