2020
DOI: 10.3103/s0025654420050052
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On Solvability of Boundary Value Problems for Elastic Micropolar Shells with Rigid Inclusions

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Cited by 4 publications
(5 citation statements)
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“…Let us note that here equation (39) includes a part of the initial conditions for the velocities, whereas the initial data for translations and rotations are treated as the ones which should be formulated explicitly. Now for shortness, we introduce the notation as in Eremeev and Lebedev [34]: U = ((u, f), u 1 , . .…”
Section: The Principle Of Virtual Work and Weak Solutionsmentioning
confidence: 99%
See 4 more Smart Citations
“…Let us note that here equation (39) includes a part of the initial conditions for the velocities, whereas the initial data for translations and rotations are treated as the ones which should be formulated explicitly. Now for shortness, we introduce the notation as in Eremeev and Lebedev [34]: U = ((u, f), u 1 , . .…”
Section: The Principle Of Virtual Work and Weak Solutionsmentioning
confidence: 99%
“…Now for shortness, we introduce the notation as in Eremeev and Lebedev [34]: U = ( ( u , ϕ ) , u 1 , , u n , ϑ 1 , , ϑ N ) and, respectively, δ U = ( ( δ u , δ ϕ ) , δ u 1 , , δ u n , δ ϑ 1 , , δ ϑ N ) . On the set of U where ( u , f ) are smooth functions satisfying boundary conditions (9) 3 and (9) 4 , we introduce an inner product defined by the energy terms for ( u , ϕ ) :…”
Section: The Principle Of Virtual Work and Weak Solutionsmentioning
confidence: 99%
See 3 more Smart Citations