Moment Distribution · Problem 3 of 5All problems
Moment Distribution Solved ProblemMoment distribution support settlement, two-span beam
Problem. The two-span beam has a pin at A and rollers at B and C. A uniform load of 10 kN/m acts over its full length, and support B settles 15 mm. EI = 30,000 kN·m². Use moment distribution to find the end moments and support reactions, and draw the shear and moment diagrams.

Try it yourself before reading the solution. Show the results
- 28.75 kN
- 62.50 kN
- 28.75 kN
Solution
FEM table: fixed-end moments
| # | Loading | ||
|---|---|---|---|
| 1 | Uniform load (full span) w over the whole span | ||
| 2 | Point load at midspan P at x = L/2 | ||
| 3 | Point load (general) P at a from end i, b from end j | ||
| 4 | Triangular load (0 → w) 0 at end i, w at end j | ||
| 5 | Partial uniform load w from x = a to x = b | ||
| 6 | Couple moment M0 (counterclockwise +) at a from end i, ξ = a/L | ||
| 7 | Support settlement (chord rotation) ψ = (Δⱼ − Δᵢ)/L, settlement down + | ||
| 8 | Pinned far end (modified FEM) if end j is a pin |
Member fixed at both ends. Sign convention: an end moment is positive when it acts clockwise on the member (counterclockwise on the joint), as in Hibbeler. Use row 8 for a pinned end. The values match the engine's load integration exactly.
Sign convention: as in Hibbeler, a member end moment is positive when it acts clockwise on the member (counterclockwise on the joint). Kassimali's counterclockwise-positive values have the opposite sign. Each span is first treated as fixed at both ends to get its fixed-end moments. At a pin or roller end support the moment must be zero, so that end is released at the start and half of its moment is carried over to the other end (near = the end that stays fixed; far = the released end):
FEM table, row 8
A support settles, so the member undergoes a chord rotation , and a fixed-end moment of is added at both ends (already included in the FEM values below): FEM table, row 7
Member AB (L = 6.00 m): FEM table, row 1
Member BC (L = 6.00 m): FEM table, row 1
Released end supports: A, C (the moment at these ends is zero, and the member stiffness is taken as ).
, . It adds to the FEM: −30 − 75 = −105 and 30 − 75 = −45. Releasing A gives −45 + 105/2 = 7.5.
At each interior joint, find the member stiffnesses ( if the far end is pinned); the distribution factor is
Joint B:
The FEM row lists the modified fixed-end moments. Balance each joint (distribute the negative of the unbalanced moment according to the distribution factors), then carry over to the far ends. Repeat until the carry-over moments are negligible.
| B | ||
|---|---|---|
| DF | 0.500 | 0.500 |
| FEM | 7.50 | −7.50 |
| ΣM | 7.50 | −7.50 |
At B, 7.5 − 7.5 = 0: the structure and load are symmetric, so nothing is left to distribute. The table ends in one row.
✓ The results match the matrix (direct stiffness) solution (largest difference 8.0 × 10⁻¹⁵ kN·m).
Each member is cut free: the end moments come from above and the end shears from member equilibrium (). The arcs and arrows are the end moments and forces acting on the member (kN, kN·m); each box is in equilibrium by itself.
| Support | Rx (kN) | Ry (kN) | M (kN·m, ccw +) |
|---|---|---|---|
| A | 0 | 28.75 | 0 |
| B | 0 | 62.50 | 0 |
| C | 0 | 28.75 | 0 |
Check a reaction by hand: (10 × 6 × 3 − 7.5) / 6 = 28.75, and .


Results
- 28.75 kN
- 62.50 kN
- 28.75 kN
Matches the independent stiffness solution.
Common mistakes
- If the sign of is reversed, the result can still satisfy statics, so an equilibrium check won't catch the error.
- When 3EI/L is used at a pinned end, no moment is carried over to that end. If you carry over, the stiffness must be 4EI/L.
- Once the reactions are found, check vertical equilibrium: 28.75 + 62.5 + 28.75 = 10 × 12.
Same problem, another method
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