Description
A quarter-circle beam with a rectangular cross-section w × h is loaded by means of an out-of-plane force F. While neglecting self-weight, the goal is to determine the total deflection uz of the curved beam.
| Material | Isotropic Linear Elastic | Modulus of Elasticity | E | 210000.000 | MPa |
| Poisson's Ratio | ν | 0.296 | - | ||
| Geometry | Rectangular Section | Radius | r | 1.000 | m |
| Cross-Section Width | w | 25.000 | mm | ||
| Cross-Section Height | h | 50.000 | mm | ||
| Load | Out-of-Plane | Force | F | 1.000 | kN |
Analytical Solution
The curved beam is loaded by a bending moment Mb, torsional moment Mt, and by a transverse force T. Considering the following schema, these loads at an arbitrary section are equal to:
The deflection of the structure is determined according to Castigliano's second theorem:
Where the total strain energy U is composed of bending (Ub), torsional (Ut), and shear (Us) components. Using polar coordinates (ds = r dφ):
The total deflection uz is then equal to:
RFEM Settings
- Modeled in RFEM 6.13 and RFEM 5.39
- Element size: lFE = 0.010 m
- Isotropic linear elastic material
- Mindlin plate bending theory
Results
| Entity | Theory uz [mm] |
RFEM 6 uz [mm] |
Ratio [-] |
RFEM 5 uz [mm] |
Ratio [-] |
| Member | 38.960 | 38.973 | 1.000 | 38.973 | 1.000 |
| Plate, horizontal | 39.129 | 1.004 | 38.642 | 0.992 | |
| Plate, vertical | 38.158 | 0.979 | 38.117 | 0.978 | |
| Solid | 38.703 | 0.993 | 38.398 | 0.986 |