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Collapse load of frame with UDL on column

Short answer

Using kinematik theorem: beam mechanism gives λ=M_p/12≈0.0833M_p; sway mechanism λ=M_p/25=0.04M_p. The lowest is from combined mechanism (hinges at B, under the 4m load, D) yielding λ=13M_p/370≈0.0351M_p. Thus collapse load factor is 13M_p/370; all loads proportionally increase.

Evaluate the collapse load for the given frame. [Figure: portal frame ABCD, height 5 m, A hinged, D fixed; beam BC of 6 m with 20 kN at 2 m and 20 kN at 4 m from B; plastic moments: AB = MpM_p, beam BC = 2Mp2M_p, column CD = 2Mp2M_p; 10 kN/m UDL on column CD.]

Assumptions

  • Portal frame: A (0,0) hinged, B (0,5), C (6,5), D (6,0) fixed. Column AB has plastic moment MpM_p, beam BC and column CD have 2Mp2M_p.
  • The loads (two 20 kN point loads at 2 m and 4 m from B, and 10 kN/m on column CD) are applied proportionally with a load factor λ\lambda; the 10 kN/m acts horizontally towards the left on CD. The collapse load factor λc\lambda_c is found in terms of MpM_p (in kN·m).
  • Method: kinematic (upper-bound) theorem with virtual work, ∑Mpθ=λ∑Pδ\sum M_p\theta = \lambda \sum P\delta.

Possible hinge positions

B (in the weaker member AB, MpM_p), under each 20 kN load, C and D. Degree of indeterminacy = 5 - 3 = 2 (A hinged gives 2 reactions, D fixed gives 3), so with 5 critical sections the number of independent mechanisms is 5 - 2 = 3: two beam mechanisms (one with the hinge under each load) and the sway mechanism. Combining them gives further mechanisms.

Mechanism 1: beam mechanism

Joints B and C do not move. The beam BC forms hinges under the second load P2 (4 m from B) and at C; at B the hinge forms at the top of the weaker column AB (MpM_p). With rotation θ\theta at P2, the left portion (4 m) rotates θ/3\theta/3 and the right portion (2 m) rotates 2θ/32\theta/3 (rigid portions); the deflection under the second load is 4×θ/34\times\theta/3.

HingeRotationPlastic momentInternal work
under the second 20 kN1θ1\theta2Mp2M_p2 Mpθ2\,M_p\theta
C23θ\frac{2}{3}\theta2Mp2M_p43 Mpθ\frac{4}{3}\,M_p\theta
B (top of column AB)13θ\frac{1}{3}\thetaMpM_p13 Mpθ\frac{1}{3}\,M_p\theta

Internal work =113 Mp θ= \frac{11}{3}\,M_p\,\theta.

LoadDisplacement along the loadExternal work
20 kN at 2 m23θ\frac{2}{3}\theta403 kN⋅m θ\frac{40}{3}\,\text{kN·m}\,\theta
20 kN at 4 m43θ\frac{4}{3}\theta803 kN⋅m θ\frac{80}{3}\,\text{kN·m}\,\theta
10 kN/m UDL on CD-0 kN⋅m θ0\,\text{kN·m}\,\theta

Equation: λ×40 θ=113 Mpθ\lambda\times40\,\theta = \frac{11}{3}\,M_p\theta, so λ=11120Mp=0.0917 Mp\lambda = \frac{11}{120}M_p = 0.0917\,M_p.

With the hinge under the first load instead (2 m from B), the portions rotate 2θ/32\theta/3 and θ/3\theta/3: internal work =2Mpθ+Mp⋅23θ (B)+2Mp⋅13θ (C)=103Mpθ= 2M_p\theta + M_p\cdot\frac{2}{3}\theta\ (\text{B}) + 2M_p\cdot\frac{1}{3}\theta\ (\text{C}) = \frac{10}{3}M_p\theta, and the external work is again 40θ40\theta, so λ=112Mp=0.0833 Mp\lambda = \frac{1}{12}M_p = 0.0833\,M_p (the lower beam value).

Mechanism 2: sway mechanism

Columns rotate through θ\theta about A and D, and the beam translates horizontally by 5θ5\theta. Hinges form at B (the weaker section is AB, MpM_p), C and D. The vertical loads do no work. (The column CD is moved to the left by the UDL.)

HingeRotationPlastic momentInternal work
B (in column AB)1θ1\thetaMpM_p1 Mpθ1\,M_p\theta
C1θ1\theta2Mp2M_p2 Mpθ2\,M_p\theta
D1θ1\theta2Mp2M_p2 Mpθ2\,M_p\theta

Internal work =5 Mp θ= 5\,M_p\,\theta.

LoadDisplacement along the loadExternal work
20 kN at 2 m0θ0\theta0 kN⋅m θ0\,\text{kN·m}\,\theta
20 kN at 4 m0θ0\theta0 kN⋅m θ0\,\text{kN·m}\,\theta
10 kN/m UDL on CD-125 kN⋅m θ125\,\text{kN·m}\,\theta

Equation: λ×125 θ=5 Mpθ\lambda\times125\,\theta = 5\,M_p\theta, so λ=125Mp=0.0400 Mp\lambda = \frac{1}{25}M_p = 0.0400\,M_p.

Mechanism 3: combined mechanism

Combine mechanisms 1 and 2 so that the hinge at C cancels. Both columns rotate 2θ/32\theta/3 (sway to the left), the beam portion from B to the hinge rotates θ/3\theta/3 in the opposite sense (hinge at B =2θ/3+θ/3=θ= 2\theta/3 + \theta/3 = \theta), and the portion from the hinge to C rotates 2θ/32\theta/3 with the column (hinge at the load =θ= \theta, no hinge at C).

HingeRotationPlastic momentInternal work
B (in column AB)1θ1\thetaMpM_p1 Mpθ1\,M_p\theta
under the second 20 kN1θ1\theta2Mp2M_p2 Mpθ2\,M_p\theta
D23θ\frac{2}{3}\theta2Mp2M_p43 Mpθ\frac{4}{3}\,M_p\theta

Internal work =133 Mp θ= \frac{13}{3}\,M_p\,\theta.

LoadDisplacement along the loadExternal work
20 kN at 2 m23θ\frac{2}{3}\theta403 kN⋅m θ\frac{40}{3}\,\text{kN·m}\,\theta
20 kN at 4 m43θ\frac{4}{3}\theta803 kN⋅m θ\frac{80}{3}\,\text{kN·m}\,\theta
10 kN/m UDL on CD-2503 kN⋅m θ\frac{250}{3}\,\text{kN·m}\,\theta

Equation: λ×3703 θ=133 Mpθ\lambda\times\frac{370}{3}\,\theta = \frac{13}{3}\,M_p\theta, so λ=13370Mp=0.03514 Mp\lambda = \frac{13}{370}M_p = 0.03514\,M_p.

(The same combination with the hinge under the first load gives λ=11245Mp=0.0449 Mp\lambda = \frac{11}{245}M_p = 0.0449\,M_p, which is higher.)

Collapse load

The smallest value governs (combined mechanism, lower than both the beam value 0.0833 and the sway value 0.04):

λc=13370Mp=0.0351 Mp\lambda_c = \frac{13}{370}M_p = 0.0351\,M_p

So the collapse loads are: point loads 20λc=0.703 Mp20\lambda_c = 0.703\,M_p kN each and UDL 10λc=0.351 Mp10\lambda_c = 0.351\,M_p kN/m (with MpM_p in kN·m). A check with a linear-programming search over all possible hinge sets gave the same value 0.03514 Mp0.03514\,M_p.

Answer: collapse load factor λc=13Mp/370≈0.0351 Mp\lambda_c = 13M_p/370 \approx 0.0351\,M_p (combined mechanism with hinges at B, under the 20 kN load at 4 m, and at D).

✓ Answer checked by Claude Opus 5.5 (high effort)

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