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Collapse load P: portal frame with UDL 2P/l

Short answer

Beam, sway, and combined mechanisms yield P = 6Mp/l, 2Mp/l and 2Mp/l. The critical mechanism has a plastic hinge inside the UDL-loaded column, giving collapse load Pc = (1 + √3/2)Mp/l ≈ 1.866 Mp/l.

For the given portal frame with same plastic moment of resistance MpM_p for all the members, calculate the value of P at collapse. [Figure: portal frame, both bases hinged, height l, span l divided into three parts of l/3; vertical loads P at the first and second third-points of the beam; UDL of 2P/l on the left column.]

Assumptions

  • Portal frame: A and F hinged, columns AB and EF of height ll, beam BE of span ll; the vertical loads PP act at C and D (the third points). A UDL of 2P/l2P/l acts horizontally to the right on column AB. All members have the same plastic moment MpM_p. Take l=1l = 1 in the tables.
  • Hinged bases: degree of indeterminacy =4−3=1= 4 - 3 = 1.

Mechanisms

Mechanism 1: beam mechanism

Taking l=1l = 1. No sway; hinges at B, C and E. Part BC (l/3l/3) rotates 2θ/32\theta/3 and CE (2l/32l/3) rotates θ/3\theta/3, so the hinge at C turns θ\theta.

HingeRotationPlastic momentInternal work
C1θ1\thetaMpM_p1 Mpθ1\,M_p\theta
B (beam end)23θ\frac{2}{3}\thetaMpM_p23 Mpθ\frac{2}{3}\,M_p\theta
E (beam end)13θ\frac{1}{3}\thetaMpM_p13 Mpθ\frac{1}{3}\,M_p\theta

Internal work =2 Mp θ= 2\,M_p\,\theta.

LoadDisplacement along the loadExternal work
P at C29θ\frac{2}{9}\theta29P θ\frac{2}{9}P\,\theta
P at D19θ\frac{1}{9}\theta19P θ\frac{1}{9}P\,\theta
2P/l on AB-0P θ0P\,\theta

Equation: P×13 θ=2 MpθP\times \frac{1}{3}\,\theta = 2\,M_p\theta, so P=6 Mp/lP = 6\,M_p/l.

Mechanism 2: sway mechanism (hinges at B and E)

The columns (height ll) rotate θ\theta about the hinged bases and the beam moves lθl\theta. The hinges are at B and E, at the beam ends.

HingeRotationPlastic momentInternal work
B (beam end)1θ1\thetaMpM_p1 Mpθ1\,M_p\theta
E (beam end)1θ1\thetaMpM_p1 Mpθ1\,M_p\theta

Internal work =2 Mp θ= 2\,M_p\,\theta.

LoadDisplacement along the loadExternal work
P at C0θ0\theta0P θ0P\,\theta
P at D0θ0\theta0P θ0P\,\theta
2P/l on AB-1P θ1P\,\theta

Equation: P×1 θ=2 MpθP\times 1\,\theta = 2\,M_p\theta, so P=2 Mp/lP = 2\,M_p/l.

Mechanism 3: combined mechanism

Combine 1 and 2 so that the hinge at B cancels; hinges at C and E.

HingeRotationPlastic momentInternal work
C1θ1\thetaMpM_p1 Mpθ1\,M_p\theta
E (beam end)1θ1\thetaMpM_p1 Mpθ1\,M_p\theta

Internal work =2 Mp θ= 2\,M_p\,\theta.

LoadDisplacement along the loadExternal work
P at C29θ\frac{2}{9}\theta29P θ\frac{2}{9}P\,\theta
P at D19θ\frac{1}{9}\theta19P θ\frac{1}{9}P\,\theta
2P/l on AB-23P θ\frac{2}{3}P\,\theta

Equation: P×1 θ=2 MpθP\times 1\,\theta = 2\,M_p\theta, so P=2 Mp/lP = 2\,M_p/l.

Mechanism 4: sway with the hinge inside the loaded column. With a UDL on AB, the maximum moment in the column is not at B but within the column, at height yy above A. Let the column part AK rotate θ\theta about A; the upper part of the column and the beam translate yθy\theta, and the right column rotates ϕ=yθ/l=yθ\phi = y\theta/l = y\theta (with l=1l = 1). Hinges: K (θ\theta) and E (ϕ\phi).

Internal=Mpθ(1+y)External=2Pl[y2θ2+(1−y) yθ]=2Pθ y(1−y2)\begin{aligned} \text{Internal} &= M_p\theta(1 + y) \\ \text{External} &= \tfrac{2P}{l}\left[\tfrac{y^2\theta}{2} + (1-y)\,y\theta\right] = 2P\theta\,y\left(1 - \tfrac y2\right) \end{aligned} P=Mp(1+y)2y−y2P = \frac{M_p(1+y)}{2y - y^2}

Minimising: y2+2y−2=0y^2 + 2y - 2 = 0, so y=3−1=0.732 ly = \sqrt3 - 1 = 0.732\,l, and

P=3 Mp43−6=(1+32)Mpl=1.866 MplP = \frac{\sqrt3\,M_p}{4\sqrt3 - 6} = \left(1 + \frac{\sqrt3}{2}\right)\frac{M_p}{l} = 1.866\,\frac{M_p}{l}

Collapse load

This is lower than the sway (2.0), combined (2.0) and beam (6) values, and a check of the other hinge positions (for example, adding a hinge at C to mechanism 4) gives nothing lower:

Answer: Pc=(1+32)Mpl=1.866 MplP_c = \left(1 + \dfrac{\sqrt3}{2}\right)\dfrac{M_p}{l} = 1.866\,\dfrac{M_p}{l}.

✓ Answer checked by Claude Opus 5.5 (high effort)

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