The two Archimedean spirals below, are, in fact, different sections of the same spiral. On the left is plotted (in polar coordinates) r = θ for 0 ≤ θ ≤ 6 π and on the right r = θ for − 6 π ≤ θ ≤ 0 :
If we plot these on the same graph, the two parts of the spiral intersect each other. We can colour them in as below:
The area of the blue region can be written in the form b a π c , where a , b , c are positive integers and a and b are coprime.
Please enter a + b + c as your answer.
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Great job.
The area of the central white region is W 1 = 2 ⋅ 2 1 ∫ 0 2 π θ 2 d θ = 2 4 1 π 3 .
The area of the central blue region is B 1 = 2 ⋅ 2 1 ∫ 2 π 2 3 π θ 2 d θ − W 1 = 2 4 2 6 π 3 − 2 4 1 π 3 = 2 4 2 5 π 3 .
The area of the next white region W 2 with B 1 and W 1 is B 1 + W 1 + W 2 = 2 ⋅ 2 1 ∫ 2 3 π 2 5 π θ 2 d θ = 2 4 9 8 π 3 .
The area of the next blue region is B 2 = 2 ⋅ 2 1 ∫ 2 7 π 2 5 π θ 2 d θ − ( B 1 + W 1 + W 2 ) = 2 4 2 1 8 π 3 − 2 4 9 8 π 3 = 2 4 1 2 0 π 3 .
The area of the third white region W 3 with B 1 , B 2 , W 1 , and W 2 is B 1 + B 2 + W 1 + W 2 + W 3 = 2 ⋅ 2 1 ∫ 2 7 π 2 9 π θ 2 d θ = 2 4 3 8 6 π 3 .
The area of the third blue region is B 3 = 2 ⋅ 2 1 ∫ 2 9 π 2 1 1 π θ 2 d θ − ( B 1 + B 2 + W 1 + W 2 + W 3 ) = 2 4 6 0 2 π 3 − 2 4 3 8 6 π 3 = 2 4 2 1 6 π 3 .
The total area of the blue regions is therefore B = B 1 + B 2 + B 3 = 2 4 2 5 π 3 + 2 4 1 2 0 π 3 + 2 4 2 1 6 π 3 = 2 4 3 6 1 π 3 , so a = 3 6 1 , b = 2 4 , c = 3 , and a + b + c = 3 8 8 .
Thanks for writing up your solution - very nice! Down to the notation ( B i etc) this is what I would have posted, so I won't write a solution up here. (The only difference would be taking the factor 2 4 1 π 3 out early on just to write less LaTeX!)
They're not significant ones, but you've a typo in the very last line (somehow 3 2 1 has come in instead of 3 6 1 ) and in the integral limits for B 2 .
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Slip the blue region into three rings A 1 , A 2 , and A 3 as shown. As the areas are symmetrical about the y -axis, we need only to consider the positive side of x -axis then multiplied by 2 . We note that:
A 1 = 2 ( ∫ 2 π 2 3 π 2 r 2 d θ − ∫ 0 2 π 2 r 2 d θ ) = ∫ 2 π 2 3 π θ 2 d θ − ∫ 0 2 π θ 2 d θ = 3 θ 3 ∣ ∣ ∣ ∣ 2 π 2 3 π − 3 θ 3 ∣ ∣ ∣ ∣ 0 2 π = 2 4 2 7 π 3 − 2 4 1 π 3 − 2 4 1 π 3 − 0 = 2 4 2 5 π 3
Similarly, A 2 = 3 θ 3 ∣ ∣ ∣ ∣ 2 5 π 2 7 π − 3 θ 3 ∣ ∣ ∣ ∣ 2 3 π 2 5 π = 2 4 1 2 0 π 3 and A 3 = 3 θ 3 ∣ ∣ ∣ ∣ 2 9 π 2 1 1 π − 3 θ 3 ∣ ∣ ∣ ∣ 2 7 π 2 9 π = 2 4 2 1 6 π 3 .
Therefore, A 1 + A 2 + A 3 = 2 4 2 5 + 1 2 0 + 2 1 6 π 3 = 2 4 3 6 1 π 3 ⟹ a + b + c = 3 6 1 + 2 4 + 3 = 3 8 8 .