Difference between revisions of "Template:Added mass damping and force matrices definition"
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Jump to navigationJump to search (Created page with 'We then define the matrices <center><math> A_{\mu\nu} = \mathrm{Re} \left\{ -\frac{\mathrm{i}}{\omega}\rho\iint_{\partial\Omega_{B}} \phi_{\nu}^{\mathrm{R}} n_{\mu}\, dS \right\…') |
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<center><math> | <center><math> | ||
A_{\mu\nu} = \mathrm{Re} \left\{ -\frac{\mathrm{i}}{\omega}\rho\iint_{\partial\Omega_{B}} | A_{\mu\nu} = \mathrm{Re} \left\{ -\frac{\mathrm{i}}{\omega}\rho\iint_{\partial\Omega_{B}} | ||
− | \phi_{\nu}^{\mathrm{R}} | + | \phi_{\nu}^{\mathrm{R}} \mathbf{n}_{\mu}\, dS \right\} |
</math></center> | </math></center> | ||
which is called the added mass matrix and | which is called the added mass matrix and | ||
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<center><math> | <center><math> | ||
B_{\mu\nu} = \mathrm{Im} \left\{ \rho\iint_{\partial\Omega_{B}} | B_{\mu\nu} = \mathrm{Im} \left\{ \rho\iint_{\partial\Omega_{B}} | ||
− | \phi_{\nu}^{\mathrm{R}} | + | \phi_{\nu}^{\mathrm{R}} \mathbf{n}_{\mu}\, dS \right\} |
</math></center> | </math></center> | ||
which is called the damping matrix and the forcing vector is | which is called the damping matrix and the forcing vector is | ||
<center><math> | <center><math> | ||
f_{\mu} = -\mathrm{i}\omega\rho\iint_{\partial\Omega_{B}} | f_{\mu} = -\mathrm{i}\omega\rho\iint_{\partial\Omega_{B}} | ||
− | \left(\phi^{\mathrm{I}} + \phi^{\mathrm{D}} \right) | + | \left(\phi^{\mathrm{I}} + \phi^{\mathrm{D}} \right) \mathbf{n}_{\mu}\, dS |
</math></center> | </math></center> |
Revision as of 22:26, 28 April 2010
We then define the matrices
which is called the added mass matrix and We then define the matrices
which is called the damping matrix and the forcing vector is