Simply Supported Beam Deflection — Worked Example
A complete deflection calculation for a simply supported steel beam under a central point load, with stress check and FEA comparison.
1. Problem
A simply supported steel beam, length L = 2000 mm, carries a central point load P = 15 kN. The cross-section is a rectangular bar 60 mm wide × 30 mm deep. Calculate the maximum deflection, maximum bending stress, and compare with an FEA result.
2. Given
| Parameter | Value | Units |
|---|---|---|
| Material | Structural steel (S355) | — |
| Young's modulus E | 200 | GPa |
| Yield strength Fy | 355 | MPa |
| Span L | 2000 | mm |
| Load P | 15 | kN (central) |
| Width b | 60 | mm |
| Depth h | 30 | mm |
3. Required
- Maximum deflection at midspan
- Maximum bending stress
- Margin of safety against yielding
- Comparison with FEA result
4. Assumptions
- Euler-Bernoulli beam theory (plane sections remain plane)
- Linear elastic material
- Small deflections (slope < 5°)
- Prismatic constant cross-section
- Self-weight neglected
- Supports are ideal pins (no rotational restraint)
5. Governing Equations
Max deflection (central point load): δ_max = P·L³ / (48·E·I) Max bending moment: M_max = P·L / 4 Max bending stress: σ_max = M·c / I = M / Z Section properties (rectangle): I = b·h³/12 Z = b·h²/6 c = h/2
6. Calculation
I = 60 × 30³ / 12 = 60 × 27,000 / 12 = 135,000 mm⁴
Z = 60 × 30² / 6 = 60 × 900 / 6 = 9000 mm³
c = 30 / 2 = 15 mm
M_max = 15,000 × 2000 / 4 = 7,500,000 N·mm = 7.5 kN·m
σ_max = 7,500,000 / 9000 = 833 MPa
δ_max = 15,000 × 2000³ / (48 × 200,000 × 135,000)
= 15,000 × 8 × 10⁹ / (48 × 2.7 × 10¹⁰)
= 1.2 × 10¹⁴ / 1.296 × 10¹²
= 92.6 mm7. Result
σ_max = 833 MPa — exceeds Fy = 355 MPa. The beam yields. δ_max = 92.6 mm — a very large deflection (L/21.6). The beam is grossly under-sized.
8. Check
- Deflection ratio: δ/L = 92.6/2000 = 1/21.6 — far exceeds typical serviceability limit of L/250
- Stress: σ = 833 MPa >> Fy = 355 MPa — confirms yielding
- Sanity: a 60×30 mm bar spanning 2 m under 15 kN is clearly too small — the numbers are physically plausible
- Dimensional check: mm⁴ × GPa = N·mm² → deflection in mm — consistent
9. Interpretation
The beam fails both strength and serviceability. The section needs to be increased. For a target deflection of L/250 = 8 mm, the required I = PL³/(48Eδ) = 1.56 × 10⁶ mm⁴. A 100×50 mm rectangular section (I = 1.04 × 10⁶ mm⁴) is still insufficient; a standard I-section (e.g. 152×152 UC 30, I = 22.3 × 10⁶ mm⁴) would give δ = 0.56 mm and σ = 16 MPa — well within limits.
FEA comparison: a beam model with 20 B31 elements gives δ_max = 92.4 mm (0.2% below the analytical value). A solid model with a coarse mesh (5 mm elements) gives 89 mm — the slight underestimate is due to shear deformation in the solid model (Timoshenko effect), which the Euler-Bernoulli beam formula neglects.
10. Limitations
- Euler-Bernoulli theory neglects shear deformation — significant for deep beams (h/L > 0.1)
- No plasticity — the beam would actually form a plastic hinge at a load lower than that causing first yield
- No self-weight included
- No lateral-torsional buckling check — relevant for slender beams in bending
- The FEA comparison assumes the beam is modelled as a 2D beam, not a 3D solid