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This is the differential equation for the shell section. It relates the change in the longitudinal bending moment my to the hoop force nx and the hydrostatic pressure py. • Kinematic compatibility: dw 1 dw = − (r dφ)2 + ν ( )2 iv) dy 2 dy • Linear material law: nx = E t (1/r) dw/dy v) Substitute iv) and v) into iii) to eliminate strains: d 2

Author

Jonas Gyllensten

Language

EN