Mechanics of deformable solids Definition
Euler–Bernoulli beam equation
Builds on Beam theoryBending momentSecond moment of areaYoung's modulus
Definition
Let a straight beam occupy along its axis. Let be the Young's modulus of its material and the second moment of area of its cross-section about the neutral axis. Let be the transverse load per unit length and the deflection of the axis, both measured in the same direction. The Euler–Bernoulli beam equation is The bending moment and the shear force are and . For a beam with mass per unit length the dynamic equation is
Remarks
Example: a cantilever with constant , clamped at and loaded by a point force at , has . Check: on , , so , and . The tip deflection is . A simply supported beam with constant under a uniform load has the largest deflection at mid-span.
Non-example: with and constant satisfies the equation. It fails the condition of a simply supported beam, so it is not the deflection of such a beam.
The usual boundary conditions are at a clamped end, at a simply supported end, and at a free end when is constant. The equation assumes small deflections and neglects shear deformation; Timoshenko–Ehrenfest beam theory adds the shear.
Reading path
To understand this page from the ground up, read these 5 pages in order. The foundations come first.
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- no evidence level
- Beam theory concept
- Bending moment concept
- Second moment of area concept
- Young's modulus concept
- Euler–Bernoulli beam equation definition
Further reading
About this page
| Tag | CPMD36AH43 |
|---|---|
| URI | m2://CPMD36AH43 |
| Kind | definition |
| Writing | W0 stub |
| MSC | 74K10, 74B05, 34B60 |
| Defines | Euler–Bernoulli beam equation |
| Uses | Beam theory, Bending moment, Second moment of area, Young's modulus |
| Changed | 3 November 2026 |
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