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CST: nodal deformations and stresses

Short answer

Using one CST in plane stress with the given G, node 3 displaces u3=-2.143e-7 m and v3=-4.699e-8 m. The constant element stresses are sigma_x=0.748, sigma_y=-15.70, and tau_xy=-37.50 kN/m^2.

A steel plate of 10 mm thickness is loaded as shown in the figure below. For the plane stress problem, obtain the nodal deformations and the stresses in the CST element. Take E=2×105E = 2\times10^5 MPa, G=105×103G = 105\times10^3 MPa and unit weight of steel is 78.5 kN/m3^3.

[Figure: right triangular plate with node 1 at the origin, node 2 at 80 cm to the right of node 1 and node 3 at 60 cm above node 1; a 50 kN/m2^2 distributed load acts on the left edge 1-3, directed in the negative x direction]

The plate is idealised as one constant strain triangle (CST) in plane stress. Units: kN and m.

Assumptions

  • Nodes: 1 (0, 0), 2 (0.8, 0), 3 (0, 0.6) m, numbered anticlockwise. Thickness t=0.01t = 0.01 m.
  • The base nodes 1 and 2 are fixed (u1=v1=u2=v2=0u_1=v_1=u_2=v_2=0); node 3 is free. The figure gives no other support, so this is the usual reading.
  • E=2×108E = 2\times10^{8} kN/m2^2 and G=105×106G = 105\times10^{6} kN/m2^2 are used exactly as given, so ν=E2G−1=−0.0476\nu = \dfrac{E}{2G}-1 = -0.0476 (the given GG is not consistent with ν=0.3\nu=0.3; the stated data are followed).

Step 1: Geometry

A=12(0.8)(0.6)=0.24 m2A = \tfrac12(0.8)(0.6) = 0.24\ \text{m}^2

With b1=y2−y3=−0.6, b2=y3−y1=0.6, b3=y1−y2=0b_1=y_2-y_3=-0.6,\ b_2=y_3-y_1=0.6,\ b_3=y_1-y_2=0 and c1=x3−x2=−0.8, c2=x1−x3=0, c3=x2−x1=0.8c_1=x_3-x_2=-0.8,\ c_2=x_1-x_3=0,\ c_3=x_2-x_1=0.8:

[B]=12A[−0.600.60000−0.80000.8−0.8−0.600.60.80][B]=\frac{1}{2A}\begin{bmatrix} -0.6 & 0 & 0.6 & 0 & 0 & 0 \\ 0 & -0.8 & 0 & 0 & 0 & 0.8 \\ -0.8 & -0.6 & 0 & 0.6 & 0.8 & 0 \end{bmatrix}

Step 2: Elasticity matrix (plane stress)

[D]=E1−ν2[1ν0ν10001−ν2]=[2.0045×108−95454550−95454552.0045×1080001.05×108] kN/m2[D]=\frac{E}{1-\nu^2}\begin{bmatrix}1&\nu&0\\ \nu&1&0\\ 0&0&\frac{1-\nu}{2}\end{bmatrix} = \begin{bmatrix} 2.0045\times10^{8} & -9545455 & 0 \\ -9545455 & 2.0045\times10^{8} & 0 \\ 0 & 0 & 1.05\times10^{8} \end{bmatrix}\ \text{kN/m}^2

(the shear term is GG).

Step 3: Element stiffness [k]=tA[B]T[D][B][k]=tA[B]^T[D][B]

Only the rows and columns of the free dofs (u3,v3)(u_3, v_3) are needed:

[k]33=[700000001336364] kN/m[k]_{33}=\begin{bmatrix} 700000 & 0 \\ 0 & 1336364 \end{bmatrix}\ \text{kN/m}

Step 4: Nodal loads

  • Edge load: 50×0.01×0.6=0.3050\times0.01\times0.6 = 0.30 kN in the −x-x direction, shared equally by nodes 1 and 3, so F3x=−0.15F_{3x}=-0.15 kN.
  • Self weight: W=78.5×0.24×0.01=0.1884W = 78.5\times0.24\times0.01 = 0.1884 kN, one third to each node, so F3y=−0.0628F_{3y}=-0.0628 kN.

Step 5: Nodal deformations

[700000001336363.6][u3v3]=[−0.15−0.0628]\begin{bmatrix}700000 & 0\\ 0 & 1336363.6\end{bmatrix}\begin{bmatrix}u_3\\ v_3\end{bmatrix}=\begin{bmatrix}-0.15\\ -0.0628\end{bmatrix} u3=−2.143×10−7 m,v3=−4.699×10−8 mu_3 = -2.143\times10^{-7}\ \text{m},\qquad v_3 = -4.699\times10^{-8}\ \text{m}

All other nodal displacements are zero.

Step 6: Stresses, {σ}=[D][B]{u}\{\sigma\}=[D][B]\{u\}

{σ}=[σxσyτxy]=[0.748−15.70−37.50] kN/m2\{\sigma\}=\begin{bmatrix}\sigma_x\\ \sigma_y\\ \tau_{xy}\end{bmatrix}=\begin{bmatrix}0.748\\ -15.70\\ -37.50\end{bmatrix}\ \text{kN/m}^2

Check: the element force at node 3 in the xx direction, from tA[B]T{σ}tA[B]^T\{\sigma\}, is t2(b3σx+c3τxy)=0.005×0.8×(−37.5)=−0.15\tfrac{t}{2}(b_3\sigma_x+c_3\tau_{xy})=0.005\times0.8\times(-37.5)=-0.15 kN, which balances the applied F3xF_{3x}.

Answer: u3=−2.143×10−7u_3=-2.143\times10^{-7} m, v3=−4.699×10−8v_3=-4.699\times10^{-8} m; σx=0.748\sigma_x=0.748, σy=−15.70\sigma_y=-15.70, τxy=−37.50\tau_{xy}=-37.50 kN/m2^2 (constant over the element).

✓ Answer checked by Claude Opus 5.5 (high effort)

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