Changing Center of Ellipse in Polar Coordinates

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To change the center of an ellipse in polar coordinates, start with the Cartesian equation of the ellipse centered at (0, 0) and modify it for a new center at (c, d). Substitute polar representations for x and y, then expand and simplify the resulting equation, paying attention to trigonometric identities. The discussion highlights a method to express the transformed equation in a compact form involving constants A, B, C, and a phase-shifted angle phi. This approach allows for flexibility in defining the ellipse's center without restrictions on the semi-axis lengths.
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Hi, does exist an easy way to change the center of circle or a ellipse in polar coordinates?

thanks!
 
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Yes, and it was given in any textbook dealing with the conic sections that I have ever seen:
If the equation of an ellipse centered at (0, 0) is
\frac{x^2}{a^2}+ \frac{y^2}{b^2}= 1
then the same ellipse, centered at (a, b) has equation
\frac{(x- a)^2}{a^2}+ \frac{(y-b)^2}{b^2}= 1
 
Now you have to pass from the cartesian eqns that Halls wrote to polar coordinates and you're done.
 
Yes thanks...but I need it in polar coordinates
 
Insert polar representations for "x" and "y", multiply out parentheses and simplify and redefine variables/constants.
In particular, remember simplifying trig identities, such as, for example:
2\sin^{2}\theta=1-\cos(2\theta)
 
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Now, HallsofIvy made out a special case, with the center with the same values as the lengths of the semi-axes.

You shouldn't make that restriction here (call one of the (a,b)-pairs (c,d)-for example).

To give you the first step on your way, multiplying up and out, we get (with (c,d) centre coordinates):
b^{2}r^{2} \cos^{2}\theta+a^{2}r^{2} \sin^{2}\theta-2b^{2}cr \cos\theta-2a^{2} dr\sin\theta=a^{2}b^{2}-c^{2}-d^{2}
There would be various ways to simplify this expression further, and redefing independent constants.

One very compact way of doing so would be to transform your equation into the following form:
Ar^{2}\cos\gamma+Br\sin\phi=C
where the angle "phi" is a phase-shifted version of "gamma"/2 with a fourth constant D to be determined along with A, B and C (gamma being twice the value of "theta")
 
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Here is a little puzzle from the book 100 Geometric Games by Pierre Berloquin. The side of a small square is one meter long and the side of a larger square one and a half meters long. One vertex of the large square is at the center of the small square. The side of the large square cuts two sides of the small square into one- third parts and two-thirds parts. What is the area where the squares overlap?

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