Abstract
To obtain proper stresses , three new triangular elements are formulated in this study. First, a complementary energy functional is used within an element for the analysis of plane problems. In this energy manifestation, the Airy stress function will be applied as a functional variable. Then, some basic analytical solutions are assigned for the stress functions. These trial functions are matched with each element number of degrees of freedom. The result is a number of equations with anonymous constants. Subsequently, according to the principle of minimum complementary energy, the unknown constants can be expressed in terms of displacements. Finally, this system can be rewritten in terms of the nodal displacement. In this way, three new triangular elements are formulated. To validate the results, extensive numerical studies are performed. The findings clearly demonstrate accuracies of structural displacements as well as stresses.
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Abbreviations
- AT6:
-
Accurate triangular element
- t :
-
Thickness of the element
- U :
-
Displacement vector along element boundaries
- \( \mu \) :
-
Poisson’s ratio
- \( {D_{ij}} \) :
-
Elastic modulus
- \( l \) and m :
-
Direction cosines of the outer normal
- \( {{\varPi }}_C^* \) :
-
Complementary energy within the element
- \( \sigma \) :
-
The stress vector of the element
- C :
-
Elastic flexibility matrix
- \( \varphi \) :
-
Airy stress function
- \( {C_{ij}} \) :
-
Elastic compliances
- \( {u_i} \) :
-
Nodal displacements belong to x
- \( V_C^* \) :
-
Complementary energy along the element boundaries
- T :
-
Surface force vector on the element boundaries
- \( E \) :
-
Young’s modulus
- \( {q^e} \) :
-
Elemental nodal displacement vector
- x′ and y′:
-
Axes of material symmetry
- v i :
-
Nodal displacements belong to y
- \( N_i^0\left( {{\xi_1},{\xi_2}} \right) \) :
-
Shape function
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Rezaiee-Pajand, M., Karimipour, A. Three stress-based triangular elements. Engineering with Computers 36, 1325–1345 (2020). https://doi.org/10.1007/s00366-019-00765-6
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DOI: https://doi.org/10.1007/s00366-019-00765-6