Advanced Solid Mechanics Assignment - 4: Balance Laws 1. Determine which of the following Cauchy stress fields are possible within a body at rest assuming that there are no body forces acting on it: 3 2 2 xy 3 0 −2x y − 41 y 4 0 , (a) σ = xy 3 0 0 0 3yz z 2 5y 2 (b) σ = z 2 7xz 2x2 , 5y 2 2x2 9xy 3x + 5y 7x − 3y 0 (c) σ = 7x − 3y 2x − 7y 0 , 0 0 0 3x −3y 0 (d) σ = −7x 7y 0 , 0 0 0 7x −3x 0 (e) σ = 7y 3y 0 , 0 0 0 where the components of the stress are with respect to orthonormal Cartesian basis and (x, y, z) denote the Cartesian coordinates of a typical material particle in the current configuration of the body. 2. The Cartesian components of the Cauchy stress tensor in a plate at rest is −2x2 −7 + 4xy + z 1 + x − 3y . 0 σ = −7 + 4xy + z 3x2 − 2y 2 + 5z 1 + x − 3y 0 −5 + x + 3y + 3z 1 Find the body force that should act on the plate so that this state of stress is realizable in the body. 3. A body at rest is subjected to a plane state of stress such that the non-zero Cartesian components of the Cauchy stress are σxx , σxz and σzz . Derive the equilibrium equations for this special case. Then, show that in the absence of body forces the equilibrium equations hold if, σxx = ∂ 2φ , ∂z 2 σxz = − ∂ 2φ , ∂x∂z σzz = ∂ 2φ , ∂x2 where φ = φ̄(x, y), for any choice of φ. φ is called the Airy’s stress potential. 4. Derive form first principles and show that for the plane stress problem in cylindrical polar coordinates with the non-zero cylindrical polar components of the Cauchy stress being σrr , σrθ and σθθ , as shown in figure ??, the equilibrium equations in the absence of body forces with the body in static equilibrium are ∂σrr 1 ∂σθr σrr − σθθ + + = 0, ∂r r ∂θ r ∂σrθ 1 ∂σθθ 2σrθ + + = 0. ∂r r ∂θ r 5. Is any stress field that satisfies the equilibrium equations realizable in a given body? Discuss. 2 ࣔ࣌࢘࢘ ο࢘ ࣔ࢘ ࣔ࣌ࣂ࢘ ࣌ࣂ࢘ ο࢘ ࣔ࢘ ࢋ࢘ ࣌ ࣌࢘࢘ ࣌ࣂࣂ ࣌࢘ࣂ ࣔ࣌ࣂࣂ οࣂ ࣔࣂ ࣔ࣌࢘ࣂ οࣂ ࣔࣂ ࣌ࣂ࢘ dr ࢋࢠ ࢋࣂ ࣌࢘࢘ ࣌࢘ࣂ dθ r ࣌ࣂࣂ dz Figure 1: Figure for problem 4. Variation of the cylindrical polar components of the Cauchy stress over an infinitesimal cylindrical wedge, in plane stress state 3
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