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\end{pmatrix}
\end{pmatrix}
</math>
</math>
Hier kommt jetzt irgendein Text.


<math>
::<math>
</math
Some Text
 
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}}
}}


<table class="wikitable mw-collapsible" style="background-color:white; float: none; margin-right:14px;">
<table class="wikitable mw-collapsible mw-collapsed" style="background-color:white; float: none; margin-right:14px;">
<tr><th>Element-Steigigkeitsmatrizen mit globalen Koordinaten</th></tr>
<tr><th>Element #1</th></tr>
<tr><th>Element #1</th></tr>
<tr><td>
<tr><td>
<math>
<math>
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<tr><td>
<tr><td>
<math>
<math>
{k_2} = \begin{pmatrix}\frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & -\left( \frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\\
\frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\\
\frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & \frac{{{A}^{2}} E \eta }{3 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{{{A}^{2}} E \eta }{6 {\ell_0}}\\
-\left( \frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right) \\
-\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right) \\
\frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & \frac{{{A}^{2}} E \eta }{6 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{{{A}^{2}} E \eta }{3 {\ell_0}}\end{pmatrix}
</math>
</math>
</td></tr>
</td></tr>
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<tr><td>
<tr><td>
<math>
<math>
{k_3} = \begin{pmatrix}\frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & -\left( \frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\\
-\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right) \\
\frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{{{A}^{2}} E \eta }{3 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & \frac{{{A}^{2}} E \eta }{6 {\ell_0}}\\
-\left( \frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{{{A}^{2}} E \eta +3 {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right) \\
\frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & -\left( \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta -\sqrt{3} {\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}}\right)  & \frac{3 {{A}^{2}} E \eta +{\ell_{0}^{2}} A E}{4 {\ell_{0}^{3}}} & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\\
\frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & -\left( \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{{{A}^{2}} E \eta }{6 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{4 {\ell_{0}^{2}}}\right)  & \frac{\sqrt{3} {{A}^{2}} E \eta }{4 {\ell_{0}^{2}}} & \frac{{{A}^{2}} E \eta }{3 {\ell_0}}\end{pmatrix}
</math>
</math>
</td></tr>
</td></tr>
<tr><th>Element #1</th></tr>
<tr><th>Element #4</th></tr>
<tr><td>
<tr><td>
<math>
{k_4} = \begin{pmatrix}\frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}} & 0 & \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}} & -\left( \frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}}\right)  & 0 & \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\\
</math>
0 & \frac{A E}{{\ell_0}} & 0 & 0 & -\left( \frac{A E}{{\ell_0}}\right)  & 0\\
\frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}} & 0 & \frac{{{A}^{2}} E \eta }{3 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right)  & 0 & \frac{{{A}^{2}} E \eta }{6 {\ell_0}}\\
-\left( \frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}}\right)  & 0 & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right)  & \frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}} & 0 & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right) \\
0 & -\left( \frac{A E}{{\ell_0}}\right)  & 0 & 0 & \frac{A E}{{\ell_0}} & 0\\
\frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}} & 0 & \frac{{{A}^{2}} E \eta }{6 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right)  & 0 & \frac{{{A}^{2}} E \eta }{3 {\ell_0}}\end{pmatrix}
</td></tr>
</td></tr>
</table>
</table>

Version vom 21. Oktober 2024, 15:01 Uhr


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Element-Steigigkeitsmatrizen mit globalen Koordinaten
Element #1

Element #2

Element #3

Element #4

{k_4} = \begin{pmatrix}\frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}} & 0 & \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}} & -\left( \frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}}\right) & 0 & \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\\ 0 & \frac{A E}Vorlage:\ell 0 & 0 & 0 & -\left( \frac{A E}Vorlage:\ell 0\right) & 0\\ \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}} & 0 & \frac{{{A}^{2}} E \eta }{3 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right) & 0 & \frac{{{A}^{2}} E \eta }{6 {\ell_0}}\\ -\left( \frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}}\right) & 0 & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right) & \frac{{{A}^{2}} E \eta }{{\ell_{0}^{3}}} & 0 & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right) \\ 0 & -\left( \frac{A E}Vorlage:\ell 0\right) & 0 & 0 & \frac{A E}Vorlage:\ell 0 & 0\\ \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}} & 0 & \frac{{{A}^{2}} E \eta }{6 {\ell_0}} & -\left( \frac{{{A}^{2}} E \eta }{2 {\ell_{0}^{2}}}\right) & 0 & \frac{{{A}^{2}} E \eta }{3 {\ell_0}}\end{pmatrix}


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