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Arch 100 m rise 12 m: rolling UDL 60 m, section 10 m

Short answer

Maximum horizontal thrust is 1750 kN. At 10 m from left end, maximum positive moment is +2571 kN m with thrust 531.5 kN; maximum negative moment is -2560 kN m with thrust 1518.5 kN.

A three hinged parabolic arch of span 100 m and rise 12 m carries a UDL of intensity 20 kN/m of length 60 m moving from left to right. Calculate horizontal thrust and maximum bending moments at a distance 10 m from the left end; using ILD.

Data: parabolic three-hinged arch, L=100L = 100 m, f=12f = 12 m, y=0.0048 x(100−x)y = 0.0048\,x(100-x). A UDL of 20 kN/m, 60 m long, rolls from left to right. Section at x=10x = 10 m: y=4.32y = 4.32 m, tan⁡θ=0.0048 (100−20)=0.384\tan\theta = 0.0048\,(100-20) = 0.384.

Horizontal thrust

HH is maximum when the load is symmetrical about the crown (20 m to 80 m): the ILD ordinates are x′2f=0.833\dfrac{x'}{2f} = 0.833 at 20 m and L4f=2.083\dfrac{L}{4f} = 2.083 at the crown:

Hmax=20×[2×(0.833+2.083)2×30]=1750 kNH_{max} = 20\times\left[2\times\frac{(0.833+2.083)}{2}\times 30\right] = 1750\ \text{kN}

ILDs for the section at x = 10 m

The ILD of the horizontal thrust is H=x′2fH = \dfrac{x'}{2f} for a unit load at x′x' left of the crown and L−x′2f\dfrac{L-x'}{2f} right of it (peak L4f=2.0833\dfrac{L}{4f} = 2.0833 at the crown). The ILD of the bending moment at the section is M=Mb−H yM = M_b - H\,y.

x (m)PointILD of HILD of M at section
0A00
10section D0.4177.2
35.71neutral point1.4880
50crown C2.083-4
100B00

The ILD of MM crosses zero at the neutral point, 35.71 m from AA (vertically below the intersection of line ADAD produced and line BCBC). The ordinates are positive on one side of it and negative on the other.

Maximum positive bending moment

The UDL covers the span from x=0x = 0 to 35.71 m (the rest of the load is still off the span), which is exactly the region where the ILD is positive.

M=w×(area of ILD)=20×128.571=2571.4 kN mH=w×(area of ILD of H)=20×26.573=531.46 kN\begin{aligned} M &= w\times(\text{area of ILD}) = 20\times 128.571 = 2571.4\ \text{kN m}\\ H &= w\times(\text{area of ILD of }H) = 20\times 26.573 = 531.46\ \text{kN} \end{aligned}

At the section: y=4.32y = 4.32 m, θ=21.01∘\theta = 21.01^\circ, simple-beam shear Vb=386.73V_b = 386.73 kN.

V=Vbcos⁡θ−Hsin⁡θ=386.73×0.9335−531.46×0.3585=170.51 kNN=Vbsin⁡θ+Hcos⁡θ=386.73×0.3585+531.46×0.9335=634.78 kN\begin{aligned} V &= V_b\cos\theta - H\sin\theta = 386.73\times0.9335 - 531.46\times0.3585 = 170.51\ \text{kN}\\ N &= V_b\sin\theta + H\cos\theta = 386.73\times0.3585 + 531.46\times0.9335 = 634.78\ \text{kN} \end{aligned}

Maximum negative bending moment

The negative region (35.71 m to 100 m) is longer than the load, so the 60 m load is placed with equal ILD ordinates at its two ends: it covers x=36.67x = 36.67 m to 96.67 m (the whole load is on the span).

M=w×(area of ILD)=20×(−128)=−2560 kN mH=w×(area of ILD of H)=20×75.926=1518.52 kN\begin{aligned} M &= w\times(\text{area of ILD}) = 20\times(-128) = -2560\ \text{kN m}\\ H &= w\times(\text{area of ILD of }H) = 20\times 75.926 = 1518.52\ \text{kN} \end{aligned}

At the section: y=4.32y = 4.32 m, θ=21.01∘\theta = 21.01^\circ, simple-beam shear Vb=400.0V_b = 400.0 kN.

V=Vbcos⁡θ−Hsin⁡θ=400.0×0.9335−1518.52×0.3585=−170.94 kNN=Vbsin⁡θ+Hcos⁡θ=400.0×0.3585+1518.52×0.9335=1560.99 kN\begin{aligned} V &= V_b\cos\theta - H\sin\theta = 400.0\times0.9335 - 1518.52\times0.3585 = -170.94\ \text{kN}\\ N &= V_b\sin\theta + H\cos\theta = 400.0\times0.3585 + 1518.52\times0.9335 = 1560.99\ \text{kN} \end{aligned}

Answer: maximum thrust =1750= 1750 kN; maximum bending moment at 10 m from the left end =+2571= +2571 kN m (load from the support up to the neutral point), with thrust H=531.5H = 531.5 kN, and −2560-2560 kN m (negative), with H=1518.5H = 1518.5 kN.

✓ Answer checked by Claude Opus 5.5 (high effort)

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