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Arch: reactions, BM, thrust and shear at D by ILD

Short answer

Reactions: V_A = 440 kN, V_B = 210 kN, H = 437.5 kN. At section D (15 m from A) with UDL and point load: M = 675 kN m, N = 459.35 kN, V = 0 kN. ILD method yields same results.

In the three hinged parabolic arch loaded as shown below, determine reactions at supports and also find bending moment, normal thrust and radial shear force at section D 15 m far from A. Draw influence line diagram for bending moment and normal thrust at that point and again determine the bending moment and normal thrust at D by using the ILD. [Figure: parabolic three hinged arch, span 50 m, rise 10 m at the crown C; C is 30 m from A (and 20 m from B as dimensioned); D at 15 m from A; 20 kN/m UDL over the left portion A to C; 50 kN vertical load 20 m from B.]

Data and assumptions: parabolic three-hinged arch, span L=50L = 50 m, rise f=10f = 10 m (the parabola is symmetrical about mid-span, y=4×10 x(50−x)502=0.016 x(50−x)y = \dfrac{4\times 10\,x(50-x)}{50^2} = 0.016\,x(50-x)). As dimensioned, the crown hinge CC is 30 m from AA and 20 m from BB, where yC=9.6y_C = 9.6 m. UDL 20 kN/m on ACAC (x=0x = 0 to 30 m); 50 kN vertical at 20 m from BB, i.e. at CC (x=30x = 30 m). Section DD at x=15x = 15 m: yD=8.4y_D = 8.4 m, tan⁡θ=0.016 (50−30)=0.32\tan\theta = 0.016\,(50-30) = 0.32, θ=17.74∘\theta = 17.74^\circ.

Reactions

Vertical reactions (moments about AA): the loads are 600 kN (UDL, at 15 m) and 50 kN (at 30 m).

VB×50=600×15+50×30=10500⇒VB=210 kN,VA=650−210=440 kNV_B\times 50 = 600\times 15 + 50\times 30 = 10500 \Rightarrow V_B = 210\ \text{kN}, \qquad V_A = 650 - 210 = 440\ \text{kN}

Horizontal thrust (hinge at CC, left part, load at CC itself has no moment about CC):

H×9.6=VA×30−600×15=4200⇒H=437.5 kNH\times 9.6 = V_A\times 30 - 600\times 15 = 4200 \Rightarrow H = 437.5\ \text{kN}

(Check from the right part: H×9.6=VB×20=4200H\times 9.6 = V_B\times 20 = 4200.)

Forces at D

M=VA×15−20×15×7.5−H yD=6600−2250−437.5×8.4=675 kN mVb=VA−20×15=140 kNV=Vbcos⁡θ−Hsin⁡θ=140(0.9523)−437.5(0.3047)=0 kNN=Vbsin⁡θ+Hcos⁡θ=140(0.3047)+437.5(0.9523)=459.35 kN\begin{aligned} M &= V_A\times 15 - 20\times 15\times 7.5 - H\,y_D = 6600 - 2250 - 437.5\times 8.4 = 675\ \text{kN m}\\ V_b &= V_A - 20\times 15 = 140\ \text{kN}\\ V &= V_b\cos\theta - H\sin\theta = 140(0.9523) - 437.5(0.3047) = 0\ \text{kN}\\ N &= V_b\sin\theta + H\cos\theta = 140(0.3047) + 437.5(0.9523) = 459.35\ \text{kN} \end{aligned}

Influence lines for M and N at D (unit load at x')

  • Thrust (hinge at xC=30x_C = 30, yC=9.6y_C = 9.6): for x′≤30x'\le 30 the right part CBCB is a two-force member, so H=RB(L−xC)yC=x′50⋅209.6=x′24H = \dfrac{R_B(L-x_C)}{y_C} = \dfrac{x'}{50}\cdot\dfrac{20}{9.6} = \dfrac{x'}{24}; for x′≥30x'\ge 30, H=RA xCyC=50−x′16H = \dfrac{R_A\,x_C}{y_C} = \dfrac{50-x'}{16} (peak 1.251.25 at CC).
  • M=Mb−H yDM = M_b - H\,y_D and N=Vbsin⁡θ+Hcos⁡θN = V_b\sin\theta + H\cos\theta, where VbV_b is the simple-beam shear.
Unit load at x' (m)HM at D (m)N at D
0000
150.6255.250.5038
150.6255.250.8086
301.25-4.51.3124
400.625-2.250.6562
50000

The N-ILD is discontinuous at DD by sin⁡θ\sin\theta (the two rows at 15 m are the load just left and just right of DD).

M and N at D from the ILDs

UDL on ACAC (area of ILD from 0 to 30 m) plus the 50 kN load at CC (ordinate at 30 m):

M=20×(45)+50×(−4.5)=675 kN mN=20×(19.687)+50×(1.3124)=459.35 kN\begin{aligned} M &= 20\times(45) + 50\times(-4.5) = 675\ \text{kN m}\\ N &= 20\times(19.687) + 50\times(1.3124) = 459.35\ \text{kN} \end{aligned}

These agree with the values from direct equilibrium.

Answer: reactions VA=440V_A = 440 kN, VB=210V_B = 210 kN, H=437.5H = 437.5 kN (at both supports). At DD: M=675M = 675 kN m, N=459.35N = 459.35 kN, V=0V = 0 kN.

✓ Answer checked by Claude Opus 5.5 (high effort)

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