1. Reference problem#
1.1. Geometry#
Beam \(\mathit{PA}\):
Section: \(0.1\mathrm{mm}\times 0.1\mathrm{mm}\)
Length: \(3.0m\)
Beam \(\mathit{PB}\):
Section: \(0.001\mathrm{mm}\times 0.001\mathrm{mm}\)
Length: \(2.0m\)
Mass ratio between \(\mathrm{PB}\) and \(\mathrm{PA}\): \(0.33E–04\)
1.2. Material properties#
Young’s module beams \(A\) and \(B\): |
\(E=2.1E+11N/{m}^{2}\) |
Poisson ratio beams \(A\) and \(B\): |
\(\nu =0.3\) |
Density beam \(\mathrm{PA}\): |
\({\rho }_{A}=2000\mathrm{kg}/{m}^{3}\) |
Density beam \(\mathit{PB}\): |
\({\rho }_{B}=1000\mathrm{kg}/{m}^{3}\) |
1.3. Boundary conditions and loads#
The movement is authorized in plan \((\mathrm{DX},\mathrm{DY})\).
Beam \(\mathrm{PA}\) is embedded in the support.
Beam \(\mathrm{PB}\) is connected to Beam \(\mathrm{PA}\) by three points. In each, the movements in the \(\mathrm{DX}\) and \(\mathrm{DY}\) directions of the \(\mathrm{PA}\) node and the \(\mathrm{PB}\) node are identical. The rotations are not linked.
The interspectral matrix that transmits the movements from structure \(\mathrm{PA}\) to structure \(\mathrm{PB}\) in the chained calculation is of dimension 6 (6 degrees of freedom of transmission).