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Two-hinged arch: thrust with rib shortening, support yield

Short answer

Use two-hinged parabolic arch with H as redundant, including rib shortening and 6 mm outward support yield. EI0=600 kNm², EAc=10⁶ kN. Compute numerator (∫M0y dx/EI0 – δ)=149.994, denominator (∫y²dx/EI0+∫cos²α dx/EA_c)=1.92006. H=78.12 kN. Crown BM=131.28 kNm sagging, quarter-span BM=-51.54 kNm.

A two hinge parabolic arch of span 60 m and central rise of 6 m is subjected to a concentrated load of 40 kN at the crown. Allowing for rib shortening and yielding of support B by 6 mm outwards horizontally, determine the horizontal thrust. Also draw the BMD. Take I0=6×103 cm4I_0 = 6\times10^{3}\ \text{cm}^4 [?], Ac=1000 cm2A_c = 1000\ \text{cm}^2, E=10 kN/mm2E = 10\ \text{kN/mm}^2 and consider Ix=I0sec⁡αI_x = I_0 \sec\alpha.

A two-hinged arch has one redundant, the horizontal thrust HH. Taking Ix=I0sec⁡αI_x = I_0\sec\alpha, the compatibility equation with rib shortening and yielding of a support is

H=∫M0 yEI0 dx−δ∫y2EI0 dx+∫cos⁡2αEAc dxH = \frac{\displaystyle\int \frac{M_0\,y}{EI_0}\,dx - \delta}{\displaystyle\int \frac{y^2}{EI_0}\,dx + \int \frac{\cos^2\alpha}{EA_c}\,dx}

where δ\delta is the outward yield of support B. (The small axial-force term of the free structure is neglected, as is usual.)

Data (converted to kN and m)

  • L=60L = 60 m, h=6h = 6 m, parabola y=4h x(L−x)L2=x(60−x)150y = \dfrac{4h\,x(L-x)}{L^2} = \dfrac{x(60-x)}{150}
  • EI0=10 kN/mm2×6×103 cm4=107×6×10−5=600EI_0 = 10\,\text{kN/mm}^2 \times 6\times10^3\,\text{cm}^4 = 10^7 \times 6\times10^{-5} = 600 kNm2^2
  • EAc=107×0.1=106EA_c = 10^7 \times 0.1 = 10^6 kN, δ=6\delta = 6 mm =0.006= 0.006 m
  • VA=VB=20V_A = V_B = 20 kN; M0=20xM_0 = 20x for 0≤x≤300 \le x \le 30 (peak 600 kNm at the crown)

Integrals

∫060M0y dx=2∫03020x⋅x(60−x)150 dx=90000∫060y2 dx=8h2L15=1152∫060cos⁡2α dx=57.08\begin{aligned} \int_0^{60} M_0 y\,dx &= 2\int_0^{30} 20x\cdot\frac{x(60-x)}{150}\,dx = 90000 \\ \int_0^{60} y^2\,dx &= \frac{8h^2L}{15} = 1152 \\ \int_0^{60} \cos^2\alpha\,dx &= 57.08 \end{aligned}

(tan⁡α=dydx=4h(L−2x)L2\tan\alpha = \dfrac{dy}{dx} = \dfrac{4h(L-2x)}{L^2}, so cos⁡2α=11+tan⁡2α\cos^2\alpha = \dfrac{1}{1+\tan^2\alpha}.)

∫M0y dxEI0=90000600=150.000∫y2 dxEI0=1152600=1.9200∫cos⁡2α dxEAc=57.08106=5.708×10−5\begin{aligned} \frac{\int M_0 y\,dx}{EI_0} &= \frac{90000}{600} = 150.000 \\ \frac{\int y^2\,dx}{EI_0} &= \frac{1152}{600} = 1.9200 \\ \frac{\int \cos^2\alpha\,dx}{EA_c} &= \frac{57.08}{10^6} = 5.708\times10^{-5} \end{aligned}

Horizontal thrust

H=150.000−0.0061.9200+5.708×10−5=78.12 kNH = \frac{150.000 - 0.006}{1.9200 + 5.708\times10^{-5}} = 78.12\ \text{kN}

For comparison: without rib shortening and yielding, H=25PL128h=78.125H = \dfrac{25PL}{128h} = 78.125 kN. With the printed I0I_0 the arch is very flexible in bending, so rib shortening and a 6 mm yield change the thrust only slightly. (A stiffer rib, say I0=6×106I_0 = 6\times10^6 cm4^4, would give H=72.83H = 72.83 kN.)

Bending moment M=M0−HyM = M_0 - H y

xx (m)yy (m)M0M_0 (kNm)MM (kNm)
0.00.0000.00.00
7.52.625150.0-55.06
15.04.500300.0-51.54
22.55.625450.010.58
30.06.000600.0131.28

The BMD is symmetric about the crown: zero at the hinges A and B, hogging (negative) about the quarter points, and sagging with a peak of 131.28 kNm under the load at the crown.

Answer: H≈78.12H \approx 78.12 kN; crown BM =131.28= 131.28 kNm (sagging), BM at x=15x = 15 m =−51.54= -51.54 kNm.

✓ Answer checked by Claude Opus 5.5 (high effort)

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