2. Reference solution#
2.1. Calculation method used for the reference solution#
We are based on an analytical result [bib1]:
In the case of two concentric spheres immersed in the same fluid, it is shown that the added mass induced by the fluid confined to the internal sphere \(({S}_{1})\) is equal to:
\({m}_{a}=\frac{2}{3}{\rho }_{f}\pi \left[\frac{1+2{(\frac{{R}_{1}}{{R}_{2}})}^{3}}{1-{(\frac{{R}_{1}}{{R}_{2}})}^{3}}\right]{R}_{1}^{3}\)
If we assume that the sphere has only one degree of freedom following \(\mathrm{Oz}\), the natural mode of translation of the sphere \(({S}_{1})\) following \(\mathrm{Oz}\) is given by:
\(f=\frac{1}{2\pi }\sqrt{\frac{\mathrm{2K}}{m+{m}_{a}}}\)
Digital application:
\(K={10}^{5}N/m\) |
\(m=12\mathrm{kg}\) |
\({m}_{a}=329.17\mathrm{kg}\) |
\(F=3.8534\mathrm{Hz}\) |
2.2. Bibliographical references#
R.D. BLEVINS, « Formulas for Natural Frequency and Mode Shape, » Ed. KRIEGER