Circle Square Hybrid

Calculus Level 5

Consider a unit circle centered on the origin, and a circumscribing square. We could represent these curves in polar coordinates as ( R 1 ( θ ) , θ ) \Big( R_1(\theta), \theta \Big ) and ( R 2 ( θ ) , θ ) \Big( R_2(\theta), \theta \Big ) .

Form a third curve as follows:

R 3 ( θ ) = R 1 ( θ ) + R 2 ( θ ) 2 R_3 (\theta) = \frac{R_1(\theta) + R_2(\theta)}{2}

What is the area enclosed by the third curve? Note that this is the combined area of the tan and blue regions. If this area is A A , give your answer as 1000 A \lfloor 1000 \, A \rfloor , where \lfloor \cdot \rfloor denotes the floor function.


The answer is 3548.

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2 solutions

Aaghaz Mahajan
Apr 1, 2019

We know that

R 1 = 1 \displaystyle R_1=1 and R 2 = sec θ { π 4 θ π 4 } \displaystyle R_2=\sec\theta\ \left\{-\frac{\pi}{4}\le\theta\le\frac{\pi}{4}\right\} denotes the right vertical edge of the square. Now,

R 3 = ( 1 + sec θ ) 2 { π 4 θ π 4 } \displaystyle R_3=\frac{\left(1+\sec\theta\right)}{2}\left\{-\frac{\pi}{4}\le\theta\le\frac{\pi}{4}\right\} for the right bulging side of the third curve. Now, we simply calculate the area of this part and multiply it by 4 4 since the figure is symmetrical.

Hence, we get area of one part

1 8 π 4 π 4 ( 1 + sec θ ) 2 d θ \displaystyle \frac{1}{8}\int_{-\frac{\pi}{4}}^{\frac{\pi}{4}}\left(1+\sec\theta\right)^2d\theta

= 1 8 ( π 2 + 4 ln ( 2 + 1 ) + 2 ) \displaystyle =\frac{1}{8}\left(\frac{\pi}{2}+4\ln\left(\sqrt{2}+1\right)+2\right)

Hence, total area of the third curve is

π 4 + 2 ln ( 2 + 1 ) + 1 = 3.54814.... \displaystyle \frac{\pi}{4}+2\ln\left(\sqrt{2}+1\right)+1=3.54814....

Similar solution with @Aaghaz Mahajan 's

We note that R 1 ( θ ) = 1 R_1(\theta) = 1 and R 2 ( θ ) = 1 cos θ = sec θ R_2(\theta) = \dfrac 1{\cos \theta} = \sec \theta . Then R 3 ( θ ) = R 1 ( θ ) + R 2 ( θ ) 2 = 1 + sec θ 2 R_3(\theta) = \dfrac {R_1(\theta) + R_2(\theta)}2 = \dfrac {1+\sec \theta}2 , and the area enclosed by R 3 ( θ ) R_3 (\theta) :

A = 0 2 π 1 2 R 3 2 ( θ ) d θ Since R 3 ( θ ) is symmetrical about the origin = 8 0 π 4 1 2 R 3 2 ( θ ) d θ = 0 π 4 ( 1 + sec θ ) 2 d θ = 0 π 4 ( 1 + 2 sec θ + sec 2 θ ) d θ = 0 π 4 d θ + 2 0 π 4 sec θ d θ + 0 π 4 sec 2 θ d θ = [ θ + 2 tan θ sec θ + sec 2 θ tan θ + sec θ d θ + d tan θ ] 0 π 4 = [ θ + 2 ln ( tan θ + sec θ ) + tan θ ] 0 π 4 = π 4 + 2 ln ( 1 + 2 ) + 1 3.548145 \begin{aligned} A & = \int_0^{2\pi} \frac 12 R_3^2 (\theta) \ d\theta & \small \color{#3D99F6} \text{Since }R_3(\theta) \text{ is symmetrical about the origin} \\ & = 8 \int_0^\frac \pi 4 \frac 12 R_3^2 (\theta) \ d\theta \\ & = \int_0^\frac \pi 4 (1+\sec \theta)^2 \ d\theta \\ & = \int_0^\frac \pi 4 \left(1+ 2 \sec \theta + \sec^2 \theta \right) \ d\theta \\ & = \int_0^\frac \pi 4 d\theta + 2 \int_0^\frac \pi 4 \sec \theta\ d\theta + \int_0^\frac \pi 4 \sec^2 \theta \ d\theta \\ & = \left[\theta + 2 \int \frac {\tan \theta \sec \theta + \sec^2 \theta}{\tan \theta + \sec \theta } \ d\theta + \int d \tan \theta \right]_0^\frac \pi 4 \\ & = \bigg[\theta + 2 \ln (\tan \theta + \sec \theta) + \tan \theta \bigg]_0^\frac \pi 4 \\ & = \frac \pi 4 + 2 \ln (1+\sqrt 2) + 1 \\ & \approx 3.548145 \end{aligned}

Therefore, 1000 A = 3548 \lfloor 1000A \rfloor = \boxed{3548} .

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