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Description |
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The BISTOP function models a gap element. It can be used to model forces acting on a body while moving in the gap between two boundary surfaces, which act as elastic bumpers. The properties of the two boundary surfaces can be tuned as desired. |
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Example |
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<Force_Vector_TwoBody id = "30101" type = "ForceOnly" i_marker_id = "30102031" j_floating_marker_id = "30101031" ref_marker_id = "30101010" fx_expression = BISTOP(DX(30102030,30101010,30101010),VX30102030,30101010,30101010),0.5,9.5,10000000,2.1,1,0.001)" fy_expression = "0" fz_expression = "0" /> |
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Arguments |
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The expression used for the independent variable. For example, to use the z-displacement of I marker with respect to J marker as resolved in the reference frame of RM marker as the independent variable, specify as DZ({marker_i.idstring}, {marker_j.idstring}, {marker_rm.idstring}). |
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The time derivative of the independent variable. For example, if is specified as above, then will be |
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The lower bound of . If is less than , the bistop function returns a positive value. The value of must be less than the value of . |
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The upper bound of . If is greater than , the bistop function returns a negative value. The value of must be greater than the value of . |
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The stiffness of the boundary surface interaction. It must be non-negative. |
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The exponent of the force deformation characteristic. For a stiffening spring characteristic, must be greater than 1.0 and for a softening spring characteristic, must be less than 1.0. It must always be positive. |
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The maximum damping coefficient. It must be non-negative. |
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The penetration at which the full damping coefficient is applied. It must be positive. |
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Definition |
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See Also: