Generalized Chinese Puzzle

Calculus Level 5

Consider a body that is formed by the intersection of two identical and perpendicular cylinders. The cross-section of the cylinders has at least one axis of symmetry. Also, the boundary of the half of the cross section can be expressed as a function of this axis (the half cross section is the area under the function). Now consider a second volume created by the revolution of the half cross section area. What is the ratio of the intersection volume to the revolution volume?

For example:

Take any function (it can be piecewise). Create the cylinders. We get the intersection volume V i {V}_{i} We also need the revolution volume V r {V}_{r} And calculate the ratio V i V r \dfrac{{V}_{i}}{{V}_{r}} .

Give your answer to 3 decimal places.


The answer is 1.273239.

This section requires Javascript.
You are seeing this because something didn't load right. We suggest you, (a) try refreshing the page, (b) enabling javascript if it is disabled on your browser and, finally, (c) loading the non-javascript version of this page . We're sorry about the hassle.

2 solutions

Adrian Aruștei
Apr 5, 2016

We can write the volume of the intersection body as 4 times the volume of the missing part from the solid in the figure. Cosider the height of the body as H H . V int = 4 V 1 d V = 4 0 H 0 f ( z ) 0 f ( z ) 1 d x d y d z {{V}_{\operatorname{int}}}=4\int\limits_{V}{1dV}=4\int\limits_{0}^{H}{\int\limits_{0}^{f(z)}{\int\limits_{0}^{f(z)}{1dx}}}dydz The final form we will use later is: V int = 4 0 H f ( z ) 2 d z {{V}_{\operatorname{int}}}=4\int\limits_{0}^{H}{{{f(z)}^{2}}}dz The volume of revolution of the half cross section is equal to the area of half cross section times the length of revolution of the center of the mass. Let's note the distance from the center of mass to z z -axis with D D . V r e v = A 2 π D {{V}_{rev}}=A2\pi D Where A A is the area under the function. We know the formula for the center of mass: D = A k d A A = 0 H ( 0 f ( z ) k d k ) d z A D=\frac{\int\limits_{A}{kdA}}{A}=\frac{\int\limits_{0}^{H}{\left( \int\limits_{0}^{f(z)}{kdk} \right)dz}}{A} Where k k is the axis perpendicular to z z -axis ( the coordinate of element d A dA ). Substituting and simplifying the area we get: V r e v = 2 π 0 H ( k 2 2 0 f ( z ) ) d z = π 0 H f ( z ) 2 d z {{V}_{rev}}=2\pi \int\limits_{0}^{H}{\left( \left. \frac{{{k}^{2}}}{2} \right|_{0}^{f(z)} \right)dz}=\pi \int\limits_{0}^{H}{f{{(z)}^{2}}dz} We see now that the ratio is: V int V r e v = 4 π 1.2732 \frac{{{V}_{\operatorname{int}}}}{{{V}_{rev}}}=\frac{4}{\pi }\approx1.2732

I am amazed that the ratio is a constant! That would not have occured to me without working through the details.

Calvin Lin Staff - 5 years, 2 months ago
Jon Haussmann
Apr 27, 2016

Let y = f ( z ) y = f(z) be a point on the graph. Then for this value of z z , the cross-section of the first solid is a square with side length 2 y 2y , so its area is 4 y 2 4y^2 . The cross-section of the second solid is a circle with radius y y , so its area is π y 2 \pi y^2 . The ratio of these areas is 4 π \frac{4}{\pi} , so the ratio of the volumes is also 4 π \frac{4}{\pi} .

0 pending reports

×

Problem Loading...

Note Loading...

Set Loading...