Consider a unit circle and a radiant point located at . There are four different regimes of caustics, illustrated above.
For radiant point at , the catacaustic is the nephroid
(1)
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(2)
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(Trott 2004, p. 17, mistakenly states that the catacaustic for parallel light falling on any concave mirror is a nephroid.)
For radiant point a finite distance , the catacaustic is the curve
(3)
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(4)
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which is apparently incorrectly described as a limaçon by Lawrence (1972, p. 207).
For radiant point on the circumference of the circle (), the catacaustic is the cardioid
(5)
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(6)
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with Cartesian equation
(7)
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For radiant point inside the circle, the catacaustic is a discontinuous two-part curve.
If the radiant point is the origin, then the catacaustic degenerates to a single point at the origin since all rays reflect upon themselves back through the origin.