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CST steel plate: stiffness, load vector, displacements

Short answer

For the single plane-stress CST element, form [B] and [D], then [k]=t A [B]^T[D][B] as given in N/mm. The load vector has F_x1=12.5 N and F_y1=-32.71 N at node 1, with nodes 2 and 3 fixed. Solving gives u_1=3.25e-5 mm and v_1=-2.98e-5 mm.

A steel plate of uniform thickness 10 mm is being loaded as shown in the figure below. Considering the plane stress condition, determine the stiffness matrix, load vector and nodal displacements of the given CST element. Take modulus of elasticity =200×103= 200\times10^3 MPa, Poisson's ratio =0.3= 0.3 and unit weight of steel =78.5= 78.5 kN/m3^3.

[Figure: right triangular plate, 500 mm wide at the top (fixed along the top edge) and 500 mm deep on the left edge, which carries a distributed load of 5 kN/m2^2]

Assumptions: plane stress, one CST element. Nodes: 1 = bottom of left edge (0,−500)(0,-500), 2 = top right (500,0)(500,0), 3 = top left (0,0)(0,0) (counter-clockwise). E=200×103E=200\times10^3 MPa, ν=0.3\nu=0.3, t=10t=10 mm, unit weight 78.5×10−678.5\times10^{-6} N/mm3^3. Units: N, mm.

Step 1: Geometry

  • Node 1 (bottom of left edge): (0, −500)(0,\ -500) mm
  • Node 2 (top right): (500, 0)(500,\ 0) mm
  • Node 3 (top left): (0, 0)(0,\ 0) mm

Area: A=12[x1(y2−y3)+x2(y3−y1)+x3(y1−y2)]=125000 mm2A=\tfrac12[x_1(y_2-y_3)+x_2(y_3-y_1)+x_3(y_1-y_2)]=125000\ \text{mm}^2

b1=y2−y3=0, b2=y3−y1=500, b3=y1−y2=−500b_1=y_2-y_3=0,\ b_2=y_3-y_1=500,\ b_3=y_1-y_2=-500 mm

c1=x3−x2=−500, c2=x1−x3=0, c3=x2−x1=500c_1=x_3-x_2=-500,\ c_2=x_1-x_3=0,\ c_3=x_2-x_1=500 mm

Step 2: [B] and [D] matrices (plane stress)

[B]=12A[005000−50000−500000500−50000500500−500],2A=250000 mm2[B]=\frac{1}{2A}\begin{bmatrix}0 & 0 & 500 & 0 & -500 & 0 \\ 0 & -500 & 0 & 0 & 0 & 500 \\ -500 & 0 & 0 & 500 & 500 & -500\end{bmatrix},\quad 2A=250000\ \text{mm}^2 [D]=E1−ν2[1ν0ν10001−ν2]=105[2.1980.65900.6592.1980000.769] N/mm2[D]=\frac{E}{1-\nu^2}\begin{bmatrix}1&\nu&0\\ \nu&1&0\\0&0&\frac{1-\nu}{2}\end{bmatrix}=10^{5}\begin{bmatrix}2.198 & 0.659 & 0 \\ 0.659 & 2.198 & 0 \\ 0 & 0 & 0.769\end{bmatrix}\ \text{N/mm}^2

Step 3: Element stiffness matrix

[k]=t A [B]T[D][B]=106[0.38500−0.385−0.3850.38501.099−0.33000.330−1.0990−0.3301.0990−1.0990.330−0.385000.3850.385−0.385−0.3850.330−1.0990.3851.484−0.7140.385−1.0990.330−0.385−0.7141.484] N/mm[k]=t\,A\,[B]^T[D][B]= 10^{6}\begin{bmatrix}0.385 & 0 & 0 & -0.385 & -0.385 & 0.385 \\ 0 & 1.099 & -0.330 & 0 & 0.330 & -1.099 \\ 0 & -0.330 & 1.099 & 0 & -1.099 & 0.330 \\ -0.385 & 0 & 0 & 0.385 & 0.385 & -0.385 \\ -0.385 & 0.330 & -1.099 & 0.385 & 1.484 & -0.714 \\ 0.385 & -1.099 & 0.330 & -0.385 & -0.714 & 1.484\end{bmatrix}\ \text{N/mm}

(DOF order: u1,v1,u2,v2,u3,v3u_1,v_1,u_2,v_2,u_3,v_3.)

Step 4: Load vector

Loads: (i) self-weight W=γtA=78.5×10−6×10×125000=98.125W=\gamma tA=78.5\times10^{-6}\times10\times125000=98.125 N, shared equally: W/3=32.708W/3=32.708 N downward at each node. (ii) The 5 kN/m2^2 = 0.005 N/mm2^2 traction on the left edge 1-3 (length 500 mm, acting horizontally toward +x+x, assumed): total 0.005×10×500=250.005\times10\times500=25 N, half (12.5 N) to each end node.

{F}={12.5−32.710−32.7112.5−32.71} N\{F\}=\begin{Bmatrix}12.5 \\ -32.71 \\ 0 \\ -32.71 \\ 12.5 \\ -32.71\end{Bmatrix}\ \text{N}

Boundary conditions and solution

The top edge is fixed, so nodes 2 and 3 have zero displacement. The only free node is node 1 (u1,v1u_1,v_1); use rows and columns 1 and 2 of [k][k].

106[0.385001.099]{u1v1}={12.5−32.71}10^{6}\begin{bmatrix}0.385 & 0 \\ 0 & 1.099\end{bmatrix}\begin{Bmatrix}u_1 \\ v_1\end{Bmatrix}=\begin{Bmatrix}12.5 \\ -32.71\end{Bmatrix} u1=3.25×10−5 mmv1=−2.976×10−5 mm\begin{aligned} u_1&=3.25\times10^{-5}\ \text{mm} \\ v_1&=-2.976\times10^{-5}\ \text{mm} \end{aligned}

Strains and stresses (constant over the element, so equal at the centroid)

Centroid: (166.67, −166.67)(166.67,\ -166.67) mm.

{ε}=[B]{d}={05.953×10−8−6.5×10−8}\{\varepsilon\}=[B]\{d\}=\begin{Bmatrix}0 \\ 5.953\times10^{-8} \\ -6.5\times10^{-8}\end{Bmatrix} {σ}=[D]{ε}={0.0039250.01308−0.005} MPa\{\sigma\}=[D]\{\varepsilon\}=\begin{Bmatrix}0.003925 \\ 0.01308 \\ -0.005\end{Bmatrix}\ \text{MPa}

Answer: [k][k] as above (units N/mm); nodal loads {F}\{F\} as above (only node 1 matters: Fx1=12.5F_{x1}=12.5 N, Fy1=−32.71F_{y1}=-32.71 N); u1=3.25×10−5u_1=3.25\times10^{-5} mm, v1=−2.98×10−5v_1=-2.98\times10^{-5} mm. The plate is very stiff, so the displacements are extremely small.

✓ Answer checked by Claude Opus 5.5 (high effort)

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