“…They are found everywhere at different length scales from suboceanic cables to human-sized rods and ropes, to plant and animal microstructural fabrics, to molecular pillars and chains such as carbon nanotubes and double-stranded deoxyribonucleic acids (DNAs). Their unique large deformability have received attention from the scientific community including the field of theoretical and applied mechanics, and even at present the problems associated with the intricate deformation into three-dimensional (3D) configurations are being tackled in areas such as the compressive buckling from 2D into 3D architecture 1-3 , the coiling of ealstic filaments deployed on substrate 4,5 , the mechanics of knots 6,7 , and the 3D growing rods [8][9][10][11][12] .The deformation of a slender elastic body is concisely described by the elastic rod model represented by a single arc-length parameter prescribing the center line 13,14 . Depending on the elastic rod, there are four types of deformations, i.e., stretching/compression, shearing, bending, and twisting, which are paired with the axial and shear forces and the bending and torsion moments induced inside the rod.…”