As mentioned in the Introduction, the volume of the infinite trunk at the reference point of the moment and transverse force influence surfaces for circular cylindrical shells cannot be neglected as for plates. The reason is simply, that, because of the curvature of the middle surface, these stress resultants, as compared to those in plates, will be reduced considerably, the singularity at the
... [Show full abstract] reference, however, remains. It seems advisable, contrary to the usual method of computation (cf. [6]), to proceed, herein, from the last contour line, plotted in the influence surface. Corresponding to Fig. 8, it can be assumed, herein, that the cut-off volume ΔV, due to the shell singularity, is equal to the plate singularity if the considered contour line is of the same shape. For v = 1/6 follows from [6], as plotted in Fig. 8, the contour line for mx
(or mφ
, respectively, by exchanging x and φ), and for q̄φ
(or q̄x
, respectively).