I may not agree the use of UG23 and UG 28, which is for bucking stress across the entire cross section, that is also based on ‘line of support’, the “L” dimension. Cone can be defines as line of support both ends, either end or none, that will impact the dimension “L”, hence impact the allowable buckling stress. In my case I have two cones, such that no single value for the allowable buckling stress can be obtained because I can define line of support in many ways. But regardless how I define, it can be all wrong because there is no external pressure to justify the line of support during lifting or transportation. If using the entire length as the “L”, that will make the allowable buckling stress very small and to use that as the allowable compressive stress due to bending moment, may be overkilled.
Vessel can have many vacuum stiffing rings for external pressure. Does it means we can use “B” from UG23 and 28 to calculate the allowable buckling stress and treat it as the allowable compressive stress due to bending moment during lifting or transportation ? I wouldn’t think so.
In my sketch, the maximum compressive stress is close to 2/3 of the yield due to head heavy. If UG23 and 28 are a valid method, then I can simply add two stiffing ring between the maximum point, may be 1’ part, to make B exceeds compressive stress, or even I can define the small cone as line of support and make B large enough, and then I claim the maximum compressive stress is fine? Does not sound right.
The maximum compressive stress from bending moment will be very local at the farest point from the vessel center line. I do not think a gross buckling will occur even the compressive stress exceeds the “B” value from UG23 and UG28 if that can be calculated.
I could be wrong for all the thinking, but I am still not convinced the use of UG23 and 28.