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Simply supported beam with two elements

Short answer

With two 2 m beam elements (EI=1.6×10⁶ N·m²), symmetry gives θ₂=0 and θ₃=−θ₁. Solving yields mid-span deflection 8.33 mm downward, support rotations ±6.25×10⁻³ rad. Reactions are 5 kN each. Results match the exact solution PL³/(48EI) exactly because the cubic element is exact for nodal loads.

A simply supported beam of span 4 m carries a point load of 10 kN at mid-span. E=200E = 200 GPa and I=8×106 mm4I = 8\times10^6\ \text{mm}^4. Model the beam with two equal beam elements. Find the deflection at mid-span, the rotations at the supports and the support reactions, and compare the deflection with the exact value.

Data

EI=200×109×8×10−6=1.6×106 N m2EI = 200\times10^9 \times 8\times10^{-6} = 1.6\times10^6\ \text{N m}^2, Le=2L_e = 2 m for each element.

EILe3=1.6×1068=2×105\dfrac{EI}{L_e^3} = \dfrac{1.6\times10^6}{8} = 2\times10^5 N/m.

Nodes: 1 (left support), 2 (mid-span), 3 (right support). Degrees of freedom: (v1,θ1,v2,θ2,v3,θ3)(v_1, \theta_1, v_2, \theta_2, v_3, \theta_3). Boundary conditions: v1=v3=0v_1 = v_3 = 0.

   ^              10 kN
   |               |
   o======= (1) ===o======= (2) ===o
  1                2                3
  |<------ 2 m ---->|<------ 2 m -->|

Element matrix (each element)

With Le=2L_e = 2:

[k]=2×105[1212−12121216−128−12−1212−12128−1216][k] = 2\times10^5\begin{bmatrix} 12 & 12 & -12 & 12 \\ 12 & 16 & -12 & 8 \\ -12 & -12 & 12 & -12 \\ 12 & 8 & -12 & 16 \end{bmatrix}

Reduced system

Free DOFs: θ1,v2,θ2,θ3\theta_1, v_2, \theta_2, \theta_3. By symmetry about mid-span, θ2=0\theta_2 = 0 and θ3=−θ1\theta_3 = -\theta_1.

Row for θ1\theta_1 (element 1, second row), with v1=0v_1 = 0, θ2=0\theta_2 = 0:

2×105 (16θ1−12v2)=02\times10^5\,(16\theta_1 - 12v_2) = 0

Row for v2v_2 (sum of element 1 third row and element 2 first row), with v1=v3=0v_1 = v_3 = 0, θ2=0\theta_2 = 0, θ3=−θ1\theta_3 = -\theta_1:

2×105 (−12θ1+24v2+12θ3)=2×105 (−24θ1+24v2)=−10 0002\times10^5\,(-12\theta_1 + 24v_2 + 12\theta_3) = 2\times10^5\,(-24\theta_1 + 24v_2) = -10\,000

So θ1=0.75v2\theta_1 = 0.75v_2, and −18v2+24v2=−0.05-18v_2 + 24v_2 = -0.05 gives

v2=−0.008333 m,θ1=−0.00625 radv_2 = -0.008333\ \text{m},\qquad \theta_1 = -0.00625\ \text{rad}

Reactions

R1=2×105(12v1+12θ1−12v2+12θ2)=2.4×106(−0.00625+0.008333)=5000R_1 = 2\times10^5(12v_1 + 12\theta_1 - 12v_2 + 12\theta_2) = 2.4\times10^6(-0.00625 + 0.008333) = 5000 N, and by symmetry R3=5000R_3 = 5000 N.

Comparison

Exact: vmax=PL348EI=10 000(4)348(1.6×106)=8.333v_{max} = \dfrac{PL^3}{48EI} = \dfrac{10\,000(4)^3}{48(1.6\times10^6)} = 8.333 mm; exact support rotation PL216EI=6.25×10−3\dfrac{PL^2}{16EI} = 6.25\times10^{-3} rad. The FE results match exactly because the cubic element is exact for a load applied at a node.

Answer: mid-span deflection = 8.33 mm downward; support rotations = 6.25 ×10−3\times10^{-3} rad (left clockwise, right anticlockwise); reactions = 5 kN each; the FE result equals the exact value.

✓ Answer checked by Claude Opus 5.5 (high effort)

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