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Copy file name to clipboardExpand all lines: src/PlanarMechanics/components.jl
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@@ -568,13 +568,18 @@ The force depends with friction characteristics on the slip. The slip is split i
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- lateral slip: the lateral velocity divided by the rolling velocity.
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- longitudinal slip: the longitudinal slip velocity divided by the rolling velocity.
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For low rolling velocity this definition become ill-conditioned. Hence a dry-friction model is used for low rolling velocities. For zero rolling velocity, the intitialization might fail if automatic differentiation is used. Either start with a non-zero (but tiny) rolling velocity or pass `autodiff=false` to the solver.
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For low rolling velocity this definition become ill-conditioned. Hence a dry-friction model is used for low rolling velocities. For **zero rolling velocity**, the intitialization might fail if automatic differentiation is used. Either start with a non-zero (but tiny) rolling velocity or pass `autodiff=false` to the solver.
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The radius of the wheel can be specified by the parameter `radius`. The driving direction (for `phi = 0`) can be specified by the parameter `r`. The normal load is set by `N`.
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The wheel contains a 2D connector `frame_a` for the steering on the plane. The rolling motion of the wheel can be actuated by the 1D connector `flange_a`.
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In addition there is an input `dynamicLoad` for a dynamic component of the normal load.
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# Connectors:
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- `frame_a` (Frame) Coordinate system fixed to the component with one cut-force and cut-torque
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- `flange_a` (Rotational.Flange) Flange for the rolling motion
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- `dynamicLoad` (Blocks.RealInput) Input for the dynamic component of the normal load (must be connected)
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