************************************* **Upper Velocity Function Constants** ************************************* :: Upper Velocity Function Constants = {model_name} ----------------------- **Description / Usage** ----------------------- This card takes the specification of the upper-wall velocity function for the confined channel lubrication capability, or the lub_p equation. This function specifies the velocity of the upper channel wall as a function of time. Currently two models for {model_name} are permissible: +--------------------------+-------------------------------------------------------------------------------------+ |**CONSTANT** |This model invokes a squeeze/separation velocity uniformly across the entire material| | |region, viz. the two walls are brought together/apart at a constant rate. This option| | |requires two floating point values | | | | | | * is the velocity component in the x-direction. L/t. | | | * is the velocity component in the y-direction. L/t | | | * is the velocity component in the z-direction. L/t (NOTE: this is usually | | | taken as zero as it is set in the Upper Wall Height Function model) | +--------------------------+-------------------------------------------------------------------------------------+ |**ROLL** |This model invokes a wall velocity which corresponds to a rolling-motion. This model | | |takes nine constants ???? : | | | | | | * Roll radius, L. | | | * x-coordinate of axis origin, L. | | | * y-coordinate of axis orgin, L. | | | * z-coordinate of axis origin, L. | | | * Direction angle 1 of rotation axis | | | * Direction angle 2of rotation axis | | | * Direction angle 3of rotation axis | | | * Squeeze rate | | | * rotation rate | +--------------------------+-------------------------------------------------------------------------------------+ |**TANGENTIAL_ROTATE** |his model allows a velocity that is always tangential to a shell surface, not | | |necessarily aligned along the coordinate directions. It requires three | | |specifications. First, a vector (v) that is always non-colinear to the normal vector | | |of the shell must be specified. This is used to make unique tangent vectors. The last| | |two specifications are the two tangential components to the velocity. The first | | |velocity is applied in the direction of t1 = v×n. The second velocity is then applied| | |in the t = t ×n direction. | | | | | | * vx | | | * vy | | | * vz | | | * velocity in the t1 direction | | | * velocity in the t2 direction | +--------------------------+-------------------------------------------------------------------------------------+ |**CIRCLE_MELT** |Model which allows a converging or diverging height that is like a circle. Also works| | |for melting. | | | | | | * - x-location of the circle center (circle is in x-y plane) | | | * - radius of circle | | | * - minimum height of circle | +--------------------------+-------------------------------------------------------------------------------------+ ------------ **Examples** ------------ Following is a sample card: :: Upper Velocity Function Constants = CONSTANT {v_x= -0.001} {vy=0.00} {vz=0} This card results in an upper wall speed of -0.001 in the x-direction which is tangential to the substrate, thus generating a Couette component to the flow field. ------------------------- **Technical Discussion** ------------------------- For non-curved shell meshes, most of the time they are oriented with the x-, y-, or zplane. This card is aimed at applying a tangential motion to that plane, and so one of the three components is usually zero.