Overview
Comment: | Initial revision |
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Downloads: | Tarball | ZIP archive | SQL archive |
Timelines: | family | ancestors | descendants | both | origin/master | trunk |
Files: | files | file ages | folders |
SHA3-256: |
5bb47c87590d328bc5518e0b9a27df64 |
User & Date: | gawthrop@users.sourceforge.net on 1997-07-06 16:35:20 |
Other Links: | branch diff | manifest | tags |
Context
1997-07-27
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13:11:11 | Added path checking code -- mtt_check_vars check-in: fb8c567bf5 user: gawthrop@users.sourceforge.net tags: origin/master, trunk | |
1997-07-06
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16:35:20 | Initial revision check-in: 5bb47c8759 user: gawthrop@users.sourceforge.net tags: origin/master, trunk | |
16:20:44 | Initial revision check-in: f65ef2502d user: gawthrop@users.sourceforge.net tags: origin/master, trunk | |
Changes
Added mttroot/mtt/lib/examples/Hybrid/BouncingRod/BouncingRod_desc.tex version [850ed35ecc].
> > > > > > > > > > > > > > > > > > > > > > > > > > > > > > > > > | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 | % Verbal description for system BouncingRod (BouncingRod_desc.tex) % Generated by MTT on Sun Jul 6 17:21:23 BST 1997. % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % %% Version control history % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% % %% $Id$ % %% $Log$ % %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% The acausal bond graph of system \textbf{BouncingRod} is displayed in Figure \Ref{BouncingRod_abg} and its label file is listed in Section \Ref{sec:BouncingRod_lbl}. The subsystems are listed in Section \Ref{sec:BouncingRod_sub}. The system consists of a uniform rod of mass 1kg, length 2m (and therefore of inertia about the mass centre of $frac{1}{3} \text{kgm}^2$. The rod is released at an angle of $\frac{\pi}{4}$ from the vertical, the mass centre is $10\text{m}$ above the ground and all velocities are initially zero. The gravitational constant is taken as unity. The ground is modeled as an ideal compliance in the vertical direction with compliance of $0.1 \text{mN}^{-1}$ and it is assumed that contact takes place at the rod tips only. There is no horizontal resistance to motion. This idealised setup is modeled by a two {\bf CSW} components, one for each rod tip, modulated by the height of each rod tip above the ground: each {\bf CSW} is off when the corresponding height is positive. |