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CST plate: stresses at centroid

Short answer

For the single CST, stresses are constant, so centroid stresses equal element stresses: sigma_x=0, sigma_y=0, tau_xy=-1.333 N/mm^2, indicating pure shear. The free node displacement is u2=0.00693 mm horizontally with v2=0.

A steel plate of thickness 10 mm is being loaded in the structural system as shown in the figure below. Calculate stresses at the centroid of the plate. E=200E = 200 GPa, ν=0.3\nu = 0.3.

[Figure: right triangular plate, 300 mm along the top edge (supported/hatched) and 400 mm along the left vertical edge; a distributed load of 10 kN/mm2^2 [as printed] acts on the left edge]

A CST has constant strain, so the stresses at the centroid equal the stresses everywhere in the plate. The plate is modelled as one CST in plane stress (units N and mm).

Assumptions

  • The load "10 kN/mm2^2" is read as a line load w=10w = 10 kN/m =10= 10 N/mm along the 400 mm left edge, acting horizontally (normal to the edge, in +x+x). Total load =10×400=4000= 10\times400 = 4000 N, shared equally by the end nodes of the edge.
  • Nodes (anticlockwise): 1 (0, 0) top-left, 2 (0, -400) bottom-left, 3 (300, 0) top-right. The top edge 1-3 is supported, so u1=v1=u3=v3=0u_1=v_1=u_3=v_3=0.
  • E=2×105E=2\times10^5 N/mm2^2, ν=0.3\nu=0.3, t=10t=10 mm.

Step 1: Geometry

A=12(300)(400)=60000 mm2A=\tfrac12(300)(400)=60000\ \text{mm}^2

b1=y2−y3=−400, b2=y3−y1=0, b3=y1−y2=400b_1=y_2-y_3=-400,\ b_2=y_3-y_1=0,\ b_3=y_1-y_2=400; c1=x3−x2=300, c2=x1−x3=−300, c3=x2−x1=0c_1=x_3-x_2=300,\ c_2=x_1-x_3=-300,\ c_3=x_2-x_1=0.

[B]=1120000[−400000400003000−30000300−400−30000400][B]=\frac{1}{120000}\begin{bmatrix} -400&0&0&0&400&0\\ 0&300&0&-300&0&0\\ 300&-400&-300&0&0&400\end{bmatrix}

Step 2: [D] for plane stress

[D]=E1−ν2[10.300.310000.35]=[2197806593406593421978000076923] N/mm2[D]=\frac{E}{1-\nu^2}\begin{bmatrix}1&0.3&0\\0.3&1&0\\0&0&0.35\end{bmatrix}=\begin{bmatrix} 219780 & 65934 & 0 \\ 65934 & 219780 & 0 \\ 0 & 0 & 76923 \end{bmatrix}\ \text{N/mm}^2

Step 3: Stiffness of the free node 2

[k]22=tA[B]T[D][B]∣u2,v2=[28846200824176] N/mm[k]_{22}=tA[B]^T[D][B]\Big|_{u_2,v_2}=\begin{bmatrix} 288462 & 0 \\ 0 & 824176 \end{bmatrix}\ \text{N/mm}

Step 4: Displacement

Load at node 2: F2x=4000/2=2000F_{2x}=4000/2=2000 N, F2y=0F_{2y}=0.

u2=2000288461.5=0.00693 mm,v2=0u_2=\frac{2000}{288461.5}=0.00693\ \text{mm},\qquad v_2=0

Step 5: Stresses

{ε}=[B]{u}=[00−1.733×10−5],{σ}=[D]{ε}=[00−1.333] N/mm2\{\varepsilon\}=[B]\{u\}=\begin{bmatrix}0\\0\\-1.733\times10^{-5}\end{bmatrix},\qquad \{\sigma\}=[D]\{\varepsilon\}=\begin{bmatrix}0\\0\\-1.333\end{bmatrix}\ \text{N/mm}^2

Check: the element force at node 2 in the xx direction, from tA[B]T{σ}tA[B]^T\{\sigma\}, is t2(b2σx+c2τxy)=5×(−300)×(−1.333)=2000\tfrac{t}{2}(b_2\sigma_x+c_2\tau_{xy})=5\times(-300)\times(-1.333)=2000 N, which balances the applied F2xF_{2x}.

Answer: at the centroid σx=0\sigma_x=0, σy=0\sigma_y=0, τxy=−1.333\tau_{xy}=-1.333 N/mm2^2, i.e. the plate is in pure shear.

✓ Answer checked by Claude Opus 5.5 (high effort)

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