An infinitely thin, k cm -long squeegee begins to slide down from the upper-left corner of a k cm × k cm square window. Its other end simultaneously slides toward the lower-right corner of the window, with the upper end kept in contact with the left side of the window.
If k = π 2 0 1 6 , what is the area of the window ( in cm 2 ) cleaned by the squeegee?
Note : you may end up with an integral expression that's difficult to evaluate analytically. Feel free to finish the job using the code environment below:
import math
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How did you figure out the first equation ?
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Consider the right-angled triangle formed by the squeegee and the two perpendicular sides of the window; if the squeegee has length k , and its right end is at some distance n from the left corner, then by Pythagoras's theorem, the left side of the triangle is given by k 2 − n 2 . Then the gradient of the squeegee is n − k 2 − n 2 . The y intercept is also just the left side of the triangle, which is k 2 − n 2 , so the equation of squeegee becomes S ( x ) = n − k 2 − n 2 x + k 2 − n 2 .
Placing the window in the cartesian plane, with the bottom left corner ar (0,0), at any given time, the squeegee makes an angle
θ
with the horizontal, that goes from
2
π
to
0
, If you consider a new sqeegee at angle
θ
′
=
θ
+
h
, the two squeegees intersect at a point
P
′
. As
h
→
0
,
P
′
→
P
, and
P
depends on
θ
. All these limit intersection points are, of course, 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
k
2
in the end to get the correct answer.
Since the squeegee 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 wat we have, and multiplying by
k
2
:
A
r
e
a
=
π
2
0
1
6
∫
0
2
π
3
sin
4
(
t
)
cos
2
(
t
)
d
t
=
1
8
9
Could you please explain what AA' = sin theta d there? Thanks!
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Thanks for ponting this out! I'll fix it. I actually mistakenly switched the expressions for AA' and BB', I only did it right there at the beginning, so the rest of the solution is correct. Here's the correct reasoning:
Say the height of the point where the sqeegee touches the y axis is h which is, of course equal to sin θ , well, d θ d h = cos θ , so d h = cos θ d θ , which is the same thing as AA': A tiny change in height caused by a tiny change in θ . The reasoning for BB' is analogous.
Why are you not able to simply solve this by creating a larger square made up from 4 of the ones shown\ then getting the area of the internal circle, subtracting it from the area of the larger square and divide by 4? is the blue area shown not a quarter circle?
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The blue area is actually not a quarter circle its slightly bigger than that
Let the square be represented in Cartesian coordinates, with ( 0 , 0 ) as the bottom left corner and ( 0 , k ) as the top left corner.
At any time, let ϕ be the angle between the squeegee and the vertical. Initially ϕ = 0 and at the end ϕ = 2 π .
The squeegee forms a line with gradient − cot ϕ and y-intercept k cos ϕ . Thus it has the equation y = k cos ϕ − cot ϕ x
A point is considered cleaned if it has been on a squeegee before. In other words, an angle ϕ must exist such that 0 ≤ ϕ ≤ 2 π which satisfies [y=k\cos{\phi}-\cot{\phi} x]
If we fix x then there will be a range of y values. The curve is given by the maximum y-values. Differentiating y with respect to p h i , d ϕ d y = − k sin ϕ + csc 2 ϕ x
The ϕ yielding the y m a x is given by sin ϕ = 3 k x ⇒ y m a x = k ( 1 − ( k x ) 3 2 ) 2 3
Integrating, the cleaned area is
k ∫ 0 k ( 1 − ( k x ) 3 2 ) 2 3 d x
Let r = k x ⇒ d x = k d r = k 2 ∫ 0 1 ( 1 − r 3 2 ) 2 3 d r
Let r = sin 3 θ ⇒ 3 sin 2 θ cos θ = 2 3 k 2 ∫ 0 2 π 2 sin 2 θ cos 4 θ d θ = 2 3 k 2 Γ ( 2 5 + 2 3 ) Γ ( 2 5 ) + Γ ( 2 3 ) = 2 3 ( π 2 0 1 6 ) 6 ( 2 3 ) ( 2 1 ) 2 ( π ) 2 = 1 8 9
Each line ha the form
F ( t , x , y ) = − k sin ( t ) + x tan ( t ) + y = 0
for 0 < = t < = π / 2 .
Equation of the envelope is all (x,y) such that
F ( t , x , y ) = 0 , F ( 1 , 0 , 0 ) ( t , x , y ) = 0
Solving for x,y we get
{ x = k cos 3 ( t ) , y = k sin ( t ) − k sin ( t ) cos 2 ( t ) }
So we want
∫ 2 π 0 y ( x ( t ) ) x ′ ( t ) d t = 3 2 3 π k 2
which gives 189 with k above.
I use formula for astroid area. http://www.wolframalpha.com/input/?i=astroid
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Sorry for the inconsistent image size; it would have been tiresome to copy and edit the TeX into the solutions box.