Area of Center Locus

Geometry Level 4

An ellipse with semi-major axis a a and semi-minor axis b b is sliding in place, such that it is always tangent to the x-axis at the origin, as shown in the animation image below. The center of the ellipse traces a closed locus. Find the area enclosed by this locus in terms of a a and b b .

π ( a 2 b 2 ) \pi (a^2 - b^2 ) π 2 ( a 2 b 2 ) \dfrac{\pi}{2} (a^2 - b^2) π 2 ( a b ) 2 \dfrac{\pi}{2} (a - b )^2 π ( a b ) 2 \pi (a - b)^2

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2 solutions

Uros Stojkovic
Sep 15, 2019

Standard parametric equation of ellipse is ( a cos t , b sin t ) (a\cos{t}, b\sin{t}) . Instead of letting center of ellipse move around, we will consider a scenario where center of ellipse is fixed at the origin of coordinate system S and where we set an origin of another coordinate system S' at some point on the ellipse such that its x'-axis coincide with tangent line to the ellipse at that point. So, radius vector of origin of S' with respect to S is ( a cos t , b sin t ) (a\cos{t}, b\sin{t}) . Unit vector i i' which corresponds to x'-axis is consequently: i = t ^ = 1 a 2 sin 2 t + b 2 cos 2 t ( a sin t , b cos t ) i' = \hat{t} = \frac{1}{\sqrt{a^{2}\sin^{2}{t}+b^{2}\cos^{2}{t}}}(-a\sin{t},b\cos{t}) Unit vector j j' which corresponds to y'-axis and is orthogonal to i i' is then: j = 1 a 2 sin 2 t + b 2 cos 2 t ( b cos t , a sin t ) j' = \frac{1}{\sqrt{a^{2}\sin^{2}{t}+b^{2}\cos^{2}{t}}}(-b\cos{t}, -a\sin{t}) Now, we can express origin of S with respect to S': O O = O O = a cos t i b sin t j = a cos t a 2 sin 2 t + b 2 cos 2 t ( a sin t i + b cos t j ) b sin t a 2 sin 2 t + b 2 cos 2 t ( b cos t i a sin t j ) = 1 a 2 sin 2 t + b 2 cos 2 t ( ( a 2 b 2 ) sin t cos t i + a b j ) \begin{aligned} \overrightarrow{O'O} &=- \overrightarrow{OO'} = -a\cos{t}\cdot i -b\sin{t}\cdot j \\ &= \frac{a\cos{t}}{\sqrt{a^{2}\sin^{2}{t}+b^{2}\cos^{2}{t}}}(a\sin{t}\cdot i' + b\cos{t}\cdot j') - \frac{b\sin{t}}{\sqrt{a^{2}\sin^{2}{t}+b^{2}\cos^{2}{t}}}(b\cos{t}\cdot i' - a\sin{t}\cdot j') \\ &= \frac{1}{\sqrt{a^{2}\sin^{2}{t}+b^{2}\cos^{2}{t}}}((a^{2}-b^{2})\sin{t}\cos{t}\cdot i' + ab\cdot j')\end{aligned} Thus, curve which is traced by the center of ellipse is: ρ = 1 a 2 sin 2 t + b 2 cos 2 t ( a 2 b 2 2 sin 2 t , a b ) \vec{\rho} = \frac{1}{\sqrt{a^{2}\sin^{2}{t}+b^{2}\cos^{2}{t}}}\left(\frac{a^{2}-b^{2}}{2}\sin{2t}, ab\right ) From here, it seemed to me a very tedious task to find a closed form expression for enclosed area, so I approximated the answer and matched it with the formula which is closest to it. However, I would like to know about a nice way to derive the formula, if it exists at all. @Hosam Hajjir ?

I don't know of a nice way to do this area integration.

Hosam Hajjir - 1 year, 8 months ago

I thought so. How did you find correct formula?

Uros Stojkovic - 1 year, 8 months ago

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The procedure I took is kind of lengthy, especially the integrations , but they do lead to the formula.

Hosam Hajjir - 1 year, 8 months ago

@Hosam Hajjir Can I ask you to write a solution for this problem you've posted? Somehow I didn't get it right and I want to see where I've gone wrong. Thanks in advance!

Uros Stojkovic - 1 year, 8 months ago

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I will post a solution in a couple of days. Thanks for your interest.

Hosam Hajjir - 1 year, 8 months ago

The solution of the velocity problem is now available.

Hosam Hajjir - 1 year, 8 months ago

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Hi Hosam, i'm trying to post problems with GIF file but i get a message error and support does not care. How did you do it? Thanks

Valentin Duringer - 4 months, 3 weeks ago
Abu Zubair
Jul 17, 2019

Sorry this may not be a valid solution because of choice elimination.

Firstly, if you interchange a and b the area remains same. As they can't be negative, options with a²-b² can't be the solution as replacing a with b will make area negative.

Then take a extreme case of a=0 and b=b. If you look carefully it will trace a semicircle twice(but not to take it twice as we need the area inside the loop). So now area will be πb²/2.

Therefore, π×(a-b)²/2 is the answer.

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