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A comparison of three different design methods is presented based on 15,064 composite beam cases.
For uniform beam cases, the Laplace transform is used to formulate the characteristic equations for a beam carrying intermediate concentrated masses.
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For the fixed beam case, the corresponding values are 0.54 bit/s/Hz and 1.6 bit/s/Hz.
Unlike Euler Bernoulli beam, such incoherence in the Timoshenko beam case has not been theoretically proved so far.
Additionally the effects of the liquid depth on the natural frequency is investigated and compared with the solid beam case.
However, it is obvious that the lower degree of correlation between the MIMO channels in the fixed beam case is not the only factor for better BER performance.
The BER performance corresponds well to the above findings that the MIMO channel correlation is lower in the fixed beam case.
The simulation model is exactly the same for the reference antenna domain case and the Butler beam case except that these two schemes apply different BS antenna/beam patterns of Figure 3.
In the single electron beam case there is only the electromagnetic mode but as seen the results there is the new electrostatic mode that is two times stronger than electromagnetic mode.
To demonstrate the utility and simplification procedures, the generic linear/nonlinear shell energy harvester mechanism is simplified to three specific structures, i.e., a cantilever beam case, a circular ring case and a conical shell case.
Unlike the thin beam, which corresponds to the geometry that has been experimentally tested in [5], the thick beam case is a pure numerical exercise aiming to reproduce a stiff structure for which the size of the cohesive zone is comparable to the dimensions of the sample, see also [18].
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com