The Art of the EllipseOn this page we recall the basic theory of the ellipse, and we develop Kepler's image of an ellipse inscribed in a unit circle. |
The standard ellipse, Fig. 01By definition, the ellipse in standard position is the locus of points R = (X, Y) such that(X/A)2 + (Y/B)2 = 1As shown in the figure, we visualize the ellipse with the major axis vertical, along the X axis. Let Q denote the upper end of the major axis, and C its center. Let CQ denote the distance from point C to point Q. Then the parameters of the ellipse are:
The ellipse may be drawn by attaching a string of length L at the two foci, S and S', and using it to guide a pencil around the ellipse. When the pencil is at Q, the string covers S'Q twice and SS' once, so 2*(A-C) + 2*C = L, or L = 2*A. Considering the pencil at (0, B), the end of the semi-minor axis, the Pythagorean theorem gives us the equations, B = sqrt(A2 - C2)relating A, B, C, and e. |
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Kepler's ellipse, Fig. 02Here we follow Kepler, as described in [Katz, 1993; p. 378]. We normalize the figure by rescaling both X and Y axes by 1/A. We now have another ellipse of the same eccentricity, but having a=A/A=1, b=B/A=0.6, and c=C/A=e=0.8.Now enclose the ellipse (no matter the eccentricity) in a circle of radius one. Note that the focal distance is now c = e, and the semi-minor axis of the ellipse is now b = sqrt(1 - e2) < 1. If the eccentricity is small, as it is for all planets, then we have the approximation, b ~= 1 - e2/2. |
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Kepler's ellipse and circle, Fig. 03aAgain following Kepler, we choose a point R on the ellipse, and draw a horizontal line through it, meeting the unit circle at W and the X (vertical) axis at V. If W = (X0, Y0), R = (X1, Y1), and V = (X2, Y2), then:
(Y0)2 = (Y1/b)2so Y1 = b*Y0. Thus the ellipse within the circumscribed unit circle may be understood as the circle uniformly compressed in the horizontal dimension by the factor b < 1. |
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Rev'd 29 dec 2001 by ralph abraham |