Difference between revisions of "Stewart's Theorem"
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== Statement == | == Statement == | ||
+ | Given a [[triangle]] <math>\triangle ABC</math> with sides of length <math>a, b, c</math> opposite [[vertex | vertices]] <math>A</math>, <math>B</math>, <math>C</math>, respectively. If [[cevian]] <math>AD</math> is drawn so that <math>BD = m</math>, <math>DC = n</math> and <math>AD = d</math>, we have that <math>b^2m + c^2n = amn + d^2a</math>. (This is also often written <math> cnc + bmb = man + dad</math>, a form which invites mnemonic memorization.) | ||
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<center>[[Image:Stewart's_theorem.png]]</center> | <center>[[Image:Stewart's_theorem.png]]</center> | ||
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== Proof == | == Proof == | ||
− | + | Applying the [[Law of Cosines]] in triangle <math>\triangle ABD</math> at [[angle]] <math>\angle ADB</math> and in triangle <math>\triangle ACD</math> at angle <math>\displaystyle \angle CDA</math>, we get the equations | |
+ | *<math> n^{2} + d^{2} - 2nd\cos{\angle ADB} = c^{2} </math> | ||
+ | *<math> m^{2} + d^{2} - 2md\cos{\angle CDA} = b^{2} </math> | ||
− | + | Because angles <math>\angle ADB</math> and <math>\displaystyle \angle CDA</math> are [[supplementary]], <math>m\angle ADB = 180^\circ - m\angle CDA</math>. We can therefore solve both equations for the cosine term. Using the [[trigonometric identity]] <math>\cos{\theta} = -\cos{(180^\circ - \theta)}</math> gives us | |
− | + | *<math> \frac{n^2 + d^2 - b^2}{2nd} = \cos{\angle CDA}</math> | |
− | + | *<math> \frac{c^2 - m^2 -d^2}{2md} = \cos{\angle CDA}</math> | |
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− | *<math> \frac{n^2 + d^2 - b^2}{ | ||
− | *<math> \frac{c^2 - m^2 -d^2}{ | ||
− | + | Setting the two left-hand sides equal and clearing [[denominator]]s, we arrive at the equation: <math> c^{2}n + b^{2}m=m^{2}n +n^{2}m + d^{2}m + d^{2}n </math>. | |
− | However, | + | However, <math>m+n = a</math> so <math>m^2n + n^2m = (m + n)mn</math> and we can rewrite this as <math>c^2n + b^2m = amn + d^2a</math>. |
== See also == | == See also == |
Revision as of 14:11, 5 November 2006
Statement
Given a triangle with sides of length opposite vertices , , , respectively. If cevian is drawn so that , and , we have that . (This is also often written , a form which invites mnemonic memorization.)
Proof
Applying the Law of Cosines in triangle at angle and in triangle at angle , we get the equations
Because angles and are supplementary, . We can therefore solve both equations for the cosine term. Using the trigonometric identity gives us
Setting the two left-hand sides equal and clearing denominators, we arrive at the equation: . However, so and we can rewrite this as .