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Incenter
Incenter
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The point of intersection of angle bisectors of the 3 angles of triangle ABC is the incenter (denoted by I). The incircle (whose center is I) touches each side of the triangle.

In geometry, the incenter of a triangle is a triangle center, a point defined for any triangle in a way that is independent of the triangle's placement or scale. The incenter may be equivalently defined as the point where the internal angle bisectors of the triangle cross, as the point equidistant from the triangle's sides, as the junction point of the medial axis and innermost point of the grassfire transform of the triangle, and as the center point of the inscribed circle of the triangle.

Together with the centroid, circumcenter, and orthocenter, it is one of the four triangle centers known to the ancient Greeks, and the only one of the four that does not in general lie on the Euler line. It is the first listed center, X(1), in Clark Kimberling's Encyclopedia of Triangle Centers, and the identity element of the multiplicative group of triangle centers.[1][2]

For polygons with more than three sides, the incenter only exists for tangential polygons: those that have an incircle that is tangent to each side of the polygon. In this case the incenter is the center of this circle and is equally distant from all sides.

Definition and construction

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It is a theorem in Euclidean geometry that the three interior angle bisectors of a triangle meet in a single point. In Euclid's Elements, Proposition 4 of Book IV proves that this point is also the center of the inscribed circle of the triangle. The incircle itself may be constructed by dropping a perpendicular from the incenter to one of the sides of the triangle and drawing a circle with that segment as its radius.[3]

The incenter lies at equal distances from the three line segments forming the sides of the triangle, and also from the three lines containing those segments. It is the only point equally distant from the line segments, but there are three more points equally distant from the lines, the excenters, which form the centers of the excircles of the given triangle. The incenter and excenters together form an orthocentric system.[4]

The medial axis of a polygon is the set of points whose nearest neighbor on the polygon is not unique: these points are equidistant from two or more sides of the polygon. One method for computing medial axes is using the grassfire transform, in which one forms a continuous sequence of offset curves, each at some fixed distance from the polygon; the medial axis is traced out by the vertices of these curves. In the case of a triangle, the medial axis consists of three segments of the angle bisectors, connecting the vertices of the triangle to the incenter, which is the unique point on the innermost offset curve.[5] The straight skeleton, defined in a similar way from a different type of offset curve, coincides with the medial axis for convex polygons and so also has its junction at the incenter.[6]

Proofs

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Ratio proof

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Let the bisection of and meet at , and the bisection of and meet at , and and meet at .

And let and meet at .

Then we have to prove that is the bisection of .

In , , by the Angle bisector theorem.

In , .

Therefore, , so that .

So is the bisection of .

Perpendicular proof

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A line that is an angle bisector is equidistant from both of its lines when measuring by the perpendicular. At the point where two bisectors intersect, this point is perpendicularly equidistant from the final angle's forming lines (because they are the same distance from this angles opposite edge), and therefore lies on its angle bisector line.

Relation to triangle sides and vertices

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Trilinear coordinates

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The trilinear coordinates for a point in the triangle give the ratio of distances to the triangle sides. Trilinear coordinates for the incenter are given by[2]

The collection of triangle centers may be given the structure of a group under coordinatewise multiplication of trilinear coordinates; in this group, the incenter forms the identity element.[2]

Barycentric coordinates

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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

where , , and are the lengths of the sides of the triangle, or equivalently (using the law of sines) by

where , , and are the angles at the three vertices.

Cartesian coordinates

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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—i.e., 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 , , and , and the sides opposite these vertices have corresponding lengths , , and , then the incenter is at

Distances to vertices

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Denoting the incenter of triangle ABC as I, the distances from the incenter to the vertices combined with the lengths of the triangle sides obey the equation[7]

Additionally,[8]

where R and r are the triangle's circumradius and inradius respectively.

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Other centers

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The distance from the incenter to the centroid is less than one third the length of the longest median of the triangle.[9]

By Euler's theorem in geometry, the squared distance from the incenter I to the circumcenter O is given by[10][11]

where R and r are the circumradius and the inradius respectively; thus the circumradius is at least twice the inradius, with equality only in the equilateral case.[12]

The distance from the incenter to the center N of the nine point circle is[11]

The squared distance from the incenter to the orthocenter H is[13]

Inequalities include:

The incenter is the Nagel point of the medial triangle (the triangle whose vertices are the midpoints of the sides) and therefore lies inside this triangle. Conversely the Nagel point of any triangle is the incenter of its anticomplementary triangle.[14]

The incenter must lie in the interior of a disk whose diameter connects the centroid G and the orthocenter H (the orthocentroidal disk), but it cannot coincide with the nine-point center, whose position is fixed 1/4 of the way along the diameter (closer to G). Any other point within the orthocentroidal disk is the incenter of a unique triangle.[15]

Euler line

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The Euler line of a triangle is a line passing through its circumcenter, centroid, and orthocenter, among other points. The incenter generally does not lie on the Euler line;[16] it is on the Euler line only for isosceles triangles,[17] for which the Euler line coincides with the symmetry axis of the triangle and contains all triangle centers.

Denoting the distance from the incenter to the Euler line as d, the length of the longest median as v, the length of the longest side as u, the circumradius as R, the length of the Euler line segment from the orthocenter to the circumcenter as e, and the semiperimeter as s, the following inequalities hold:[18]

Area and perimeter splitters

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Any line through a triangle that splits both the triangle's area and its perimeter in half goes through the triangle's incenter; every line through the incenter that splits the area in half also splits the perimeter in half. There are either one, two, or three of these lines for any given triangle.[19]

Relative distances from an angle bisector

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Let X be a variable point on the internal angle bisector of A. Then X = I (the incenter) maximizes or minimizes the ratio along that angle bisector.[20][21]

References

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
In , the incenter of a is the point where the three angle bisectors intersect, and it serves as the center of the incircle—the largest circle that fits inside the and is tangent to all three sides. This point is always located inside the , regardless of whether it is acute, right, or obtuse, and it represents the unique point equidistant from all three sides, with the perpendicular distance to each side equal to the inradius rr. The incenter has barycentric coordinates (a:b:c)(a : b : c) with respect to the triangle's vertices, where aa, bb, and cc are the lengths of the sides opposite those vertices, respectively; this weighting reflects its position as a balance point influenced by the side lengths. The inradius rr is given by the formula r=Asr = \frac{A}{s}, where AA is the area of the triangle and s=a+b+c2s = \frac{a + b + c}{2} is the semiperimeter. Key theorems related to the incenter include the concurrency of the angle bisectors, ensuring its existence and uniqueness in any triangle, and the angle bisector theorem, which describes how each bisector divides the opposite side in the ratio of the adjacent sides. The incenter's significance extends to applications in geometry, such as constructing incircles. The concept generalizes to tangential polygons, where the incenter is the center of the inscribed tangent to all sides. In coordinate , for a with vertices at (x1,y1)(x_1, y_1), (x2,y2)(x_2, y_2), and (x3,y3)(x_3, y_3), the incenter's Cartesian coordinates are (ax1+bx2+cx3a+b+c,ay1+by2+cy3a+b+c)\left( \frac{a x_1 + b x_2 + c x_3}{a + b + c}, \frac{a y_1 + b y_2 + c y_3}{a + b + c} \right), providing a practical way to locate it computationally.

Definition and Properties

Definition

In a , the incenter is the unique point of concurrency of the three internal bisectors, each of which divides one of the 's angles into two equal parts. This point serves as the center of the incircle, the largest circle that fits inside the and is to all three sides. The incircle touches each side of the at precisely one point, and the from the incenter to any side equals the circle's , known as the inradius and denoted by [r](/page/R)[r](/page/R). This configuration ensures the incircle is fully contained within the without intersecting its interior otherwise. The incenter holds a prominent place in classical as one of the four primary centers, alongside the , circumcenter, and orthocenter, with its properties first systematically described in mathematics. Euclid's Elements (Book IV, Proposition 4) establishes the existence of the incircle and its inscription in a , laying foundational groundwork for understanding the incenter.

Fundamental Properties

The incenter of a triangle is the unique point inside the triangle that is equidistant from all three sides, with this common distance being the inradius rr. This equidistance property arises from the incenter's role as the center of the incircle, which is tangent to each side. The inradius rr is given by the formula r=A/sr = A / s, where AA is the area of the triangle and s=(a+b+c)/2s = (a + b + c)/2 is the semiperimeter, with aa, bb, and cc denoting the side lengths. Alternative expressions for the inradius include r=(sa)tan(A/2)r = (s - a) \tan(A/2), where AA is the angle opposite side aa, and r=4Rsin(A/2)sin(B/2)sin(C/2)r = 4R \sin(A/2) \sin(B/2) \sin(C/2), where RR is the circumradius and AA, BB, CC are the angles of the triangle. The points of tangency of the incircle with the sides divide each side into segments whose lengths are determined by the semiperimeter: specifically, the segments adjacent to vertex AA (opposite side aa) are each of length sas - a, those adjacent to BB are sbs - b, and those adjacent to CC are scs - c. The incenter lies inside the regardless of whether the triangle is acute, right, or obtuse.

Construction and Proofs

Geometric Construction

The classical geometric construction of the incenter in a triangle relies on drawing the internal angle bisectors from each vertex using a compass and straightedge, a method rooted in Euclid's Elements, Book I, Proposition 9. To bisect an angle at a vertex, place the compass point at the vertex and draw an arc that intersects the two adjacent sides of the triangle at points P and Q. Then, with the compass set to the same radius, draw two arcs from P and Q that intersect at a point R inside the angle; the straight line from the vertex through R is the angle bisector. Repeating this process for all three angles yields lines that concur at the incenter. An alternative approach constructs only two angle bisectors, as their intersection point serves as the incenter, with the third bisector passing through it by the concurrency property; this verification step confirms the location without drawing the full set of bisectors. Another method begins by locating the points of tangency of the incircle on each side, exploiting the equal tangent lengths from the vertices. Using the compass to copy and add side lengths along a straight line to form the perimeter, halve it to obtain the semiperimeter s, then subtract each side length to find s - a, s - b, and s - c; mark these distances from the vertices along the sides to position the tangency points. Erect perpendiculars to the sides at these points with the compass and straightedge—their intersection is the incenter, as these radii are normal to the tangents. These constructions require a for arcs and circle segments to ensure equal radii during bisections and perpendiculars, and a for connecting points and extending lines. As angle bisection is a fundamental Euclidean operation, the incenter admits exact construction within classical .

Proofs of Key Theorems

The concurrency of the angle bisectors in a is a foundational property establishing the of the incenter. Consider ABCABC with sides a=BCa = BC, b=ACb = AC, and c=ABc = AB. Let the angle bisector from vertex AA intersect side BCBC at DD, from BB intersect CACA at EE, and from CC intersect ABAB at FF. By the angle bisector theorem, the bisector from AA divides BCBC such that BDDC=ABAC=cb\frac{BD}{DC} = \frac{AB}{AC} = \frac{c}{b}. Similarly, the bisector from BB divides CACA such that CEEA=ac\frac{CE}{EA} = \frac{a}{c}, and the bisector from CC divides ABAB such that AFFB=ba\frac{AF}{FB} = \frac{b}{a}. states that three cevians ADAD, BEBE, and CFCF are concurrent if and only if (BDDC)(CEEA)(AFFB)=1\left( \frac{BD}{DC} \right) \left( \frac{CE}{EA} \right) \left( \frac{AF}{FB} \right) = 1. Substituting the ratios yields cbacba=1\frac{c}{b} \cdot \frac{a}{c} \cdot \frac{b}{a} = 1, confirming concurrency at a single point, the incenter. This concurrency was established in antiquity, as Proposition 4 of Book IV in Euclid's Elements demonstrates the construction of an inscribed circle by intersecting angle bisectors and verifying the center's properties, implying their common intersection. The equidistance of the incenter from the triangle's sides follows directly from its position on the angle bisectors. The angle bisector from a vertex is the locus of points equidistant from the adjacent sides; to see this, consider a point PP on the bisector of BAC\angle BAC. Drop perpendiculars from PP to sides ABAB and ACAC, meeting at MM and NN, respectively. The right triangles PMAPMA and PNAPNA share hypotenuse segments along the bisector and have equal angles at AA (each half of BAC\angle BAC) and right angles at MM and NN, making them congruent by AAS; thus, PM=PNPM = PN. Since the incenter II lies on the bisector from AA, its perpendicular distances to ABAB and ACAC are equal. Similarly, lying on the bisector from BB equates distances to BABA and BCBC, and on the bisector from CC equates distances to CACA and CBCB. Therefore, the distances from II to all three sides are equal. These proofs assume a non-degenerate with positive area; if the vertices are collinear, the angle bisectors do not concur at a finite point inside the figure.

Coordinate Systems

Trilinear and Barycentric Coordinates

In trilinear coordinates, the incenter of a is represented as (1:1:1)(1 : 1 : 1), indicating that it is equidistant from the three sides in the normalized areal sense inherent to this homogeneous system. This simple form underscores the incenter's role as the intersection point of the angle bisectors, where the perpendicular distances to the sides are equal, corresponding to the inradius. In barycentric coordinates, the incenter has the form (a:b:c)(a : b : c), where aa, bb, and cc denote the lengths of the sides opposite vertices AA, BB, and CC, respectively. Equivalently, these coordinates can be expressed as (sinA:sinB:sinC)(\sin A : \sin B : \sin C), leveraging the law of sines which establishes the proportionality asinAa \propto \sin A, bsinBb \propto \sin B, and csinCc \propto \sin C. To obtain the normalized barycentric coordinates that sum to 1, divide each component by the total a+b+ca + b + c, yielding (aa+b+c:ba+b+c:ca+b+c)\left( \frac{a}{a+b+c} : \frac{b}{a+b+c} : \frac{c}{a+b+c} \right). This normalization arises from viewing the incenter as the center of mass of the triangle's vertices, weighted by the opposite side lengths, which geometrically balances the influences from each vertex according to the perimeter contributions. Trilinear coordinates prove advantageous for analyzing angle-related properties of the incenter, such as bisector intersections, due to their direct tie to side distances. In contrast, barycentric coordinates facilitate mass-point interpretations and area-based computations, making them ideal for concurrency proofs and cevian nestings involving the incenter. The incenter is cataloged as X(1) in the Encyclopedia of Triangle Centers.

Cartesian Coordinates

The Cartesian coordinates of the incenter II of a with vertices A(xA,yA)A(x_A, y_A), B(xB,yB)B(x_B, y_B), and C(xC,yC)C(x_C, y_C), and opposite side lengths a=BCa = BC, b=ACb = AC, and c=ABc = AB, are given by the weighted average formula: I=(axA+bxB+cxCa+b+c,ayA+byB+cyCa+b+c).I = \left( \frac{a x_A + b x_B + c x_C}{a + b + c}, \frac{a y_A + b y_B + c y_C}{a + b + c} \right). This expression arises from the incenter's barycentric coordinates (a:b:c)(a : b : c), which are normalized by dividing by the total weight a+b+c=2sa + b + c = 2s, where ss is the semiperimeter, to obtain the actual position in the plane as a of the vertices. To derive this, consider the incenter as the intersection of the angle bisectors, which divides each bisector in the ratio of the adjacent sides; however, the barycentric approach provides a direct path by assigning masses proportional to the side lengths at the vertices, ensuring the center of mass lies at the incenter due to the equal perpendicular distances (the inradius) to the sides. The resulting coordinates are then the normalized sum, confirming the formula as the unique point equidistant from all sides in the . For example, consider a right-angled with vertices A(0,0)A(0,0), B(1,0)B(1,0), and C(0,1)C(0,1). The side lengths are a=2a = \sqrt{2}
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