QMU Analysis of Flexoelectric Timoshenko Beam by Evidence Theory

<div>Probability distribution of flexoelectric Timoshenko beam’s forced vibration at rotational angle <span class="nowrap"><svg height="8.68572pt" id="M131" style="vertical-align:-0.0498209pt" version="1.1" viewbox="-0.0498162 -8.6359 9.93839 8.68572" width="9.93839pt" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink"><g transform="matrix(.013,0,0,-0.013,0,0)"><path d="M488 658H270V630C328 626 335 619 335 579C217 574 44 509 44 330C44 147 221 88 335 86C335 38 328 32 265 28V0H488V28C425 32 418 38 418 86C534 88 710 153 710 337C710 517 538 575 418 579C418 619 425 626 488 630V658ZM335 118C249 124 136 180 136 337C136 490 251 543 335 547V118ZM418 547C502 543 618 491 618 333S503 124 418 118V547Z"></path></g></svg>.</span></div>

Advances in Mathematical Physics

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Figure 6

Figure 6: QMU Analysis of Flexoelectric Timoshenko Beam by Evidence Theory 