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Collapse value of P: continuous beam

Short answer

Continuous beam with fixed end A. Span AB mechanism gives P = 1.333M_p. Span BC mechanism (hinges at B and under 2P) gives P = 0.625M_p. Combined mechanism gives higher value. Collapse load P_c = 5/8 M_p = 0.625M_p.

For the given continuous beam with the same plastic moment of resistance MPM_P for all the members, calculate the value of P at collapse. [Figure: beam ABC, A fixed, B and C supports; P at 3 m from A, B at 6 m, 2P at 2 m beyond B; BC = 6 m (2 m + 4 m).]

Set-up

Beam ABC: A fixed, B and C supports; AB = 6 m with PP at mid-span J (3 m from A); BC = 6 m with 2P2P at K, 2 m from B and 4 m from C. MpM_p is the same throughout. Degree of indeterminacy = 2; the possible mechanisms are the failure of each span alone and their combination.

Mechanism 1: span AB (hinges at A, J, B)

Mid-span deflection δ=3θ\delta = 3\theta; hinge rotations θ\theta, 2θ2\theta, θ\theta.

P×3θ=Mp(θ+2θ+θ)=4Mpθ  ⇒  P=43Mp=1.333 MpP\times3\theta = M_p(\theta + 2\theta + \theta) = 4M_p\theta \;\Rightarrow\; P = \frac{4}{3}M_p = 1.333\,M_p

Mechanism 2: span BC (hinges at B and K)

Part BK (2 m) rotates θ1\theta_1 about B and part KC (4 m) rotates θ2\theta_2 about C, with 2θ1=4θ22\theta_1 = 4\theta_2, so θ1=2θ2\theta_1 = 2\theta_2. The deflection under the load is δ=4θ2\delta = 4\theta_2.

  • Hinge at B: θ1=2θ2\theta_1 = 2\theta_2; hinge at K: θ1+θ2=3θ2\theta_1 + \theta_2 = 3\theta_2.
  • Internal work =Mp(2θ2+3θ2)=5Mpθ2= M_p(2\theta_2 + 3\theta_2) = 5M_p\theta_2.
  • External work =2P×4θ2=8Pθ2= 2P\times4\theta_2 = 8P\theta_2.
8Pθ2=5Mpθ2  ⇒  P=58Mp=0.625 Mp8P\theta_2 = 5M_p\theta_2 \;\Rightarrow\; P = \frac{5}{8}M_p = 0.625\,M_p

Mechanism 3: combined (hinges at A, J and K; no hinge at B)

With no hinge at B, J-B-K rotates as one rigid piece about support B, so when K moves down J moves up. Let this piece rotate θ\theta: K moves down 2θ2\theta and J moves up 3θ3\theta. Hinge rotations: A θ\theta, J 2θ2\theta, K θ+2θ4=1.5θ\theta + \dfrac{2\theta}{4} = 1.5\theta.

  • Internal work =Mp(θ+2θ+1.5θ)=4.5Mpθ= M_p(\theta + 2\theta + 1.5\theta) = 4.5M_p\theta.
  • External work =2P×2θ−P×3θ=Pθ= 2P\times2\theta - P\times3\theta = P\theta.

This gives P=4.5MpP = 4.5M_p, much larger. (In the opposite sense the external work is negative, so no mechanism forms.)

Collapse load

The lowest value is for span BC:

Answer: Pc=58Mp=0.625 MpP_c = \dfrac{5}{8}M_p = 0.625\,M_p (hinges at B and under the 2P2P load; 2Pc=1.25Mp2P_c = 1.25M_p).

Check (equilibrium)

At collapse MB=−MpM_B = -M_p and MK=+MpM_K = +M_p. For BC: MK=2P×2×46−46Mp=8P3−23MpM_K = \dfrac{2P\times2\times4}{6} - \dfrac{4}{6}M_p = \dfrac{8P}{3} - \dfrac{2}{3}M_p; setting this equal to MpM_p gives P=58MpP = \dfrac{5}{8}M_p. In AB, MAM_A is not fixed by statics at collapse (span AB is still indeterminate). For example, with MA=−0.5MpM_A = -0.5M_p the moment under PP is PL4+MA+MB2=0.9375Mp−0.75Mp=0.19Mp\dfrac{PL}{4} + \dfrac{M_A + M_B}{2} = 0.9375M_p - 0.75M_p = 0.19M_p, well within MpM_p, so the yield condition is also satisfied.

✓ Answer checked by Claude Opus 5.5 (high effort)

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