2002
DOI: 10.1016/s0020-7683(01)00254-2
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Stochastic beam equations under random dynamic loads

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Cited by 10 publications
(9 citation statements)
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“…Here G1(x,t)=4βe0.1tsinπx ${G}_{1}(x,t)=4\beta {e}^{-0.1t}\sin \pi x$ and G2(x,t)=4σe0.1tsinπx ${G}_{2}(x,t)=4\sigma {e}^{-0.1t}\sin \pi x$. Here the expressions for the notations involved in the above equation can be found in 25 . We use the values of the notations involved in the above PDE as available in 25 .…”
Section: Numerical Examplesmentioning
confidence: 99%
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“…Here G1(x,t)=4βe0.1tsinπx ${G}_{1}(x,t)=4\beta {e}^{-0.1t}\sin \pi x$ and G2(x,t)=4σe0.1tsinπx ${G}_{2}(x,t)=4\sigma {e}^{-0.1t}\sin \pi x$. Here the expressions for the notations involved in the above equation can be found in 25 . We use the values of the notations involved in the above PDE as available in 25 .…”
Section: Numerical Examplesmentioning
confidence: 99%
“…c=CρA $c=\frac{C}{\rho A}$, G(x,t;ω)=F(x,t;ω)ρA $G(x,t;\omega )=\frac{F(x,t;\omega )}{\rho A}$, α2=EIρA ${\alpha }^{2}=\frac{EI}{\rho A}$, S=NˆρA $S=\frac{\hat{N}}{\rho A}$, the above equation takes the form α24u(x,t)x4+2u(x,t)t2+cu(x,t)tS2u(x,t)x2=G1(x,t)+G2(x,t)trueB˙(t). ${\alpha }^{2}\frac{{\partial }^{4}u(x,t)}{\partial {x}^{4}}+\frac{{\partial }^{2}u(x,t)}{\partial {t}^{2}}+c\frac{\partial u(x,t)}{\partial t}-S\frac{{\partial }^{2}u(x,t)}{\partial {x}^{2}}={G}_{1}(x,t)+{G}_{2}(x,t)\dot{B}(t).$ One can refer to Galal et al 25 for the expansions of the notations involved in the above equation. Applying the following boundary and initial conditions for the simply supported beam of length l $l$, u(0,t)=0, $u(0,t)=0,$ 2u…”
Section: Introductionmentioning
confidence: 99%
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“…2. Stochastic elastic equation driven by Brownian motion has been studied by many authors, see [5,7,13,25,38]. However, there were few papers consider stochastic elastic equation driven by fractional Brownian motion.…”
Section: Y Zhang and X Yangmentioning
confidence: 99%
“…In the category of perturbation method, new tries had been made to overcome the drawbacks in that method (Elishakoff et al, 1997;Falsone and Impollonia, 2002;Kaminski, 2001). Some research works are dedicated to determine the bounds in response variability (Deodatis and Shinozuka, 1989;Deodatis et al, 2003;Papadopoulos et al, 2005) and to the dynamic and non-linear problems (Adhikari and Manohar, 1999;Anders and Hori, 1999;Galal et al, 2002;Liu et al, 1986;Li et al, 1999). In addition to the material parameters, some researchers put their focus on the evaluation of response variability due to randomness in geometrical parameters such as the thickness of plate structures and section of beams (Altus and Totry, 2003;Noh, 1996, 2000;Lawrence, 1987), due to temporal uncertainties in applied loads (Chiostrini and Facchini, 1999;Galal et al, 2002;To, 1986) and due to random temperature (Liu et al, 2001) in concrete structures.…”
Section: Introductionmentioning
confidence: 99%