2. Benchmark solution#

2.1. Calculation method#

The reference solution adopted is that obtained by solving the vibrating string equation:

_images/1000000000000207000001DBAF1FE05E64E73BB7.png

The equation for vibrating strings is:

\(\frac{{\partial }^{2}y}{\partial {t}^{2}}=\frac{{F}_{0}}{\rho S}\frac{{\partial }^{2}y}{\partial {x}^{2}}\)

with:

\({F}_{0}\): tension in the rope,

\(\rho\): density,

\(S\): rope section.

For a string of length \(L\), fixed at these 2 ends, the nth natural vibration frequency is:

\(f=\frac{n}{2L}\sqrt{\frac{{F}_{0}}{\rho S}}\)

2.2. Reference quantities and results#

The quantities tested are the natural vibration frequencies of the cables for 2 calculation moments, which correspond to 2 different voltages.

Not

Cable Voltage

Frequency

10

\(6171.050459855N\)

\(62.73227096292042\mathit{Hz}\)

20

\(12345.2954376N\)

\(88.72830898253936\mathit{Hz}\)

2.3. Uncertainties about the solution#

The solution of the vibrating string equation is obtained under the following hypotheses:

  • The movements of the rope around its equilibrium position remain small.

  • the variations in angle \(\alpha\) remain small.

  • the variation in the tension of the moving rope remains small.

Under these assumptions, the reference solution is free of uncertainty.