I have a white square piece of paper with each side 8 centimeters long, and a crayon which is also 8 centimeters long.
First, I put the crayon on the left edge of the paper. Then, I carefully rotate the crayon so that the top end of the crayon moves downwards along the left edge of the paper and the lower end moves to the right along the lower edge of the paper, all the way until the crayon lies horizontally.
Calculate the area colored by the crayon in square centimeters ( cm 2 ). Assume that the crayon has a cylindrical shape so it only leaves a very thin line when it touches the paper surface.
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Did the same way.
@Brian Charlesworth I know it is easy, but just to make the solution more complete, shouldn't you prove it Sir??? :)
This is just a copy of my solution to this problem, with some small modifications
Placing the paper in the cartesian plane, with the bottom left corner ar (0,0), at any given time, the crayon makes an angle θ with the horizontal, that goes from 2 π to 0 , If you consider a new crayon at angle θ ′ = θ + h , the two crayons intersect at a point P ′ . As h → 0 , P ′ → P , and P depends on θ . All these limit intersection points are points in the edge of the area swept by the sqeegee, and vice-versa. This is the main statement on which this solution is based. *For simplicity, I considered a sqeegee of length 1 , we'll just have to remember to multiply the area by 8 2 in the end to get the correct answer. Since the crayon has length 1 , from triangle △ O A B , we see that A O = sin θ , B O = cos θ , and consequently, A A ′ = cos θ d θ , and B B ′ = sin θ d θ . Now, from triangles △ D A A ′ and △ O A ′ B ′ , we see that ∠ A D A ′ = ∠ A ′ B ′ O , so D A = A ′ A cot θ which means D A = sin θ cos 2 θ d θ . Finally, from similar triangles △ D A P and △ P B B ′ , A P D A = P B ′ B B ′ , but we know that A P + P B = 1 . Then, making P B = p and substituting what we found earlier, we have ( p − 1 ) sin θ cos 2 θ = p sin θ p = ( 1 − p ) tan 2 θ p = ( 1 + tan 2 θ ) tan 2 θ p = sin 2 θ Then, the coordinates of the point P with respect to θ are x ( θ ) = cos θ − ( cos θ ) sin 2 θ y ( θ ) = ( sin θ ) sin 2 θ Simplifying, we have x ( θ ) = cos 3 θ y ( θ ) = sin 3 θ Finally, we know that the area under a parametric curve is ∫ t 1 t 2 y ( t ) x ′ ( t ) d t , so substituting for what we have, and multiplying by 8 2 : A r e a = 6 4 ∫ 0 2 π 3 sin 4 ( t ) cos 2 ( t ) d t ≈ 1 8 . 8 4 9
The following web article gives details of an Astroid. We need 1/4 the area
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you have to type like this [ web article ] ( https://en.m.wikipedia.org/wiki/Astroid ) , so it shows up as web article
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This describes one-quarter of the area inside an astroid , hence the area is 4 1 × 8 3 π × 8 2 ≈ 1 8 . 8 5 .