TY - CHAP
T1 - Sectional Shape Functions for a Box Beam Under Flexure
AU - Kim, Yoon Young
AU - Jang, Gang Won
AU - Choi, Soomin
N1 - Publisher Copyright:
© 2023, Springer Nature Singapore Pte Ltd.
PY - 2023
Y1 - 2023
N2 - The sectional shape functions of a box beam subjected to a flexural load are derived in this chapter using a procedure similar to that presented in Chaps. 4–6. (Other approaches may be found in Ferradi and Cespedes (2014) and Bebiano et al. (2015)). As in the cases for torsional or extensional loads, three types of deformable section modes are considered in addition to rigid-body section modes: (1) warping modes {Wk}k=1,2,…, (2) unconstrained distortion modes {χk}k=1,2,…, and (3) constrained distortion modes {η¯k,η^k}k=1,2,…. The warping mode Wk has the z-directional shape function ψzWk(s) only, which depicts the wall-membrane deformations of a beam section. On the other hand, the unconstrained distortion mode χk has both the s-directional shape function ψsχk(s) representing wall-membrane deformation and the n-directional shape function ψnχk(s) representing wall-bending deformation. The constrained distortional modes η¯k and η^k have only the n-directional shape functions ψnη¯k(s) and ψnη^k(s), respectively, representing wall-bending deformations. The shape functions ψsχk(s) and ψzWk(s) representing wall-membrane deformations are derived in Sect. 7.2 while ψnχk(s), ψnη¯k(s) and ψnη^k(s) representing wall-bending deformations are derived in Sects. 7.3–7.5. Section 7.6 presents numerical results using the derived modes.
AB - The sectional shape functions of a box beam subjected to a flexural load are derived in this chapter using a procedure similar to that presented in Chaps. 4–6. (Other approaches may be found in Ferradi and Cespedes (2014) and Bebiano et al. (2015)). As in the cases for torsional or extensional loads, three types of deformable section modes are considered in addition to rigid-body section modes: (1) warping modes {Wk}k=1,2,…, (2) unconstrained distortion modes {χk}k=1,2,…, and (3) constrained distortion modes {η¯k,η^k}k=1,2,…. The warping mode Wk has the z-directional shape function ψzWk(s) only, which depicts the wall-membrane deformations of a beam section. On the other hand, the unconstrained distortion mode χk has both the s-directional shape function ψsχk(s) representing wall-membrane deformation and the n-directional shape function ψnχk(s) representing wall-bending deformation. The constrained distortional modes η¯k and η^k have only the n-directional shape functions ψnη¯k(s) and ψnη^k(s), respectively, representing wall-bending deformations. The shape functions ψsχk(s) and ψzWk(s) representing wall-membrane deformations are derived in Sect. 7.2 while ψnχk(s), ψnη¯k(s) and ψnη^k(s) representing wall-bending deformations are derived in Sects. 7.3–7.5. Section 7.6 presents numerical results using the derived modes.
UR - http://www.scopus.com/inward/record.url?scp=85159858015&partnerID=8YFLogxK
U2 - 10.1007/978-981-19-7772-5_7
DO - 10.1007/978-981-19-7772-5_7
M3 - Chapter
AN - SCOPUS:85159858015
T3 - Solid Mechanics and its Applications
SP - 215
EP - 262
BT - Solid Mechanics and its Applications
PB - Springer Science and Business Media B.V.
ER -