3. Relating Stress to Strain Using Matrices
Overview of the Stiffness Matrix in Cubic Systems
In a general system, there can be up to 36 potential independent terms in the stiffness matrix.
For a cubic system, symmetry reduces this to 3 independent terms.
This is seen in the stiffness matrix notation:
cij = c11 for the first three diagonal terms (c11, c22, c33)
Last three diagonal terms (c44, c55, c66) are equal to each other.
Off-diagonal terms (c12, c13, c23) also have specific relationships.
All terms not mentioned in this specific case are equal to zero.
Understanding Stress and Strain
Stress (σ) components:
Axial stress: σ1, σ2, σ3 (corresponding to x, y, z directions)
Shear stress: σ4, σ5, σ6
Strain (ε) components:
Axial strain: ε1, ε2, ε3
Shear strain: ε4, ε5, ε6
Relationship of stress to strain in cubic systems:
σ1 = c11ε1 + c12ε2 + c12ε3; showing interdependence between axial strains due to Poisson’s ratio effects.
Off-axis strains influence axial stresses, while shear terms do not affect axial stresses; shear terms operate independently.
Symmetry in a Cubic System
Each direction (x, y, z) is equivalent in a cubic crystal structure, leading to the following equivalences:
c11 = c22 = c33
c12 = c13 = c23
In low symmetry systems (e.g., triclinic), the matrix terms can be independent, but the relationships (like c12 = c21) hold based on thermodynamic principles.
Generally, cubic systems simplify the analysis due to their symmetry, making calculations manageable with linear algebra.
Compliance Matrix for Cubic Systems
The relation for compliance is given by:
εi = sijσj
Where sij represents the compliance matrix.
For cubic systems, simplifications yield:
Diagonal terms in sij: s11 for axial terms, s44 for shear terms.
Off-diagonal terms also defined, but many terms are 0 in this symmetry context.
Compliance terms are similarly reduced with independence reflecting symmetry: 21 independent terms for triclinic vs. 3 for cubic.
Stress and Strain in Different Orientations
Stress matrix is defined as applied load intensifies:
Helps describe a material’s elastic response under stress, typically assuming reversibility (the material returns to original shape upon load removal).
Defined principal directions for properties (cij, sij) are typically 100, 010, 001 for cubic but can analyze other orientations as well.
Process for analysis involves:
Begin with load in the defined single crystal direction (e.g., 111).
Convert stress tensor from original coordinates to the indexed coordinates where material properties are defined using rotation matrices.
Analyze stress in the primed coordinate system with cijs and sijs, followed by deriving strain.
Possibly convert strain back via tensor transformation to relate to the original coordinates for final analysis.
This stepwise tensor transformation helps manage complexity as it avoids unnecessary complications related to an 81-term matrix.