Download Simplicity 1695079 Technical information
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In terms of a cylindrical coordinate system ( r , θ , z ), with z as the axis of material symmetry, and assuming an axially symmetric deformation field (i.e., ε zθ = ε rθ = 0 ), the constitutive law becomes: ε r = a11 ⋅ σ r + a12 ⋅ σ θ + a13 ⋅ σ z ................................................................... (5.1.2a) ε θ = a12 ⋅ σ r + a11 ⋅ σ θ + a13 ⋅ σ z ................................................................... (5.1.2b) ε z = a13 ⋅ σ r + a13 ⋅ σ θ + a33 ⋅ σ z ................................................................... (5.1.2c) ε rz = (a 44 / 2) ⋅ τ rz .......................................................................................... (5.1.2d) in which a11 = 1 / E x , a33 = 1 / E z , a12 = −ν xy / E x , a13 = −ν zx / E z and a44 = 1 / Gxz . Hence, five elastic constants are included, namely: two Young’s moduli E x (= E y ) and E z ; two Poisson’s ratios ν xy (= ν yx ) and ν zx (= ν xz ⋅ E z / E x ) ; and one shear modulus G xz (= G yz ) . The condition that the strain energy must be positive imposes the following property restrictions (PRs) on the values of the elastic constants (e.g., Poulus and Davis, 1974): (PR1) E x , E z , G xz > 0 ; (PR2) 1 −ν xy − 2 ⋅ν xz ⋅ν zx > 0 ; and (PR3) 1 − ν xy > 0 . Following Lekhnitskii (1963) and Singh (1986), the stresses ( σ r , σ θ , σ z ,τ rz ) and displacements ( u, w in the r, z directions respectively) can be derived from a stress function φ (r , z ) as follows: σr = − ∂ ⎛ ∂φ 2 b ∂φ ∂φ 2 ⎜⎜ 2 + ⋅ +a⋅ 2 r ∂r ∂z ⎝ ∂r ∂z ⎞ ⎟⎟ ............................................................. (5.1.3a) ⎠ ∂ ⎛ ∂φ 2 1 ∂φ ∂φ 2 ⎜ σθ = − ⎜b ⋅ 2 + ⋅ +a⋅ 2 r ∂r ∂z ⎝ ∂r ∂z σz = τ rz ∂ ⎛ ∂φ 2 c ∂φ ∂φ 2 ⎜⎜ c ⋅ 2 + ⋅ +d⋅ 2 r ∂r ∂z ⎝ ∂r ∂z ∂ ⎛ ∂φ 2 1 ∂φ ∂φ 2 ⎜ = ⎜ 2 + ⋅ +a⋅ 2 r ∂r ∂r ⎝ ∂r ∂z ⎞ ⎟⎟ ......................................................... (5.1.3b) ⎠ ⎞ ⎟⎟ ............................................................ (5.1.3c) ⎠ ⎞ ⎟⎟ ................................................................ (5.1.3d) ⎠ 5-2