BS-Theory: 2nd order theory -Teil 1
The differential equation for a normal flexural member is:
EI w''''(x) = q(x)
The normal force N is taken into consideration for a buckling member:
EI w''''(x) + N w''(x) = q(x)
For the sake of completeness, the differential equation for an additionally bedded system is shown here since the program also allows parallel processing of systems with 2nd order theory and elastic bedding. The equation is:
EI w''''(x) + N w''(x) + ks w(x) = q(x)
Analysis is performed on the deformed system. In
DIN EN 1993-5
Design of Steel Structures,
Part 5: Piling
analysis using 2nd order theory is recommended for analysis of sheet pile walls under buckling loads. DIN EN 1993-5 refers to
DIN EN 1993-1-1
Design of Steel Structures,
Part 1-1: General Rules and Rules for Buildings
for these analyses. Analysis using 2nd order theory produces more accurate results than the usual and simplified equivalent member method.