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Apollonius's theorem

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(Redirected from Apollonius' theorem) Relates the length of a median of a triangle to the lengths of its sides This article is about the lengths of the sides of a triangle. For his work on circles, see Problem of Apollonius.
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Pythagoras as a special case:
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In geometry, Apollonius's theorem is a theorem relating the length of a median of a triangle to the lengths of its sides. It states that the sum of the squares of any two sides of any triangle equals twice the square on half the third side, together with twice the square on the median bisecting the third side. The theorem is named for the ancient Greek mathematician Apollonius of Perga.

Statement and relation to other theorem

In any triangle A B C , {\displaystyle ABC,} if A D {\displaystyle AD} is a median, then | A B | 2 + | A C | 2 = 2 ( | B D | 2 + | A D | 2 ) . {\displaystyle |AB|^{2}+|AC|^{2}=2(|BD|^{2}+|AD|^{2}).} It is a special case of Stewart's theorem. For an isosceles triangle with | A B | = | A C | , {\displaystyle |AB|=|AC|,} the median A D {\displaystyle AD} is perpendicular to B C {\displaystyle BC} and the theorem reduces to the Pythagorean theorem for triangle A D B {\displaystyle ADB} (or triangle A D C {\displaystyle ADC} ). From the fact that the diagonals of a parallelogram bisect each other, the theorem is equivalent to the parallelogram law.

Proof

Proof of Apollonius's theorem

The theorem can be proved as a special case of Stewart's theorem, or can be proved using vectors (see parallelogram law). The following is an independent proof using the law of cosines.

Let the triangle have sides a , b , c {\displaystyle a,b,c} with a median d {\displaystyle d} drawn to side a . {\displaystyle a.} Let m {\displaystyle m} be the length of the segments of a {\displaystyle a} formed by the median, so m {\displaystyle m} is half of a . {\displaystyle a.} Let the angles formed between a {\displaystyle a} and d {\displaystyle d} be θ {\displaystyle \theta } and θ , {\displaystyle \theta ^{\prime },} where θ {\displaystyle \theta } includes b {\displaystyle b} and θ {\displaystyle \theta ^{\prime }} includes c . {\displaystyle c.} Then θ {\displaystyle \theta ^{\prime }} is the supplement of θ {\displaystyle \theta } and cos θ = cos θ . {\displaystyle \cos \theta ^{\prime }=-\cos \theta .} The law of cosines for θ {\displaystyle \theta } and θ {\displaystyle \theta ^{\prime }} states that b 2 = m 2 + d 2 2 d m cos θ c 2 = m 2 + d 2 2 d m cos θ = m 2 + d 2 + 2 d m cos θ . {\displaystyle {\begin{aligned}b^{2}&=m^{2}+d^{2}-2dm\cos \theta \\c^{2}&=m^{2}+d^{2}-2dm\cos \theta '\\&=m^{2}+d^{2}+2dm\cos \theta .\,\end{aligned}}}

Add the first and third equations to obtain b 2 + c 2 = 2 ( m 2 + d 2 ) {\displaystyle b^{2}+c^{2}=2(m^{2}+d^{2})} as required.

See also

References

  1. Godfrey, Charles; Siddons, Arthur Warry (1908). Modern Geometry. University Press. p. 20.

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