“…In many aspects, plant searcher braids can be compared to cables or ropes, except that they typically do not have a core around which individual “wires” are wrapped (Evans et al, 2005 ; Costello, 2012 ). Based on observations of real intertwined searcher stems, the following boundary conditions were assumed to allow for an approximated calculation of the axial second moments of area of a structure consisting of n intertwined shoots: (1) All searcher stems are cylindrical with circular cross-sections, (2) the cross-sections of individual stems are the same for all stems and remain constant over the length of an intertwined structure, i.e., the stems have no taper, and cross-sectional area is given as A = n · π · r s 2 (to simplify comparability, radii are normalized to r si = r s = 1), (3) the centers of gravity of the n intertwined stems ( cg 1 , cg 2 , cg 3 , cg 4 ) are at the same constant distance from the centroid of the intertwined structure C , i.e., they are arranged on a circle with radius r p , and (4) intertwined stems do not overlap and are symmetrically arranged at angles φ i = 2π · i/n , with i = 1,2,3,4,… n , and (5) a searcher braid is treated as a unit in which individual stems are fixed with respect to each other.…”