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PinnedBeam_abg.tex

MTT command:
mtt PinnedBeam abg tex

Figure 2.1: System PinnedBeam: acausal bond graph
\fbox{
\includegraphics[width=0.9\linewidth,height=18cm,keepaspectratio]{/home/...
...xamples/Mechanical/Mechanical-1D/Beams/PinnedBeam/MTT_work/PinnedBeam_abg.ps}
}

The acausal bond graph of system PinnedBeam is displayed in Figure 2.1 (on page [*]) and its label file is listed in Section 2.1.1 (on page [*]). The subsystems are listed in Section 2.1.2 (on page [*]).

This example represents the dynamics of a uniform beam with two pinned ends. The left-hand end is driven by a torque input and the corresponding collocated angular velocity is measured. The beam is approximated by 20 equal lumps using the Bernoulli-Euler. Because the two end lumps have different causality to the rest of the beam lumps, they are represented seperately. The system has 40 states (20 modes of vibration), 1 input and 1 output.


Table 2.1: Beam parameters
Name Value
Beam Length, $ L$ 0.60 m
Beam Width $ w$ 0.05 m
Beam Thickness $ t_b$ 0.003
Young's Modulus $ E$ $ 68.94 \times 10^9$
Density $ \rho$ 2712.8
Derived quantities  
$ EI$ 7.76
$ \rho A$ 0.40692


The beam was made of aluminium with physical dimensions and constants given in Table 2.1. The derived beam constants are given by the formulae:

\begin{displaymath}\begin{align}EI &= E \times w \frac{1}{12} t_b^3\\  \rho A &= \rho \times w t_b \end{align}\end{displaymath}

The system parameters are also given in Section [*] (on page [*]).


Table 2.2: Resonant and anti-resonant frequencies (Hz)
Index $ f_r$ (theory) $ f_r$ (model) $ f_a$ (theory) $ f_a$ (model)
1 19.05 19.01 29.72 31.28
2 76.24 75.57 96.50 100.80
3 171.58 168.29 200.73 208.20
4 304.76 294.89 344.13 350.88
5 476.34 452.25 524.98 525.23


Standard modal analysis give the theoretical system resonant frequencies $ f_r$ (based on the Bernoulli-Euler beam with the same values of $ EI$ and $ \rho A$). The system anti-resonances $ f_a$ correspond to those of the inverse system with reversed causality, that the driven pinned end is replaced by a clamped end; again modal analysis of the inverse system gives the system anti resonances. The model and theoretical values are compared in Table 2.2 for the first 5 modes. (This table was generated using the script MakeFreqTable.m)



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