Beam Bending Stress Calculator
Calculate bending stress in beams from bending moment, moment of inertia, and cross-section geometry.
Bending Stress Varies Linearly Through Beam Depth
In elastic beam bending, fibers on one side of the neutral axis stretch while fibers on the other side compress. The flexure formula σ=My/I gives normal stress at distance y from the neutral axis. Stress is zero at the neutral axis and reaches its largest magnitude at the extreme fibers where |y| is greatest.
The second moment of area I captures how cross-section geometry resists bending. Placing material farther from the neutral axis increases I strongly, which is why I-beams and deep sections can resist bending efficiently. The simple formula assumes elastic behavior and beam-theory conditions.
| Symbol | Meaning | Why it appears / units |
|---|---|---|
| M | Bending moment | N·m at the section being checked. |
| y | Distance from neutral axis | m; signed through the beam depth. |
| I | Second moment of area | m⁴. |
| S=I/c | Section modulus | m³; convenient for maximum bending stress. |
A moment diagram identifies where bending stress is likely largest along a beam, while the cross-section identifies where it is largest through the depth. Both loading and geometry therefore matter.
The section geometry is the first bending-stress check. Confirm that I is taken about the actual bending axis and that y is the distance to the point where stress is wanted. At the neutral axis y=0, bending stress must be zero; moving toward the extreme fiber must increase its magnitude linearly.
Worked Examples
Common Mistakes
J is associated with circular-shaft torsion. Beam bending uses the area second moment about the relevant neutral axis.
Maximum stress often occurs where |M| is largest, which must be found from statics and the moment diagram.
The linear flexure formula is not a complete model after yielding or near stress concentrations, holes, notches, or very short/deep beams.
Frequently Asked Questions
Formula Explorer connections
Interpretation: This engineering-physics relationship connects load, material property, geometry, deformation or system response. Assumption: Confirm material linearity, geometry, support conditions and safety convention. Small deformation, elastic behavior and ideal loading are common assumptions.