The maximum bending stress in a curved beam having symmetrical section always occurs at the
Inside fibre
When a beam is subjected to bending, internal stresses are developed within its cross-section to resist the applied bending moment. For straight beams, the bending stress is zero at the neutral axis and increases linearly with the distance from the neutral axis, reaching maximum values at the outermost fibres.
However, the behavior of curved beams under bending is different from that of straight beams. Due to the initial curvature, the distribution of bending stress across the section is not linear. This non-linear distribution arises because the fibres closer to the center of curvature are shorter, and those further away are longer, even before bending occurs. When subjected to a bending moment, the strain distribution is still generally assumed to be linear across the depth, but the corresponding stress distribution becomes hyperbolic.
In curved beams, the neutral axis, where the bending stress is zero, does not coincide with the centroidal axis. Instead, the neutral axis shifts towards the center of curvature. The bending stress ($\sigma_b$) in a curved beam section at a distance 'y' from the neutral axis is given by a formula, often based on the Winkler-Bach theory. A simplified representation of the stress distribution shows that the magnitude of the stress is inversely proportional to the distance from the center of curvature.
Consequently, the fibres closer to the center of curvature (the inside fibres) experience a higher magnitude of stress compared to the fibres further away from the center of curvature (the outside fibres), for the same magnitude of strain difference from the neutral axis. This effect is more pronounced for beams with a larger curvature (smaller radius of curvature relative to the section depth).
Therefore, even for a symmetrical cross-section, the maximum bending stress (in terms of magnitude) under a given bending moment will occur at the fibre located closest to the center of curvature, which is the inside fibre.
Based on the principles of curved beam theory, the maximum bending stress in a curved beam with a symmetrical section always occurs at the inside fibre.
| Feature | Straight Beam | Curved Beam |
|---|---|---|
| Bending Stress Distribution | Linear | Hyperbolic (Non-linear) |
| Neutral Axis location (Symmetrical Section) | Coincides with Centroidal axis | Shifted from Centroidal axis (towards center of curvature) |
| Location of Maximum Bending Stress | Outermost Fibres (equal magnitude top/bottom for symmetrical section) | Fibre closest to center of curvature (Inside fibre) |
| Stress at Neutral Axis | Zero | Zero |
The analysis of stress in curved beams is more complex than in straight beams. Key concepts include:
Understanding the shift of the neutral axis and the hyperbolic nature of the stress distribution is crucial to correctly identifying the location of maximum bending stress in a curved beam.
The maximum shear stress in a circular beam is
An increase in load at the free end of a cantilever is likely to cause failure-
The stresses caused by the bending moment is called -
The bending moment at a section of a beam will have its local maximum where the shear force is-