2004
DOI: 10.1080/03052150410001666569
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Influence of a shearing force on optimal design of shells against buckling under overall bending

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Cited by 4 publications
(9 citation statements)
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“…For pure bending case of loading (n 0 Z0, m b0 Z0, m b1 Z1) the optimal structure is a cylindrical shell (the first rows in Tables 2 and 4 -r(0)Zr(1)Z1) with the variable wall-thickness, whereas accounting for a shearing effect (n 0 Z0, m b0 Z1, m b1 Z0) leads to the optimal shell with double curvature (the first rows in Tables 1 and 3), where the geometrical constraint is active, r(1)Zr adm Z0.5. These results are in agreement with [3,5]. On the other hand, a limit case of a pure external pressure (n 0 /N) leads to an optimal shell, which is fully axial symmetric double curvature structure (wall thickness is also axially symmetric).…”
Section: Numerical Resultssupporting
confidence: 88%
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“…For pure bending case of loading (n 0 Z0, m b0 Z0, m b1 Z1) the optimal structure is a cylindrical shell (the first rows in Tables 2 and 4 -r(0)Zr(1)Z1) with the variable wall-thickness, whereas accounting for a shearing effect (n 0 Z0, m b0 Z1, m b1 Z0) leads to the optimal shell with double curvature (the first rows in Tables 1 and 3), where the geometrical constraint is active, r(1)Zr adm Z0.5. These results are in agreement with [3,5]. On the other hand, a limit case of a pure external pressure (n 0 /N) leads to an optimal shell, which is fully axial symmetric double curvature structure (wall thickness is also axially symmetric).…”
Section: Numerical Resultssupporting
confidence: 88%
“…It allows satisfying the conditions of continuity of the function up to the second derivative. This procedure was applied in [3][4][5] to optimization of shells under stability constraints. It turned out that more effective and even easier in application is introducing the Bézier polynomial (only one but of enough high order), which approximates a shape of the whole shell.…”
Section: Generating Of the Shapementioning
confidence: 99%
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“…16 Barski et al considered the stability of the shell with a double positive curvature and studied the optimal design of the shell shape and thickness against bucking subjected to the bending moment, the shearing force, the axial force, and torsional moment. [17][18][19][20] Nonetheless, there is a lack of an efficient optimal design model for the wall thickness. In this paper, an optimal design model for the wall thickness of the propellant tank is proposed to decrease the mass and optimize the stress distribution of the tank.…”
Section: Introductionmentioning
confidence: 99%