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<record version="2" id="3031">
 <title>alternate proof of parallelogram law</title>
 <name>AlternateProofOfParallelogramLaw</name>
 <created>2002-06-04 11:42:13</created>
 <modified>2002-06-04 13:42:20</modified>
 <type>Proof</type>
<parent id="1082">parallelogram law</parent>
 <selfproof></selfproof>
 <creator id="3" name="drini"/>
 <author id="58" name="fiziko"/>
 <classification>
	<category scheme="msc" code="51-00"/>
 </classification>
 <related>
	<object name="ProofOfParallelogramLaw2"/>
 </related>
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 <content>Proof of this is simple, given the cosine law:
\[
c^2 = a^2 + b^2 - 2ab\cos\phi
\]
where $a$, $b$, and $c$ are the lengths of the sides of the triangle, and angle $\phi$ is the corner angle opposite the side of length $c$.


Let us define the largest interior angles as angle $\theta$.
Applying this to the parallelogram, we find that
\begin{eqnarray*}
d_1^2 &amp;=&amp; u^2 + v^2 - 2uv\cos\theta\\
d_2^2 &amp;=&amp; u^2+v^2 - 2uv\cos\left(\pi-\theta\right)
\end{eqnarray*}
 


Knowing that
\[
\cos\left(\pi-\theta\right) = - \cos\theta
\]
we can add the two expressions together, and find ourselves with
\begin{eqnarray*}
d_1^2+d_2^2 &amp;=&amp; 2u^2 + 2v^2 - 2uv\cos\theta + 2uv\cos\theta\\
d_1^2+d_2^2 &amp;=&amp; 2u^2 + 2v^2
\end{eqnarray*}
which is the theorem we set out to prove.</content>
</record>
