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CST plate: deflection and stresses at centroid

Short answer

Using a constant strain triangle, the stiffness matrix is assembled and solved for the free displacements. Deflection at load point: u1=2.05×10^-4 mm, v1=-1.17×10^-3 mm. Stresses at centroid: σx=0.450, σy=0.135, τxy=-0.900 N/mm^2.

A plate of thickness 8 mm is being loaded as shown in the figure. Determine the deflection at the point of load application. Also calculate the stresses at the centroid of the plate. Take E=69900E = 69900 MPa and ν=0.3\nu = 0.3.

[Figure: triangular plate with node 1 at (35, 25) mm, node 2 at (0, 25) mm and node 3 at (0, 0) mm; thickness t=8t = 8 mm; the left edge is fixed; a 90 N vertical load and a 45 N horizontal load act at node 1]

A constant strain triangle (CST) is used with plane stress (E=69900E=69900 MPa, ν=0.3\nu=0.3, t=8t=8 mm). Units: N, mm. Node 1 is the loaded node; the nodes 2 and 3 on the left edge are fixed.

Step 1: Geometry

  • Node 1: (35, 25)(35,\ 25) mm
  • Node 2: (0, 25)(0,\ 25) mm
  • Node 3: (0, 0)(0,\ 0) mm

Area: A=12[x1(y2−y3)+x2(y3−y1)+x3(y1−y2)]=437.5 mm2A=\tfrac12[x_1(y_2-y_3)+x_2(y_3-y_1)+x_3(y_1-y_2)]=437.5\ \text{mm}^2

b1=y2−y3=25, b2=y3−y1=−25, b3=y1−y2=0b_1=y_2-y_3=25,\ b_2=y_3-y_1=-25,\ b_3=y_1-y_2=0 mm

c1=x3−x2=0, c2=x1−x3=35, c3=x2−x1=−35c_1=x_3-x_2=0,\ c_2=x_1-x_3=35,\ c_3=x_2-x_1=-35 mm

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

[B]=12A[250−25000000350−3502535−25−350],2A=875 mm2[B]=\frac{1}{2A}\begin{bmatrix}25 & 0 & -25 & 0 & 0 & 0 \\ 0 & 0 & 0 & 35 & 0 & -35 \\ 0 & 25 & 35 & -25 & -35 & 0\end{bmatrix},\quad 2A=875\ \text{mm}^2 [D]=E1−ν2[1ν0ν10001−ν2]=104[7.6812.30402.3047.6810002.688] 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^{4}\begin{bmatrix}7.681 & 2.304 & 0 \\ 2.304 & 7.681 & 0 \\ 0 & 0 & 2.688\end{bmatrix}\ \text{N/mm}^2

Step 3: Element stiffness matrix

[k]=t A [B]T[D][B]=105[2.1950−2.1950.9220−0.92200.7681.075−0.768−1.0750−2.1951.0753.700−1.997−1.5060.9220.922−0.768−1.9975.0701.075−4.3020−1.075−1.5061.0751.5060−0.92200.922−4.30204.302] N/mm[k]=t\,A\,[B]^T[D][B]= 10^{5}\begin{bmatrix}2.195 & 0 & -2.195 & 0.922 & 0 & -0.922 \\ 0 & 0.768 & 1.075 & -0.768 & -1.075 & 0 \\ -2.195 & 1.075 & 3.700 & -1.997 & -1.506 & 0.922 \\ 0.922 & -0.768 & -1.997 & 5.070 & 1.075 & -4.302 \\ 0 & -1.075 & -1.506 & 1.075 & 1.506 & 0 \\ -0.922 & 0 & 0.922 & -4.302 & 0 & 4.302\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 act at node 1 only. Assumed directions: 45 N horizontal toward +x+x and 90 N vertical downward (−y-y). Self-weight is neglected (not given).

{F}={45−900000} N\{F\}=\begin{Bmatrix}45 \\ -90 \\ 0 \\ 0 \\ 0 \\ 0\end{Bmatrix}\ \text{N}

Boundary conditions and solution

The left edge is fixed, so nodes 2 and 3 have u=v=0u=v=0. Only u1u_1 and v1v_1 are unknown, so use rows and columns 1 and 2 of [k][k].

105[2.195000.768]{u1v1}={45−90}10^{5}\begin{bmatrix}2.195 & 0 \\ 0 & 0.768\end{bmatrix}\begin{Bmatrix}u_1 \\ v_1\end{Bmatrix}=\begin{Bmatrix}45 \\ -90\end{Bmatrix} u1=2.05×10−4 mmv1=−0.001172 mm\begin{aligned} u_1&=2.05\times10^{-4}\ \text{mm} \\ v_1&=-0.001172\ \text{mm} \end{aligned}

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

Centroid: (11.67, 16.67)(11.67,\ 16.67) mm.

{ε}=[B]{d}={5.858×10−60−3.348×10−5}\{\varepsilon\}=[B]\{d\}=\begin{Bmatrix}5.858\times10^{-6} \\ 0 \\ -3.348\times10^{-5}\end{Bmatrix} {σ}=[D]{ε}={0.450.135−0.9} MPa\{\sigma\}=[D]\{\varepsilon\}=\begin{Bmatrix}0.45 \\ 0.135 \\ -0.9\end{Bmatrix}\ \text{MPa}

Answer: deflection at the load point (node 1): u1=2.05×10−4u_1=2.05\times10^{-4} mm (horizontal), v1=−0.00117v_1=-0.00117 mm (vertical, downward). Stresses at the centroid: σx=0.450\sigma_x=0.450, σy=0.135\sigma_y=0.135, τxy=−0.900\tau_{xy}=-0.900 N/mm2^2.

✓ Answer checked by Claude Opus 5.5 (high effort)

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