Axissymmetric Buckling of Hollow Spheres And Hemispheres
Axissymmetric Buckling of Hollow Spheres And Hemispheres
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Thus for example, the branch joining B^ „ at its lower critical pressure should be called Br o' But since Br n bifurcates from P^ we also call it Bk -, . The notation in Table II is now rather obvious if we merely observe that most critical pressures, P . Or P . , have dual representations. On the branches bifurcating from unsymmetric eigenvalues the eigenvalues are also upper or lower critical pressures, that is, P = P . Or P = P -, . '^ ' ' n n, l n n, l In Figures 3 and ^ we show how the sol...utions for P decreasing on the lowest symmetric bifurcation branch Br -, go over continuously to the solutions for P increasing on the adjacent branch B^ „. There is an obvious difference in the shapes and stresses between the states on branches Br -, and Br q for P > 0. 05; compare Figures 3a and ^a with Figures 3c and 4c. However, for P near Pg -, - ^ ({ n ~ 0. 0105 the shapes on both branches are quite similar. Thus there is no abrupt change in mode (see Figures 3b and 4b). As P Increases the states on Br Q develop a boundary layer near 9 = tt/2.
What to read after Axissymmetric Buckling of Hollow Spheres And Hemispheres?
You can find similar books in the "Read Also" column, or choose other free books by Louis Bauer to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
Thus for example, the branch joining B^ „ at its lower critical pressure should be called Br o' But since Br n bifurcates from P^ we also call it Bk -, . The notation in Table II is now rather obvious if we merely observe that most critical pressures, P . Or P . , have dual representations. On the branches bifurcating from unsymmetric eigenvalues the eigenvalues are also upper or lower critical pressures, that is, P = P . Or P = P -, . '^ ' ' n n, l n n, l In Figures 3 and ^ we show how the sol...utions for P decreasing on the lowest symmetric bifurcation branch Br -, go over continuously to the solutions for P increasing on the adjacent branch B^ „. There is an obvious difference in the shapes and stresses between the states on branches Br -, and Br q for P > 0. 05; compare Figures 3a and ^a with Figures 3c and 4c. However, for P near Pg -, - ^ ({ n ~ 0. 0105 the shapes on both branches are quite similar. Thus there is no abrupt change in mode (see Figures 3b and 4b). As P Increases the states on Br Q develop a boundary layer near 9 = tt/2.
What to read after Axissymmetric Buckling of Hollow Spheres And Hemispheres?
You can find similar books in the "Read Also" column, or choose other free books by Louis Bauer to read onlineMoreLess
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