Heron's formula

In geometry, Heron's formula (or Hero's formula) gives the area of a triangle in terms of the three side lengths ${\displaystyle a,}$ ${\displaystyle b,}$ ${\displaystyle c.}$ Letting ${\displaystyle s}$ be the semiperimeter of the triangle, ${\displaystyle s={\tfrac {1}{2}}(a+b+c),}$ the area ${\displaystyle A}$ is^[1]

${\displaystyle A={\sqrt {s(s-a)(s-b)(s-c)}}.}$

It is named after first-century engineer Heron of Alexandria (or Hero) who proved it in his work Metrica, though it was probably known centuries earlier.

Example

Let ${\displaystyle \triangle ABC}$ be the triangle with sides ${\displaystyle a=4,}$ ${\displaystyle b=13,}$ and ${\displaystyle c=15.}$ This triangle's semiperimeter is ${\displaystyle s={\tfrac {1}{2}}(a+b+c)={}}$${\displaystyle {\tfrac {1}{2}}(4+13+15)=16}$ and so the area is

${\displaystyle {\begin{aligned}A&={\sqrt {s(s-a)(s-b)(s-c)}}={\sqrt {16\cdot (16-4)\cdot (16-13)\cdot (16-15)}}\\&={\sqrt {16\cdot 12\cdot 3\cdot 1}}={\sqrt {576}}=24.\end{aligned}}}$

In this example, the side lengths and area are integers, making it a Heronian triangle. However, Heron's formula works equally well in cases where one or more of the side lengths are not integers.

Alternate expressions

Heron's formula can also be written in terms of just the side lengths instead of using the semiperimeter, in several ways,

${\displaystyle {\begin{aligned}A&={\tfrac {1}{4}}{\sqrt {(a+b+c)(-a+b+c)(a-b+c)(a+b-c)}}\\[6mu]&={\tfrac {1}{4}}{\sqrt {2(a^{2}b^{2}+a^{2}c^{2}+b^{2}c^{2})-(a^{4}+b^{4}+c^{4})}}\\[6mu]&={\tfrac {1}{4}}{\sqrt {(a^{2}+b^{2}+c^{2})^{2}-2(a^{4}+b^{4}+c^{4})}}\\[6mu]&={\tfrac {1}{4}}{\sqrt {4(a^{2}b^{2}+a^{2}c^{2}+b^{2}c^{2})-(a^{2}+b^{2}+c^{2})^{2}}}\\[6mu]&={\tfrac {1}{4}}{\sqrt {4a^{2}b^{2}-(a^{2}+b^{2}-c^{2})^{2}}}.\end{aligned}}}$

After expansion, the expression under the square root is a quadratic polynomial of the squared side lengths ${\displaystyle a^{2}}$, ${\displaystyle b^{2}}$, ${\displaystyle c^{2}}$.

The same relation can be expressed using the Cayley–Menger determinant,^[2]

${\displaystyle -16A^{2}={\begin{vmatrix}0&a^{2}&b^{2}&1\\a^{2}&0&c^{2}&1\\b^{2}&c^{2}&0&1\\1&1&1&0\end{vmatrix}}.}$

History

The formula is credited to Heron (or Hero) of Alexandria (fl. 60 AD),^[3] and a proof can be found in his book Metrica. Mathematical historian Thomas Heath suggested that Archimedes knew the formula over two centuries earlier,^[4] and since Metrica is a collection of the mathematical knowledge available in the ancient world, it is possible that the formula predates the reference given in that work.^[5]

A formula equivalent to Heron's, namely,

${\displaystyle A={\frac {1}{2}}{\sqrt {a^{2}c^{2}-\left({\frac {a^{2}+c^{2}-b^{2}}{2}}\right)^{2}}}}$

was discovered by the Chinese. It was published in Mathematical Treatise in Nine Sections (Qin Jiushao, 1247).^[6]

Proofs

There are many ways to prove Heron's formula, for example using trigonometry as below, or the incenter and one excircle of the triangle,^[7] or as a special case of De Gua's theorem (for the particular case of acute triangles),^[8] or as a special case of Brahmagupta's formula (for the case of a degenerate cyclic quadrilateral).

Trigonometric proof using the law of cosines

A modern proof, which uses algebra and is quite different from the one provided by Heron, follows.^[9] Let ${\displaystyle a,}$ ${\displaystyle b,}$ ${\displaystyle c}$ be the sides of the triangle and ${\displaystyle \alpha ,}$ ${\displaystyle \beta ,}$ ${\displaystyle \gamma }$ the angles opposite those sides. Applying the law of cosines we get

${\displaystyle \cos \gamma ={\frac {a^{2}+b^{2}-c^{2}}{2ab}}}$

From this proof, we get the algebraic statement that

${\displaystyle \sin \gamma ={\sqrt {1-\cos ^{2}\gamma }}={\frac {\sqrt {4a^{2}b^{2}-(a^{2}+b^{2}-c^{2})^{2}}}{2ab}}.}$

The altitude of the triangle on base ${\displaystyle a}$ has length ${\displaystyle b\sin \gamma }$, and it follows

${\displaystyle {\begin{aligned}A&={\tfrac {1}{2}}({\mbox{base}})({\mbox{altitude}})\\[6mu]&={\tfrac {1}{2}}ab\sin \gamma \\[6mu]&={\frac {ab}{4ab}}{\sqrt {4a^{2}b^{2}-(a^{2}+b^{2}-c^{2})^{2}}}\\[6mu]&={\tfrac {1}{4}}{\sqrt {-a^{4}-b^{4}-c^{4}+2a^{2}b^{2}+2a^{2}c^{2}+2b^{2}c^{2}}}\\[6mu]&={\tfrac {1}{4}}{\sqrt {(a+b+c)(-a+b+c)(a-b+c)(a+b-c)}}\\[6mu]&={\sqrt {\left({\frac {a+b+c}{2}}\right)\left({\frac {-a+b+c}{2}}\right)\left({\frac {a-b+c}{2}}\right)\left({\frac {a+b-c}{2}}\right)}}\\[6mu]&={\sqrt {s(s-a)(s-b)(s-c)}}.\end{aligned}}}$

Algebraic proof using the Pythagorean theorem

The following proof is very similar to one given by Raifaizen.^[10] By the Pythagorean theorem we have ${\displaystyle b^{2}=h^{2}+d^{2}}$ and ${\displaystyle a^{2}=h^{2}+(c-d)^{2}}$ according to the figure at the right. Subtracting these yields ${\displaystyle a^{2}-b^{2}=c^{2}-2cd.}$ This equation allows us to express ${\displaystyle d}$ in terms of the sides of the triangle:

${\displaystyle d={\frac {-a^{2}+b^{2}+c^{2}}{2c}}.}$

For the height of the triangle we have that ${\displaystyle h^{2}=b^{2}-d^{2}.}$ By replacing ${\displaystyle d}$ with the formula given above and applying the difference of squares identity we get

${\displaystyle {\begin{aligned}h^{2}&=b^{2}-\left({\frac {-a^{2}+b^{2}+c^{2}}{2c}}\right)^{2}\\&={\frac {(2bc-a^{2}+b^{2}+c^{2})(2bc+a^{2}-b^{2}-c^{2})}{4c^{2}}}\\&={\frac {{\big (}(b+c)^{2}-a^{2}{\big )}{\big (}a^{2}-(b-c)^{2}{\big )}}{4c^{2}}}\\&={\frac {(b+c-a)(b+c+a)(a+b-c)(a-b+c)}{4c^{2}}}\\&={\frac {2(s-a)\cdot 2s\cdot 2(s-c)\cdot 2(s-b)}{4c^{2}}}\\&={\frac {4s(s-a)(s-b)(s-c)}{c^{2}}}.\end{aligned}}}$

We now apply this result to the formula that calculates the area of a triangle from its height:

${\displaystyle {\begin{aligned}A&={\frac {ch}{2}}\\&={\sqrt {{\frac {c^{2}}{4}}\cdot {\frac {4s(s-a)(s-b)(s-c)}{c^{2}}}}}\\&={\sqrt {s(s-a)(s-b)(s-c)}}.\end{aligned}}}$

Trigonometric proof using the law of cotangents

If ${\displaystyle r}$ is the radius of the incircle of the triangle, then the triangle can be broken into three triangles of equal altitude ${\displaystyle r}$ and bases ${\displaystyle a,}$ ${\displaystyle b,}$ and ${\displaystyle c.}$ Their combined area is

${\displaystyle A={\tfrac {1}{2}}ar+{\tfrac {1}{2}}br+{\tfrac {1}{2}}cr=rs,}$

where ${\displaystyle s={\tfrac {1}{2}}(a+b+c)}$ is the semiperimeter.

The triangle can alternately be broken into six triangles (in congruent pairs) of altitude ${\displaystyle r}$ and bases ${\displaystyle s-a,}$ ${\displaystyle s-b,}$ and ${\displaystyle s-c}$ of combined area (see law of cotangents)

${\displaystyle {\begin{aligned}A&=r(s-a)+r(s-b)+r(s-c)\\[2mu]&=r^{2}\left({\frac {s-a}{r}}+{\frac {s-b}{r}}+{\frac {s-c}{r}}\right)\\[2mu]&=r^{2}\left(\cot {\frac {\alpha }{2}}+\cot {\frac {\beta }{2}}+\cot {\frac {\gamma }{2}}\right)\\[3mu]&=r^{2}\left(\cot {\frac {\alpha }{2}}\cot {\frac {\beta }{2}}\cot {\frac {\gamma }{2}}\right)\\[3mu]&=r^{2}\left({\frac {s-a}{r}}\cdot {\frac {s-b}{r}}\cdot {\frac {s-c}{r}}\right)\\[3mu]&={\frac {(s-a)(s-b)(s-c)}{r}}.\end{aligned}}}$

The middle step above is ${\textstyle \cot {\tfrac {\alpha }{2}}+\cot {\tfrac {\beta }{2}}+\cot {\tfrac {\gamma }{2}}={}}$${\displaystyle \cot {\tfrac {\alpha }{2}}\cot {\tfrac {\beta }{2}}\cot {\tfrac {\gamma }{2}},}$ the triple cotangent identity, which applies because the sum of half-angles is ${\textstyle {\tfrac {\alpha }{2}}+{\tfrac {\beta }{2}}+{\tfrac {\gamma }{2}}={\tfrac {\pi }{2}}.}$

Combining the two, we get

${\displaystyle A^{2}=s(s-a)(s-b)(s-c),}$

from which the result follows.

Numerical stability

Heron's formula as given above is numerically unstable for triangles with a very small angle when using floating-point arithmetic. A stable alternative involves arranging the lengths of the sides so that ${\displaystyle a\geq b\geq c}$ and computing^[11][12]

${\displaystyle A={\tfrac {1}{4}}{\sqrt {{\big (}a+(b+c){\big )}{\big (}c-(a-b){\big )}{\big (}c+(a-b){\big )}{\big (}a+(b-c){\big )}}}.}$

The brackets in the above formula are required in order to prevent numerical instability in the evaluation.

Similar triangle-area formulae

Three other formulae for the area of a general triangle have a similar structure as Heron's formula, expressed in terms of different variables.

First, if ${\displaystyle m_{a},}$ ${\displaystyle m_{b},}$ and ${\displaystyle m_{c}}$ are the medians from sides ${\displaystyle a,}$ ${\displaystyle b,}$ and ${\displaystyle c}$ respectively, and their semi-sum is ${\displaystyle \sigma ={\tfrac {1}{2}}(m_{a}+m_{b}+m_{c}),}$ then^[13]

${\displaystyle A={\frac {4}{3}}{\sqrt {\sigma (\sigma -m_{a})(\sigma -m_{b})(\sigma -m_{c})}}.}$

Next, if ${\displaystyle h_{a}}$, ${\displaystyle h_{b}}$, and ${\displaystyle h_{c}}$ are the altitudes from sides ${\displaystyle a,}$ ${\displaystyle b,}$ and ${\displaystyle c}$ respectively, and semi-sum of their reciprocals is ${\displaystyle H={\tfrac {1}{2}}{\bigl (}h_{a}^{-1}+h_{b}^{-1}+h_{c}^{-1}{\bigr )},}$ then^[14]

${\displaystyle A^{-1}=4{\sqrt {H{\bigl (}H-h_{a}^{-1}{\bigr )}{\bigl (}H-h_{b}^{-1}{\bigr )}{\bigl (}H-h_{c}^{-1}{\bigr )}}}.}$

Finally, if ${\displaystyle \alpha ,}$ ${\displaystyle \beta ,}$ and ${\displaystyle \gamma }$ are the three angle measures of the triangle, and the semi-sum of their sines is ${\displaystyle S={\tfrac {1}{2}}(\sin \alpha +\sin \beta +\sin \gamma ),}$ then^[15][16]

${\displaystyle {\begin{aligned}A&=D^{2}{\sqrt {S(S-\sin \alpha )(S-\sin \beta )(S-\sin \gamma )}}\\[5mu]&={\tfrac {1}{2}}D^{2}\sin \alpha \,\sin \beta \,\sin \gamma ,\end{aligned}}}$

where ${\displaystyle D}$ is the diameter of the circumcircle, ${\displaystyle D=a/{\sin \alpha }=b/{\sin \beta }=c/{\sin \gamma }.}$ This last formula coincides with the standard Heron formula when the circumcircle has unit diameter.

Generalizations

Heron's formula is a special case of Brahmagupta's formula for the area of a cyclic quadrilateral. Heron's formula and Brahmagupta's formula are both special cases of Bretschneider's formula for the area of a quadrilateral. Heron's formula can be obtained from Brahmagupta's formula or Bretschneider's formula by setting one of the sides of the quadrilateral to zero.

Brahmagupta's formula gives the area ${\displaystyle K}$ of a cyclic quadrilateral whose sides have lengths ${\displaystyle a,}$ ${\displaystyle b,}$ ${\displaystyle c,}$ ${\displaystyle d}$ as

${\displaystyle K={\sqrt {(s-a)(s-b)(s-c)(s-d)}}}$

where ${\displaystyle s={\tfrac {1}{2}}(a+b+c+d)}$ is the semiperimeter.

Heron's formula is also a special case of the formula for the area of a trapezoid or trapezium based only on its sides. Heron's formula is obtained by setting the smaller parallel side to zero.

Expressing Heron's formula with a Cayley–Menger determinant in terms of the squares of the distances between the three given vertices,

${\displaystyle A={\frac {1}{4}}{\sqrt {-{\begin{vmatrix}0&a^{2}&b^{2}&1\\a^{2}&0&c^{2}&1\\b^{2}&c^{2}&0&1\\1&1&1&0\end{vmatrix}}}}}$

illustrates its similarity to Tartaglia's formula for the volume of a three-simplex.

Another generalization of Heron's formula to pentagons and hexagons inscribed in a circle was discovered by David P. Robbins.^[17]

Heron-type formula for the volume of a tetrahedron

If ${\displaystyle U,}$ ${\displaystyle V,}$ ${\displaystyle W,}$ ${\displaystyle u,}$ ${\displaystyle v,}$ ${\displaystyle w}$ are lengths of edges of the tetrahedron (first three form a triangle; ${\displaystyle u}$ opposite to ${\displaystyle U}$ and so on), then^[18]

${\displaystyle {\text{volume}}={\frac {\sqrt {\,(-a+b+c+d)\,(a-b+c+d)\,(a+b-c+d)\,(a+b+c-d)}}{192\,u\,v\,w}}}$

where

${\displaystyle {\begin{aligned}a&={\sqrt {xYZ}}\\b&={\sqrt {yZX}}\\c&={\sqrt {zXY}}\\d&={\sqrt {xyz}}\\X&=(w-U+v)\,(U+v+w)\\x&=(U-v+w)\,(v-w+U)\\Y&=(u-V+w)\,(V+w+u)\\y&=(V-w+u)\,(w-u+V)\\Z&=(v-W+u)\,(W+u+v)\\z&=(W-u+v)\,(u-v+W).\end{aligned}}}$

Heron formulae in non-Euclidean geometries

There are also formulae for the area of a triangle in terms of its side lengths for triangles in the sphere or the hyperbolic plane. ^[19] For a triangle in the sphere with side lengths ${\displaystyle a,}$ ${\displaystyle b,}$ and ${\displaystyle c}$ the semiperimeter ${\displaystyle s={\tfrac {1}{2}}(a+b+c)}$ and area ${\displaystyle S}$, such a formula is

${\displaystyle \tan ^{2}{\frac {S}{4}}=\tan {\frac {s}{2}}\tan {\frac {s-a}{2}}\tan {\frac {s-b}{2}}\tan {\frac {s-c}{2}}}$

while for the hyperbolic plane we have

${\displaystyle \tan ^{2}{\frac {S}{4}}=\tanh {\frac {s}{2}}\tanh {\frac {s-a}{2}}\tanh {\frac {s-b}{2}}\tanh {\frac {s-c}{2}}.}$

See also

• Shoelace formula

References

External links

• A Proof of the Pythagorean Theorem From Heron's Formula at cut-the-knot
• Interactive applet and area calculator using Heron's Formula
• J. H. Conway discussion on Heron's Formula
• "Heron's Formula and Brahmagupta's Generalization". MathPages.com.
• A Geometric Proof of Heron's Formula
• An alternative proof of Heron's Formula without words
• Factoring Heron

This page was last edited on 20 May 2024, at 00:45