Description of snooker simulation

Analyze a single snooker shoot as depicted under the following assumptions:

2D problem

plane strain condition and hyperelastic material

4 node element

Newmark's time integration

2D smooth deformable-deformable contact with Coulomb friction

augmented Lagrange multipliers method

Example has been contributed by Jakub Lengiewicz, Institute of Fundamental Technological Research, Warszawa, Poland.

Out[525]=

Graphics:None

Hypersolid dynamic element

"Snooker1_2.gif"

Generate two-dimensional, four node finite element for the analysis of the steady state problems in the mechanics of solids. The element has the following characteristics:
⇒    quadrilateral topology,
⇒    4 node element,
⇒    isoparametric mapping from the reference to the actual frame,

⇒    global unknowns are displacements of the nodes,
⇒    the element should allow arbitrary large displacements and rotations,
⇒    the problem is defined by the hyperelastic Neo-Hooke type strain energy potential,
    "Snooker1_3.gif",
    where "Snooker1_4.gif" is right Cauchy-Green tensor, F=I+u  is deformation gradient,
    u is displacements field, Q is prescribed body force, t is prescribed surface traction,
    "Snooker1_5.gif" is the initial domain of the problem and λ, μ are the first and the second Lame's material constants.
    
⇒    The Newmark's time integration
    "Snooker1_6.gif"="Snooker1_7.gif" + (1-"Snooker1_8.gif") dt "Snooker1_9.gif" ,
    "Snooker1_10.gif"="Snooker1_11.gif" - ("Snooker1_12.gif"-1) dt "Snooker1_13.gif" ,
    β , γ ...Newmark's - constants
    
The following user subroutines have to be generated:
⇒    user subroutine for the direct implicit analysis,
⇒    user subroutine for the  post-processing that returns the Green-Lagrange strain tensor and
    the Cauchy stress tensor.

Smooth master segment contact element

"Snooker1_14.gif"

Node-to-segment smooth element for analysis of the 2-D contact problems has the following characteristics:
⇒    8 node element: one slave node + two dummy slave nodes (referential area) + four master nodes (3rd order Bezier curve) + lagrange multipliers node,
⇒    global unknowns are displacements of the nodes + lagrange multipliers,
⇒    the element should allow arbitrary large displacements,
⇒    the impenetrability condition is regularized with augmented lagrange multipliers method and formulated as energy potential (for each node on slave contact surface):
        "Snooker1_15.gif"
    where:
        "Snooker1_16.gif"
    and
        "Snooker1_17.gif"
    and
        "Snooker1_18.gif"

     and ρ is regularisation parameter, "Snooker1_19.gif" is normal gap (at the point of orthogonal projection of slave point on master boundary), "Snooker1_20.gif" is tangential slip.
     "Snooker1_21.gif" and "Snooker1_22.gif" are lagrange multipliers and have a meaning of normal and tangential nominal pressure respectively.

The following user subroutines have to be generated:
⇒    user subroutine for specification of  nodal positions,
⇒    user subroutine for the direct implicit analysis,


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