Pool Math

Calculus Level 4

In a pool party, you decide to test your mad Math skills.

Having nothing better to do, you place a rigid iron bar inside a section c of an empty pool such that either end of it lies on the same plane and touch the insides of the pool. You then choose a point P on the bar such that the distance to one end is 7 and the distance to the other end is 3 , with the length of the bar being 10 . Finally, you move the bar in a way that, at any given time, neither end leaves c .

Suppose that each pool is a surface such that its horizontal sections are convex closed curves.

After one lap - at the moment the bar is back where it was first placed - what is the area between the curve covered by point P and the border of c , rounded to the closest integer?


The answer is 66.

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2 solutions

Sandro Saporito
Mar 12, 2014

First, look here .

As shown in the figure above, we assume that, as the bar moves, it is always tangent to a given curve e inside of the original section - and this curve is not the curve described by point P. Let Q be the point at which the bar is tangent to e , A and B be the points at each end of the bar and r the distance from A to Q. We then use the fact that the area of a tangent sweep equals the area of a tangent cluster ( Mamikon's Theorem , probably not the most famous of theorems) to say that the area covered by a given tangent cluster is:

0 2 π 0 k ( θ ) R d R d θ = 1 2 0 2 π k 2 ( θ ) d θ \int_{0}^{2\pi}\int_{0}^{k(\theta)}RdRd\theta = \frac{1}{2}\int_{0}^{2\pi}k^{2}(\theta)d\theta

Instead of solving for numbers, I'll suppose segment AP has length a and segment PB has segment b, for a total of a+b. We can then write three integrals:

1) The area covered by segment AQ

I A Q = 1 2 0 2 π r 2 d θ I_{AQ}=\frac{1}{2}\int_{0}^{2\pi}r^{2}d\theta

2) The area covered by segment BQ

I B Q = 1 2 0 2 π ( a + b r ) 2 d θ I_{BQ}=\frac{1}{2}\int_{0}^{2\pi}(a+b-r)^{2}d\theta

3) The area covered by segment PQ

I P Q = 1 2 0 2 π ( a r ) 2 d θ I_{PQ}=\frac{1}{2}\int_{0}^{2\pi}(a-r)^{2}d\theta

Notice that segments AQ and BQ sweep the same area, which means I A Q = I B Q I_{AQ}=I_{BQ} . Notice also that if we take the area swept by BQ minus the area swept by PQ, we get the area swept by PB - which is what we wanted in the first place. Therefore:

A = I B Q I P Q = 1 2 0 2 π ( a + b r ) 2 ( a r ) 2 d θ = 1 2 0 2 π ( 2 a b + b 2 2 b r ) d θ A=I_{BQ}-I_{PQ}=\frac{1}{2}\int_{0}^{2\pi}(a+b-r)^{2}-(a-r)^{2}d\theta=\frac{1}{2}\int_{0}^{2\pi}(2ab+b^{2}-2br)d\theta

However, r depends on \theta; we then use our previous relation

I A Q = I B Q I_{AQ}=I_{BQ}

which yields

0 2 π r d θ = π ( a + b ) \int_{0}^{2\pi}r d\theta = \pi(a+b) .

Finally, we substitute this last integral on A:

A = 1 2 0 2 π ( 2 a b + b 2 2 b r ) d θ = 2 π a b + π b 2 π a b π b 2 = π a b A=\frac{1}{2}\int_{0}^{2\pi}(2ab+b^{2}-2br)d\theta=2\pi ab+\pi b^{2}-\pi ab-\pi b^{2}=\pi ab

Therefore, A = π a b A=\pi ab . This is called Holditch's Theorem .

Choosing a=3 and b=7, we get A = π × 3 × 7 = 65.97344... 66 A=\pi\times 3\times 7=65.97344...\approx \boxed{66} .

Steven Perkins
Mar 26, 2014

Since the problem implies that the difference in area is constant no matter the shape of the pool, I envisioned a simplified pool to make the problem easier. It is very interesting that this is invariant, by the way.

I used a circular pool of diameter 10, so that the bar just fit across. Then the point P makes a circle of radius 2. The difference in area is just pi*(5^2 - 2^2). This is just a bit less than:

66 \boxed{66}

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