Incircle and excircles

Incircle and excircles of a triangle.
  Extended sides of triangle ABC
  Incircle (incenter at I)
  Excircles (excenters at JA, JB, JC)
  Internal angle bisectors
  External angle bisectors (forming the excentral triangle)

In geometry, the incircle or inscribed circle of a triangle is the largest circle that can be contained in the triangle; it touches (is tangent to) the three sides. The center of the incircle is a triangle center called the triangle's incenter.[1]

An excircle or escribed circle[2] of the triangle is a circle lying outside the triangle, tangent to one of its sides and tangent to the extensions of the other two. Every triangle has three distinct excircles, each tangent to one of the triangle's sides.[3]

The center of the incircle, called the incenter, can be found as the intersection of the three internalangle bisectors.[3][4] The center of an excircle is the intersection of the internal bisector of one angle (at vertex A, for example) and the external bisectors of the other two. The center of this excircle is called the excenter relative to the vertex A, or the excenter of A.[3] Because the internal bisector of an angle is perpendicular to its external bisector, it follows that the center of the incircle together with the three excircle centers form an orthocentric system.[5]

Incircle and Incenter

Suppose ABC{\displaystyle \triangle ABC} has an incircle with radius r{\displaystyle r} and center I{\displaystyle I}. Let a{\displaystyle a} be the length of BC¯{\displaystyle {\overline {BC}}}, b{\displaystyle b} the length of AC¯{\displaystyle {\overline {AC}}}, and c{\displaystyle c} the length of AB¯{\displaystyle {\overline {AB}}}.

Also let TA{\displaystyle T_{A}}, TB{\displaystyle T_{B}}, and TC{\displaystyle T_{C}} be the touchpoints where the incircle touches BC¯{\displaystyle {\overline {BC}}}, AC¯{\displaystyle {\overline {AC}}}, and AB¯{\displaystyle {\overline {AB}}}.

Incenter

The incenter is the point where the internal angle bisectors of ABC,BCA, and BAC{\displaystyle \angle ABC,\angle BCA,{\text{ and }}\angle BAC} meet.

Trilinear coordinates

The trilinear coordinates for a point in the triangle is the ratio of all the distances to the triangle sides. Because the incenter is the same distance from all sides of the triangle, the trilinear coordinates for the incenter are[6]

 1:1:1.{\displaystyle \ 1:1:1.}

Barycentric coordinates

The barycentric coordinates for a point in a triangle give weights such that the point is the weighted average of the triangle vertex positions. Barycentric coordinates for the incenter are given by

a:b:c{\displaystyle a:b:c}

where a{\displaystyle a}, b{\displaystyle b}, and c{\displaystyle c} are the lengths of the sides of the triangle, or equivalently (using the law of sines) by

sinA:sinB:sinC{\displaystyle \sin A:\sin B:\sin C}

where A{\displaystyle A}, B{\displaystyle B}, and C{\displaystyle C} are the angles at the three vertices.

Cartesian coordinates

The Cartesian coordinates of the incenter are a weighted average of the coordinates of the three vertices using the side lengths of the triangle relative to the perimeter (that is, using the barycentric coordinates given above, normalized to sum to unity) as weights. The weights are positive so the incenter lies inside the triangle as stated above. If the three vertices are located at (xa,ya){\displaystyle (x_{a},y_{a})}, (xb,yb){\displaystyle (x_{b},y_{b})}, and (xc,yc){\displaystyle (x_{c},y_{c})}, and the sides opposite these vertices have corresponding lengths a{\displaystyle a}, b{\displaystyle b}, and c{\displaystyle c}, then the incenter is at

(axa+bxb+cxca+b+c,aya+byb+cyca+b+c)=a(xa,ya)+b(xb,yb)+c(xc,yc)a+b+c.{\displaystyle \left({\frac {ax_{a}+bx_{b}+cx_{c}}{a+b+c}},{\frac {ay_{a}+by_{b}+cy_{c}}{a+b+c}}\right)={\frac {a\left(x_{a},y_{a}\right)+b\left(x_{b},y_{b}\right)+c\left(x_{c},y_{c}\right)}{a+b+c}}.}

Radius

The inradius r{\displaystyle r} of the incircle in a triangle with sides of length a{\displaystyle a}, b{\displaystyle b}, c{\displaystyle c} is given by[7]

r=(sa)(sb)(sc)s,{\displaystyle r={\sqrt {\frac {(s-a)(s-b)(s-c)}{s}}},}

where s=12(a+b+c){\displaystyle s={\tfrac {1}{2}}(a+b+c)} is the semiperimeter (see Heron's formula).

The tangency points of the incircle divide the sides into segments of lengths sa{\displaystyle s-a} from A{\displaystyle A}, sb{\displaystyle s-b} from B{\displaystyle B}, and sc{\displaystyle s-c} from C{\displaystyle C} (see Tangent lines to a circle).[8]

Distances to the vertices

Denote the incenter of ABC{\displaystyle \triangle ABC} as I{\displaystyle I}.

The distance from vertex A{\displaystyle A} to the incenter I{\displaystyle I} is:

AI¯=d(A,I)=csinB2cosC2=bsinC2cosB2.{\displaystyle {\overline {AI}}=d(A,I)=c\,{\frac {\sin {\frac {B}{2}}}{\cos {\frac {C}{2}}}}=b\,{\frac {\sin {\frac {C}{2}}}{\cos {\frac {B}{2}}}}.}

Derivation of the formula stated above

Use the Law of sines in the triangle IAB{\displaystyle \triangle IAB}.

We get AI¯sinB2=csinAIB{\displaystyle {\frac {\overline {AI}}{\sin {\frac {B}{2}}}}={\frac {c}{\sin \angle AIB}}}. We have that AIB=πA2B2=π2+C2{\displaystyle \angle AIB=\pi -{\frac {A}{2}}-{\frac {B}{2}}={\frac {\pi }{2}}+{\frac {C}{2}}}.

It follows that AI¯=c sinB2cosC2{\displaystyle {\overline {AI}}=c\ {\frac {\sin {\frac {B}{2}}}{\cos {\frac {C}{2}}}}}.

The equality with the second expression is obtained the same way.

The distances from the incenter to the vertices combined with the lengths of the triangle sides obey the equation[9]

IA¯IA¯CA¯AB¯+IB¯IB¯AB¯BC¯+IC¯IC¯BC¯CA¯=1.{\displaystyle {\frac {{\overline {IA}}\cdot {\overline {IA}}}{{\overline {CA}}\cdot {\overline {AB}}}}+{\frac {{\overline {IB}}\cdot {\overline {IB}}}{{\overline {AB}}\cdot {\overline {BC}}}}+{\frac {{\overline {IC}}\cdot {\overline {IC}}}{{\overline {BC}}\cdot {\overline {CA}}}}=1.}

Additionally,[10]

IA¯IB¯IC¯=4Rr2,{\displaystyle {\overline {IA}}\cdot {\overline {IB}}\cdot {\overline {IC}}=4Rr^{2},}

where R{\displaystyle R} and r{\displaystyle r} are the triangle's circumradius and inradius respectively.

Other properties

The collection of triangle centers may be given the structure of a group under coordinate-wise multiplication of trilinear coordinates; in this group, the incenter forms the identity element.[6]

Incircle and its radius properties

Distances between vertex and nearest touchpoints

The distances from a vertex to the two nearest touchpoints are equal; for example:[11]

d(A,TB)=d(A,TC)=12(b+ca)=sa.{\displaystyle d\left(A,T_{B}\right)=d\left(A,T_{C}\right)={\tfrac {1}{2}}(b+c-a)=s-a.}

Other properties

If the altitudes from sides of lengths a{\displaystyle a}, b{\displaystyle b}, and c{\displaystyle c} are ha{\displaystyle h_{a}}, hb{\displaystyle h_{b}}, and hc{\displaystyle h_{c}}, then the inradius r{\displaystyle r} is one third the harmonic mean of these altitudes; that is,[12]

r=11ha+1hb+1hc.{\displaystyle r={\frac {1}{{\dfrac {1}{h_{a}}}+{\dfrac {1}{h_{b}}}+{\dfrac {1}{h_{c}}}}}.}

The product of the incircle radius r{\displaystyle r} and the circumcircle radius R{\displaystyle R} of a triangle with sides a{\displaystyle a}, b{\displaystyle b}, and c{\displaystyle c} is[13]

rR=abc2(a+b+c).{\displaystyle rR={\frac {abc}{2(a+b+c)}}.}

Some relations among the sides, incircle radius, and circumcircle radius are:[14]

ab+bc+ca=s2+(4R+r)r,a2+b2+c2=2s22(4R+r)r.{\displaystyle {\begin{aligned}ab+bc+ca&=s^{2}+(4R+r)r,\\a^{2}+b^{2}+c^{2}&=2s^{2}-2(4R+r)r.\end{aligned}}}

Any line through a triangle that splits both the triangle's area and its perimeter in half goes through the triangle's incenter (the center of its incircle). There are either one, two, or three of these for any given triangle.[15]

The incircle radius is no greater than one-ninth the sum of the altitudes.[16]: 289

The squared distance from the incenter I{\displaystyle I} to the circumcenterO{\displaystyle O} is given by[17]: 232

OI¯2=R(R2r)=abca+b+c[abc(a+bc)(ab+c)(a+b+c)1]{\displaystyle {\overline {OI}}^{2}=R(R-2r)={\frac {a\,b\,c\,}{a+b+c}}\left[{\frac {a\,b\,c\,}{(a+b-c)\,(a-b+c)\,(-a+b+c)}}-1\right]}

and the distance from the incenter to the center N{\displaystyle N} of the nine point circle is[17]: 232

IN¯=12(R2r)<12R.{\displaystyle {\overline {IN}}={\tfrac {1}{2}}(R-2r)<{\tfrac {1}{2}}R.}

The incenter lies in the medial triangle (whose vertices are the midpoints of the sides).[17]: 233, Lemma 1

Relation to area of the triangle

The radius of the incircle is related to the area of the triangle.[18] The ratio of the area of the incircle to the area of the triangle is less than or equal to π/33{\displaystyle \pi {\big /}3{\sqrt {3}}}, with equality holding only for equilateral triangles.[19]

Suppose ABC{\displaystyle \triangle ABC} has an incircle with radius r{\displaystyle r} and center I{\displaystyle I}. Let a{\displaystyle a} be the length of BC¯{\displaystyle {\overline {BC}}}, b{\displaystyle b} the length of AC¯{\displaystyle {\overline {AC}}}, and c{\displaystyle c} the length of AB¯{\displaystyle {\overline {AB}}}.

Now, the incircle is tangent to AB¯{\displaystyle {\overline {AB}}} at some point TC{\displaystyle T_{C}}, and so ATCI{\displaystyle \angle AT_{C}I} is right. Thus, the radius TCI{\displaystyle T_{C}I} is an altitude of IAB{\displaystyle \triangle IAB}.

Therefore, IAB{\displaystyle \triangle IAB} has base length c{\displaystyle c} and height r{\displaystyle r}, and so has area 12cr{\displaystyle {\tfrac {1}{2}}cr}.

Proof without words that the area of a triangle equals the product of its inradius and its semiperimeter

Similarly, IAC{\displaystyle \triangle IAC} has area 12br{\displaystyle {\tfrac {1}{2}}br} and IBC{\displaystyle \triangle IBC} has area 12ar{\displaystyle {\tfrac {1}{2}}ar}.

Since these three triangles decompose ABC{\displaystyle \triangle ABC}, we see that the area Δ ofABC{\displaystyle \Delta {\text{ of}}\triangle ABC} is:

Δ=12(a+b+c)r=sr,{\displaystyle \Delta ={\tfrac {1}{2}}(a+b+c)r=sr,}

     and     r=Δs,{\displaystyle r={\frac {\Delta }{s}},}

where Δ{\displaystyle \Delta } is the area of ABC{\displaystyle \triangle ABC} and s=12(a+b+c){\displaystyle s={\tfrac {1}{2}}(a+b+c)} is its semiperimeter.

For an alternative formula, consider ITCA{\displaystyle \triangle IT_{C}A}. This is a right-angled triangle with one side equal to r{\displaystyle r} and the other side equal to rcotA2{\displaystyle r\cot {\tfrac {A}{2}}}. The same is true for IBA{\displaystyle \triangle IB'A}. The large triangle is composed of six such triangles and the total area is:

Δ=r2(cotA2+cotB2+cotC2).{\displaystyle \Delta =r^{2}\left(\cot {\tfrac {A}{2}}+\cot {\tfrac {B}{2}}+\cot {\tfrac {C}{2}}\right).}

Gergonne triangle and point

  Triangle ABC
  Incircle (incenter at I)
  Contact triangle TATBTC
  Lines between opposite vertices of ABC and TATBTC (concur at Gergonne point Ge)

The Gergonne triangle (of ABC{\displaystyle \triangle ABC}) is defined by connecting the three touchpoints of the incircle on the three sides. The touchpoint opposite A{\displaystyle A} is denoted TA{\displaystyle T_{A}}, etc.

This Gergonne triangle, TATBTC{\displaystyle \triangle T_{A}T_{B}T_{C}}, is also known as the contact triangle or intouch triangle of ABC{\displaystyle \triangle ABC}. Its area is

KT=K2r2sabc{\displaystyle K_{T}=K{\frac {2r^{2}s}{abc}}}

where K{\displaystyle K}, r{\displaystyle r}, and s{\displaystyle s} are the area, radius of the incircle, and semiperimeter of the original triangle, and a{\displaystyle a}, b{\displaystyle b}, and c{\displaystyle c} are the side lengths of the original triangle. This is the same area as that of the extouch triangle.[20]

The three lines ATA{\displaystyle AT_{A}}, BTB{\displaystyle BT_{B}}, and CTC{\displaystyle CT_{C}} intersect in a single point called the Gergonne point, denoted as Ge{\displaystyle G_{e}} (or triangle centerX7). The Gergonne point lies in the open orthocentroidal disk punctured at its own center, and can be any point therein.[21]

The Gergonne point of a triangle has a number of properties, including that it is the symmedian point of the Gergonne triangle.[22]

Trilinear coordinates for the vertices of the intouch triangle are given by

TA=0:sec2B2:sec2C2TB=sec2A2:0:sec2C2TC=sec2A2:sec2B2:0.{\displaystyle {\begin{array}{ccccccc}T_{A}&=&0&:&\sec ^{2}{\frac {B}{2}}&:&\sec ^{2}{\frac {C}{2}}\\[2pt]T_{B}&=&\sec ^{2}{\frac {A}{2}}&:&0&:&\sec ^{2}{\frac {C}{2}}\\[2pt]T_{C}&=&\sec ^{2}{\frac {A}{2}}&:&\sec ^{2}{\frac {B}{2}}&:&0.\end{array}}}

Trilinear coordinates for the Gergonne point are given by

sec2A2:sec2B2:sec2C2,{\displaystyle \sec ^{2}{\tfrac {A}{2}}:\sec ^{2}{\tfrac {B}{2}}:\sec ^{2}{\tfrac {C}{2}},}

or, equivalently, by the law of cosines,

bcb+ca:cac+ab:aba+bc.{\displaystyle {\frac {bc}{b+c-a}}:{\frac {ca}{c+a-b}}:{\frac {ab}{a+b-c}}.}

Excircles and excenters

  Extended sides of ABC
  Incircle (incenter at I)
  Excircles (excenters at JA, JB, JC)
  Internal angle bisectors
  External angle bisectors (forming the excentral triangle)

An excircle or escribed circle[2] of the triangle is a circle lying outside the triangle, tangent to one of its sides, and tangent to the extensions of the other two. Every triangle has three distinct excircles, each tangent to one of the triangle's sides.[3]

The center of an excircle is the intersection of the internal bisector of one angle (at vertex A{\displaystyle A}, for example) and the external bisectors of the other two. The center of this excircle is called the excenter relative to the vertex A{\displaystyle A}, or the excenter of A{\displaystyle A}.[3] Because the internal bisector of an angle is perpendicular to its external bisector, it follows that the center of the incircle together with the three excircle centers form an orthocentric system.[5]

Trilinear coordinates of excenters

While the incenter of ABC{\displaystyle \triangle ABC} has trilinear coordinates1:1:1{\displaystyle 1:1:1}, the excenters have trilinears

JA=1:1:1JB=1:1:1JC=1:1:1{\displaystyle {\begin{array}{rrcrcr}J_{A}=&-1&:&1&:&1\\J_{B}=&1&:&-1&:&1\\J_{C}=&1&:&1&:&-1\end{array}}}

Exradii

The radii of the excircles are called the exradii.

The exradius of the excircle opposite A{\displaystyle A} (so touching BC{\displaystyle BC}, centered at JA{\displaystyle J_{A}}) is[23][24]

ra=rssa=s(sb)(sc)sa,{\displaystyle r_{a}={\frac {rs}{s-a}}={\sqrt {\frac {s(s-b)(s-c)}{s-a}}},} where s=12(a+b+c).{\displaystyle s={\tfrac {1}{2}}(a+b+c).}

See Heron's formula.

Derivation of exradii formula

Source:[23]

Let the excircle at side AB{\displaystyle AB} touch at side AC{\displaystyle AC} extended at G{\displaystyle G}, and let this excircle's radius be rc{\displaystyle r_{c}} and its center be Jc{\displaystyle J_{c}}. Then JcG{\displaystyle J_{c}G} is an altitude of ACJc{\displaystyle \triangle ACJ_{c}}, so ACJc{\displaystyle \triangle ACJ_{c}} has area 12brc{\displaystyle {\tfrac {1}{2}}br_{c}}. By a similar argument, BCJc{\displaystyle \triangle BCJ_{c}} has area 12arc{\displaystyle {\tfrac {1}{2}}ar_{c}} and ABJc{\displaystyle \triangle ABJ_{c}} has area 12crc{\displaystyle {\tfrac {1}{2}}cr_{c}}. Thus the area Δ{\displaystyle \Delta } of triangle ABC{\displaystyle \triangle ABC} is

Δ=12(a+bc)rc=(sc)rc{\displaystyle \Delta ={\tfrac {1}{2}}(a+b-c)r_{c}=(s-c)r_{c}}.

So, by symmetry, denoting r{\displaystyle r} as the radius of the incircle,

Δ=sr=(sa)ra=(sb)rb=(sc)rc{\displaystyle \Delta =sr=(s-a)r_{a}=(s-b)r_{b}=(s-c)r_{c}}.

By the Law of Cosines, we have

cosA=b2+c2a22bc{\displaystyle \cos A={\frac {b^{2}+c^{2}-a^{2}}{2bc}}}

Combining this with the identity sin2A+cos2A=1{\displaystyle \sin ^{2}\!A+\cos ^{2}\!A=1}, we have

sinA=a4b4c4+2a2b2+2b2c2+2a2c22bc{\displaystyle \sin A={\frac {\sqrt {-a^{4}-b^{4}-c^{4}+2a^{2}b^{2}+2b^{2}c^{2}+2a^{2}c^{2}}}{2bc}}}

But Δ=12bcsinA{\displaystyle \Delta ={\tfrac {1}{2}}bc\sin A}, and so

Δ=14a4b4c4+2a2b2+2b2c2+2a2c2=14(a+b+c)(a+b+c)(ab+c)(a+bc)=s(sa)(sb)(sc),{\displaystyle {\begin{aligned}\Delta &={\tfrac {1}{4}}{\sqrt {-a^{4}-b^{4}-c^{4}+2a^{2}b^{2}+2b^{2}c^{2}+2a^{2}c^{2}}}\\[5mu]&={\tfrac {1}{4}}{\sqrt {(a+b+c)(-a+b+c)(a-b+c)(a+b-c)}}\\[5mu]&={\sqrt {s(s-a)(s-b)(s-c)}},\end{aligned}}}

which is Heron's formula.

Combining this with sr=Δ{\displaystyle sr=\Delta }, we have

r2=Δ2s2=(sa)(sb)(sc)s.{\displaystyle r^{2}={\frac {\Delta ^{2}}{s^{2}}}={\frac {(s-a)(s-b)(s-c)}{s}}.}

Similarly, (sa)ra=Δ{\displaystyle (s-a)r_{a}=\Delta } gives

ra2=s(sb)(sc)sara=s(sb)(sc)sa.{\displaystyle {\begin{aligned}&r_{a}^{2}={\frac {s(s-b)(s-c)}{s-a}}\\[4pt]&\implies r_{a}={\sqrt {\frac {s(s-b)(s-c)}{s-a}}}.\end{aligned}}}

Other properties

From the formulas above one can see that the excircles are always larger than the incircle and that the largest excircle is the one tangent to the longest side and the smallest excircle is tangent to the shortest side. Further, combining these formulas yields:[25]

Δ=rrarbrc.{\displaystyle \Delta ={\sqrt {rr_{a}r_{b}r_{c}}}.}

Other excircle properties

The circular hull of the excircles is internally tangent to each of the excircles and is thus an Apollonius circle.[26] The radius of this Apollonius circle is r2+s24r{\displaystyle {\tfrac {r^{2}+s^{2}}{4r}}} where r{\displaystyle r} is the incircle radius and s{\displaystyle s} is the semiperimeter of the triangle.[27]

The following relations hold among the inradius r{\displaystyle r}, the circumradius R{\displaystyle R}, the semiperimeter s{\displaystyle s}, and the excircle radii ra{\displaystyle r_{a}}, rb{\displaystyle r_{b}}, rc{\displaystyle r_{c}}:[14]

ra+rb+rc=4R+r,rarb+rbrc+rcra=s2,ra2+rb2+rc2=(4R+r)22s2.{\displaystyle {\begin{aligned}r_{a}+r_{b}+r_{c}&=4R+r,\\r_{a}r_{b}+r_{b}r_{c}+r_{c}r_{a}&=s^{2},\\r_{a}^{2}+r_{b}^{2}+r_{c}^{2}&=\left(4R+r\right)^{2}-2s^{2}.\end{aligned}}}

The circle through the centers of the three excircles has radius 2R{\displaystyle 2R}.[14]

If H{\displaystyle H} is the orthocenter of ABC{\displaystyle \triangle ABC}, then[14]

ra+rb+rc+r=AH¯+BH¯+CH¯+2R,ra2+rb2+rc2+r2=AH¯2+BH¯2+CH¯2+(2R)2.{\displaystyle {\begin{aligned}r_{a}+r_{b}+r_{c}+r&={\overline {AH}}+{\overline {BH}}+{\overline {CH}}+2R,\\r_{a}^{2}+r_{b}^{2}+r_{c}^{2}+r^{2}&={\overline {AH}}^{2}+{\overline {BH}}^{2}+{\overline {CH}}^{2}+(2R)^{2}.\end{aligned}}}

Nagel triangle and Nagel point

  Extended sides of triangle ABC
  Excircles of ABC (tangent at TA. TB, TC)
  Nagel/Extouch triangleTATBTC
  Splitters: lines connecting opposite vertices of ABC and TATBTC (concur at Nagel pointN)

The Nagel triangle or extouch triangle of ABC{\displaystyle \triangle ABC} is denoted by the vertices TA{\displaystyle T_{A}}, TB{\displaystyle T_{B}}, and TC{\displaystyle T_{C}} that are the three points where the excircles touch the reference ABC{\displaystyle \triangle ABC} and where TA{\displaystyle T_{A}} is opposite of A{\displaystyle A}, etc. This TATBTC{\displaystyle \triangle T_{A}T_{B}T_{C}} is also known as the extouch triangle of ABC{\displaystyle \triangle ABC}. The circumcircle of the extouch TATBTC{\displaystyle \triangle T_{A}T_{B}T_{C}} is called the Mandart circle (cf. Mandart inellipse).

The three line segments ATA¯{\displaystyle {\overline {AT_{A}}}}, BTB¯{\displaystyle {\overline {BT_{B}}}} and CTC¯{\displaystyle {\overline {CT_{C}}}} are called the splitters of the triangle; they each bisect the perimeter of the triangle,

AB¯+BTA¯=AC¯+CTA¯=12(AB¯+BC¯+AC¯).{\displaystyle {\overline {AB}}+{\overline {BT_{A}}}={\overline {AC}}+{\overline {CT_{A}}}={\frac {1}{2}}\left({\overline {AB}}+{\overline {BC}}+{\overline {AC}}\right).}

The splitters intersect in a single point, the triangle's Nagel pointNa{\displaystyle N_{a}} (or triangle centerX8).

Trilinear coordinates for the vertices of the extouch triangle are given by

TA=0:csc2B2:csc2C2TB=csc2A2:0:csc2C2TC=csc2A2:csc2B2:0{\displaystyle {\begin{array}{ccccccc}T_{A}&=&0&:&\csc ^{2}{\frac {B}{2}}&:&\csc ^{2}{\frac {C}{2}}\\[2pt]T_{B}&=&\csc ^{2}{\frac {A}{2}}&:&0&:&\csc ^{2}{\frac {C}{2}}\\[2pt]T_{C}&=&\csc ^{2}{\frac {A}{2}}&:&\csc ^{2}{\frac {B}{2}}&:&0\end{array}}}

Trilinear coordinates for the Nagel point are given by

csc2A2:csc2B2:csc2C2,{\displaystyle \csc ^{2}{\tfrac {A}{2}}:\csc ^{2}{\tfrac {B}{2}}:\csc ^{2}{\tfrac {C}{2}},}

or, equivalently, by the Law of Sines,

b+caa:c+abb:a+bcc.{\displaystyle {\frac {b+c-a}{a}}:{\frac {c+a-b}{b}}:{\frac {a+b-c}{c}}.}

Barycentric coordinates for the Nagel point are therefore

b+ca:c+ab:a+bc,{\displaystyle b+c-a:c+a-b:a+b-c,}

or equivalently

sa:sb:sc.{\displaystyle s-a:s-b:s-c.}

The Nagel point is the isotomic conjugate of the Gergonne point.

Nine-point circle and Feuerbach point

The nine-point circle is tangent to the incircle and excircles

In geometry, the nine-point circle is a circle that can be constructed for any given triangle. It is so named because it passes through nine significant concyclic points defined from the triangle. These nine points are:[28][29]

In 1822, Karl Feuerbach discovered that any triangle's nine-point circle is externally tangent to that triangle's three excircles and internally tangent to its incircle; this result is known as Feuerbach's theorem. He proved that:[30]

... the circle which passes through the feet of the altitudes of a triangle is tangent to all four circles which in turn are tangent to the three sides of the triangle ... (Feuerbach 1822)

The triangle center at which the incircle and the nine-point circle touch is called the Feuerbach point.

The incircle may be described as the pedal circle of the incenter. The locus of points whose pedal circles are tangent to the nine-point circle is known as the McCay cubic.

Incentral and excentral triangles

The points of intersection of the interior angle bisectors of ABC{\displaystyle \triangle ABC} with the segments BC{\displaystyle BC}, CA{\displaystyle CA}, and AB{\displaystyle AB} are the vertices of the incentral triangle. Trilinear coordinates for the vertices of the incentral triangle ABC{\displaystyle \triangle A'B'C'} are given by

A=0:1:1B=1:0:1C=1:1:0{\displaystyle {\begin{array}{ccccccc}A'&=&0&:&1&:&1\\[2pt]B'&=&1&:&0&:&1\\[2pt]C'&=&1&:&1&:&0\end{array}}}

The excentral triangle of a reference triangle has vertices at the centers of the reference triangle's excircles. Its sides are on the external angle bisectors of the reference triangle (see figure at top of page). Trilinear coordinates for the vertices of the excentral triangle ABC{\displaystyle \triangle A'B'C'} are given by

A=1:1:1B=1:1:1C=1:1:1{\displaystyle {\begin{array}{ccrcrcr}A'&=&-1&:&1&:&1\\[2pt]B'&=&1&:&-1&:&1\\[2pt]C'&=&1&:&1&:&-1\end{array}}}

Equations for four circles

Let x:y:z{\displaystyle x:y:z} be a variable point in trilinear coordinates, and let u=cos2(A/2){\displaystyle u=\cos ^{2}\left(A/2\right)}, v=cos2(B/2){\displaystyle v=\cos ^{2}\left(B/2\right)}, w=cos2(C/2){\displaystyle w=\cos ^{2}\left(C/2\right)}. The four circles described above are given equivalently by either of the two given equations:[31]: 210–215

  • Incircle:u2x2+v2y2+w2z22vwyz2wuzx2uvxy=0±xcosA2±ytcosB2±zcosC2=0{\displaystyle {\begin{aligned}u^{2}x^{2}+v^{2}y^{2}+w^{2}z^{2}-2vwyz-2wuzx-2uvxy&=0\\[4pt]{\textstyle \pm {\sqrt {x}}\cos {\tfrac {A}{2}}\pm {\sqrt {y{\vphantom {t}}}}\cos {\tfrac {B}{2}}\pm {\sqrt {z}}\cos {\tfrac {C}{2}}}&=0\end{aligned}}}
  • A{\displaystyle A}-excircle:u2x2+v2y2+w2z22vwyz+2wuzx+2uvxy=0±xcosA2±ytcosB2±zcosC2=0{\displaystyle {\begin{aligned}u^{2}x^{2}+v^{2}y^{2}+w^{2}z^{2}-2vwyz+2wuzx+2uvxy&=0\\[4pt]{\textstyle \pm {\sqrt {-x}}\cos {\tfrac {A}{2}}\pm {\sqrt {y{\vphantom {t}}}}\cos {\tfrac {B}{2}}\pm {\sqrt {z}}\cos {\tfrac {C}{2}}}&=0\end{aligned}}}
  • B{\displaystyle B}-excircle:u2x2+v2y2+w2z2+2vwyz2wuzx+2uvxy=0±xcosA2±ytcosB2±zcosC2=0{\displaystyle {\begin{aligned}u^{2}x^{2}+v^{2}y^{2}+w^{2}z^{2}+2vwyz-2wuzx+2uvxy&=0\\[4pt]{\textstyle \pm {\sqrt {x}}\cos {\tfrac {A}{2}}\pm {\sqrt {-y{\vphantom {t}}}}\cos {\tfrac {B}{2}}\pm {\sqrt {z}}\cos {\tfrac {C}{2}}}&=0\end{aligned}}}
  • C{\displaystyle C}-excircle:u2x2+v2y2+w2z2+2vwyz+2wuzx2uvxy=0±xcosA2±ytcosB2±zcosC2=0{\displaystyle {\begin{aligned}u^{2}x^{2}+v^{2}y^{2}+w^{2}z^{2}+2vwyz+2wuzx-2uvxy&=0\\[4pt]{\textstyle \pm {\sqrt {x}}\cos {\tfrac {A}{2}}\pm {\sqrt {y{\vphantom {t}}}}\cos {\tfrac {B}{2}}\pm {\sqrt {-z}}\cos {\tfrac {C}{2}}}&=0\end{aligned}}}

Euler's theorem

Euler's theorem states that in a triangle:

(Rr)2=d2+r2,{\displaystyle (R-r)^{2}=d^{2}+r^{2},}

where R{\displaystyle R} and r{\displaystyle r} are the circumradius and inradius respectively, and d{\displaystyle d} is the distance between the circumcenter and the incenter.

For excircles the equation is similar:

(R+rex)2=dex2+rex2,{\displaystyle \left(R+r_{\text{ex}}\right)^{2}=d_{\text{ex}}^{2}+r_{\text{ex}}^{2},}

where rex{\displaystyle r_{\text{ex}}} is the radius of one of the excircles, and dex{\displaystyle d_{\text{ex}}} is the distance between the circumcenter and that excircle's center.[32][33][34]

Generalization to other polygons

Some (but not all) quadrilaterals have an incircle. These are called tangential quadrilaterals. Among their many properties, perhaps the most important is that their two pairs of opposite sides have equal sums. This is called the Pitot theorem.[35]

More generally, a polygon with any number of sides that has an inscribed circle (that is, one that is tangent to each side) is called a tangential polygon.

Generalization to topological triangles

If topological triangles are considered, it is still possible to define an inscribed circle. It is no longer described as tangent to all sides, since the topological triangle might not be differentiable everywhere. Rather, it is defined as a circle whose center has the same minimal distance to each side. It has been proven that all topological triangles have an inscribed circle.[36]

See also

Notes

  1. ^Kay (1969, p. 140)
  2. ^ abAltshiller-Court (1925, p. 74)
  3. ^ abcdeAltshiller-Court (1925, p. 73)
  4. ^Kay (1969, p. 117)
  5. ^ abJohnson 1929, p. 182.
  6. ^ abEncyclopedia of Triangle CentersArchived 2012-04-19 at the Wayback Machine, accessed 2014-10-28.
  7. ^Kay (1969, p. 201)
  8. ^Chu, Thomas, The Pentagon, Spring 2005, p. 45, problem 584.
  9. ^Allaire, Patricia R.; Zhou, Junmin; Yao, Haishen (March 2012), "Proving a nineteenth century ellipse identity", Mathematical Gazette, 96: 161–165, doi:10.1017/S0025557200004277, S2CID 124176398.
  10. ^Altshiller-Court, Nathan (1980), College Geometry, Dover Publications. #84, p. 121.
  11. ^Mathematical Gazette, July 2003, 323-324.
  12. ^Kay (1969, p. 203)
  13. ^Johnson 1929, p. 189, #298(d).
  14. ^ abcdBell, Amy. ""Hansen's right triangle theorem, its converse and a generalization", Forum Geometricorum 6, 2006, 335–342"(PDF). Archived from the original(PDF) on 2021-08-31. Retrieved 2012-05-05.
  15. ^Kodokostas, Dimitrios, "Triangle Equalizers", Mathematics Magazine 83, April 2010, pp. 141-146.
  16. ^Posamentier, Alfred S., and Lehmann, Ingmar. The Secrets of Triangles, Prometheus Books, 2012.
  17. ^ abcFranzsen, William N. (2011). "The distance from the incenter to the Euler line"(PDF). Forum Geometricorum. 11: 231–236. MR 2877263. Archived from the original(PDF) on 2020-12-05. Retrieved 2012-05-09..
  18. ^Coxeter, H.S.M. "Introduction to Geometry 2nd ed. Wiley, 1961.
  19. ^Minda, D., and Phelps, S., "Triangles, ellipses, and cubic polynomials", American Mathematical Monthly 115, October 2008, 679-689: Theorem 4.1.
  20. ^ Weisstein, Eric W. "Contact Triangle." From MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/ContactTriangle.html
  21. ^Christopher J. Bradley and Geoff C. Smith, "The locations of triangle centers", Forum Geometricorum 6 (2006), 57–70. http://forumgeom.fau.edu/FG2006volume6/FG200607index.htmlArchived 2016-03-04 at the Wayback Machine
  22. ^Dekov, Deko (2009). "Computer-generated Mathematics : The Gergonne Point"(PDF). Journal of Computer-generated Euclidean Geometry. 1: 1–14. Archived from the original(PDF) on 2010-11-05.
  23. ^ abAltshiller-Court (1925, p. 79)
  24. ^Kay (1969, p. 202)
  25. ^Baker, Marcus, "A collection of formulae for the area of a plane triangle", Annals of Mathematics, part 1 in vol. 1(6), January 1885, 134-138. (See also part 2 in vol. 2(1), September 1885, 11-18.)
  26. ^"Grinberg, Darij, and Yiu, Paul, "The Apollonius Circle as a Tucker Circle", Forum Geometricorum 2, 2002: pp. 175-182"(PDF). Archived from the original(PDF) on 2023-06-25. Retrieved 2012-05-02.
  27. ^"Stevanovi´c, Milorad R., "The Apollonius circle and related triangle centers", Forum Geometricorum 3, 2003, 187-195"(PDF). Archived from the original(PDF) on 2022-10-06. Retrieved 2012-05-03.
  28. ^Altshiller-Court (1925, pp. 103–110)
  29. ^Kay (1969, pp. 18, 245)
  30. ^Feuerbach, Karl Wilhelm; Buzengeiger, Carl Heribert Ignatz (1822), Eigenschaften einiger merkwürdigen Punkte des geradlinigen Dreiecks und mehrerer durch sie bestimmten Linien und Figuren. Eine analytisch-trigonometrische Abhandlung (in German) (Monograph ed.), Nürnberg: Wiessner.
  31. ^Whitworth, William Allen. Trilinear Coordinates and Other Methods of Modern Analytical Geometry of Two Dimensions, Forgotten Books, 2012 (orig. Deighton, Bell, and Co., 1866). https://www.forgottenbooks.com/en/search?q=%22Trilinear+coordinates%22
  32. ^Nelson, Roger, "Euler's triangle inequality via proof without words", Mathematics Magazine 81(1), February 2008, 58-61.
  33. ^Johnson 1929, p. 187.
  34. ^"Emelyanov, Lev, and Emelyanova, Tatiana. "Euler's formula and Poncelet's porism", Forum Geometricorum 1, 2001: pp. 137–140"(PDF). Archived from the original(PDF) on 2023-01-17. Retrieved 2012-05-02.
  35. ^Josefsson (2011, See in particular pp. 65–66.)
  36. ^Al-Ajrawi, Ezzaddin (20 October 2024). "Inscribing Spheres in Topologically Embedded Simplices". The American Mathematical Monthly. 131 (9): 806–813. doi:10.1080/00029890.2024.2380233. ISSN 0002-9890.

References

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