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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.

Continuous beam with two 6 m spans: pin at A, rollers at B and C, 10 kN/m uniform load, support B settling 15 mm
Figure 1. The beam, its loads, and its dimensions.
Try it yourself before reading the solution. Show the results
AyA_{y}
28.75 kN
ByB_{y}
62.50 kN
CyC_{y}
28.75 kN

Solution

FEM table: fixed-end moments
#Loading(FEM)i(\mathrm{FEM})_i(FEM)j(\mathrm{FEM})_j
1Uniform load (full span)
w over the whole span
−wL212-\dfrac{wL^2}{12}+wL212+\dfrac{wL^2}{12}
2Point load at midspan
P at x = L/2
−PL8-\dfrac{PL}{8}+PL8+\dfrac{PL}{8}
3Point load (general)
P at a from end i, b from end j
−P a b2L2-\dfrac{P\,a\,b^2}{L^2}+P a2bL2+\dfrac{P\,a^2 b}{L^2}
4Triangular load (0 → w)
0 at end i, w at end j
−wL230-\dfrac{wL^2}{30}+wL220+\dfrac{wL^2}{20}
5Partial uniform load
w from x = a to x = b
−w[x22−2x33L+x44L2]ab-w\Big[\tfrac{x^2}{2}-\tfrac{2x^3}{3L}+\tfrac{x^4}{4L^2}\Big]_a^b+w[x33L−x44L2]ab+w\Big[\tfrac{x^3}{3L}-\tfrac{x^4}{4L^2}\Big]_a^b
6Couple moment
M0 (counterclockwise +) at a from end i, ξ = a/L
M0(1−4ξ+3ξ2)M_0\big(1-4\xi+3\xi^2\big)M0(3ξ2−2ξ)M_0\big(3\xi^2-2\xi\big)
7Support settlement (chord rotation)
ψ = (Δⱼ − Δᵢ)/L, settlement down +
−6EILψ-\dfrac{6EI}{L}\psi−6EILψ-\dfrac{6EI}{L}\psi
8Pinned far end (modified FEM)
if end j is a pin
(FEM)i′=(FEM)i−12(FEM)j(\mathrm{FEM})'_{i} = (\mathrm{FEM})_i - \tfrac{1}{2}(\mathrm{FEM})_jMj=0M_{j} = 0

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.

1Fixed-end moments and released ends

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):

Δ = 1.5 cm10 kN/m10 kN/m30.030.030.030.0ABC
All joints locked: fixed-end moments at the ends of the loaded members (kN·m)

(FEM)near′=(FEM)near−12 (FEM)far(\mathrm{FEM})'_{\text{near}} = (\mathrm{FEM})_{\text{near}} - \tfrac{1}{2}\,(\mathrm{FEM})_{\text{far}} FEM table, row 8

A support settles, so the member undergoes a chord rotation ψ0=Δj−ΔiL\psi_0 = \dfrac{\Delta_j - \Delta_i}{L}, and a fixed-end moment of −6EILψ0-\tfrac{6EI}{L}\psi_0 is added at both ends (already included in the FEM values below): −6EILψ0,AB=−75 kN⋅m-\tfrac{6EI}{L}\psi_{0,AB} = -75\ \text{kN·m}−6EILψ0,BC=75 kN⋅m-\tfrac{6EI}{L}\psi_{0,BC} = 75\ \text{kN·m} FEM table, row 7

Member AB (L = 6.00 m): FEM table, row 1

(FEM)AB=−105 kN⋅m,(FEM)BA=−45 kN⋅m(\mathrm{FEM})_{AB} = -105\ \text{kN·m},\qquad (\mathrm{FEM})_{BA} = -45\ \text{kN·m}⇒ (FEM)BA′=7.50,MAB=0\Rightarrow\ (\mathrm{FEM})'_{BA} = 7.50,\quad M_{AB} = 0

Member BC (L = 6.00 m): FEM table, row 1

(FEM)BC=45 kN⋅m,(FEM)CB=105 kN⋅m(\mathrm{FEM})_{BC} = 45\ \text{kN·m},\qquad (\mathrm{FEM})_{CB} = 105\ \text{kN·m}⇒ (FEM)BC′=−7.50,MCB=0\Rightarrow\ (\mathrm{FEM})'_{BC} = -7.50,\quad M_{CB} = 0

Released end supports: A, C (the moment at these ends is zero, and the member stiffness is taken as 3EI/L3EI/L).

ψ=0.015/6=0.0025\psi = 0.015/6 = 0.0025, 6EIψ/L=756EI\psi/L = 75. It adds to the FEM: −30 − 75 = −105 and 30 − 75 = −45. Releasing A gives −45 + 105/2 = 7.5.

2Distribution factors (interior joints)

At each interior joint, find the member stiffnesses k=4EILk = \tfrac{4EI}{L} (3EIL\tfrac{3EI}{L} if the far end is pinned); the distribution factor is

DFij=kij∑kDF_{ij} = \frac{k_{ij}}{\sum k}

Joint B: DFBA=0.500DF_{BA} = 0.500DFBC=0.500DF_{BC} = 0.500

3Moment distribution table

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 ×12\times\tfrac12 to the far ends. Repeat until the carry-over moments are negligible.

B
MBAM_{BA}MBCM_{BC}
DF0.5000.500
FEM7.50−7.50
ΣM7.50−7.50

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.

4Results and check
MBA=7.50 kN⋅mM_{BA} = 7.50\ \text{kN·m}MBC=−7.50 kN⋅mM_{BC} = -7.50\ \text{kN·m}

✓ The results match the matrix (direct stiffness) solution (largest difference 8.0 × 10⁻¹⁵ kN·m).

5Member equilibrium check (free-body diagrams)

Each member is cut free: the end moments come from above and the end shears from member equilibrium (∑M=0, ∑F=0\sum M = 0,\ \sum F = 0). The arcs and arrows are the end moments and forces acting on the member (kN, kN·m); each box is in equilibrium by itself.

AB7.528.831.310 kN/mBC7.531.328.810 kN/m
6Support reactions and equilibrium check
Δ = 1.5 cm10 kN/m10 kN/m28.862.528.8ABC
Equilibrium check: loads and support reactions together
SupportRx (kN)Ry (kN)M (kN·m, ccw +)
A028.750
B062.500
C028.750
Equilibrium check (ΣFx, ΣFy, and ΣM about the origin):
ΣFx0.00 (reactions) + 0.00 (loads) = 0.00 kN ✓
ΣFy120.00 (reactions) − 120.00 (loads) = 0.00 kN ✓
ΣM0720.00 (reactions) − 720.00 (loads) = 0.00 kN·m ✓

Check a reaction by hand: (10 × 6 × 3 − 7.5) / 6 = 28.75, and VB=2×31.25=62.5V_B = 2 \times 31.25 = 62.5.

Bending moment diagram of the settling beam solved by moment distribution: −7.50 at B and a maximum of 41.33 kN·m in span
Figure 2. Bending moment (kN·m).
Shear diagram of the settling beam solved by moment distribution: 28.75 at A and 31.25 kN just right of B
Figure 3. Shear force (kN).

Results

AyA_{y}
28.75 kN
ByB_{y}
62.50 kN
CyC_{y}
28.75 kN

Matches the independent stiffness solution.

Common mistakes

  • If the sign of 6EIψ/L6EI\psi/L 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.

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