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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> | ||
Zeile 89: | Zeile 89: | ||
<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> | ||
Zeile 94: | Zeile 100: | ||
<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 # | <tr><th>Element #4</th></tr> | ||
<tr><td> | <tr><td> | ||
{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}{{\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 |
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Element #1 |
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Element #2 |
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Element #3 |
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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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