Pedal Triangle

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Given a point P, the pedal triangle of P is the triangle whose polygon vertices are the feet of the perpendiculars from P to the side lines. The pedal triangle of a triangle with trilinear coordinates alpha:beta:gamma and angles A, B, and C has trilinear vertex matrix

 [0 beta+alphacosC gamma+alphacosB; alpha+betacosC 0 gamma+betacosA; alpha+gammacosB beta+gammacosA 0]
(1)

(Kimberling 1998, p. 186), and is a central triangle of type 2 (Kimberling 1998, p. 55).

The side lengths are

a^'=(abcsqrt(beta^2+gamma^2+2betagammacosA))/(2R|aalpha+bbeta+cgamma|)
(2)
b^'=(abcsqrt(alpha^2+gamma^2+2alphagammacosB))/(2R|aalpha+bbeta+cgamma|)
(3)
c^'=(abcsqrt(alpha^2+beta^2+2alphabetacosC))/(2R|aalpha+bbeta+cgamma|),
(4)

where R is the circumradius of DeltaABC, and area is

 Delta^'=(4(calphabeta+balphagamma+abetagamma)Delta^3)/(abc(aalpha+bbeta+cgamma)^2),
(5)

where Delta is the area of DeltaABC.

The following table summarizes a number of special pedal triangles for various special pedal points P.

pedal pointKimberling centeranticevian triangle
incenter IX_1contact triangle
circumcenter OX_3medial triangle
orthocenter HX_4orthic triangle
Bevan point VX_(40)extouch triangle

The symmedian point of a triangle is the triangle centroid of its pedal triangle (Honsberger 1995, pp. 72-74).

The third pedal triangle is similar to the original one. This theorem can be generalized to: the nth pedal n-gon of any n-gon is similar to the original one. It is also true that

 P_BP_C=APsinA
(6)

(Johnson 1929, pp. 135-136; Stewart 1940; Coxeter and Greitzer 1967, p. 25). The area Delta_P of the pedal triangle of a point P is proportional to the power of P with respect to the circumcircle,

A=1/2(R^2-OP^2)sinAsinBsinC
(7)
=(R^2-OP^2)/(4R^2)Delta
(8)

(Johnson 1929, pp. 139-141).

The only closed billiards path of a single circuit in an acute triangle is the pedal triangle. There are an infinite number of multiple-circuit paths, but all segments are parallel to the sides of the pedal triangle (Wells 1991).

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