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refs modelica#3661: Add alternative Clutch model based on CombiTable1Ds
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within Modelica.Mechanics.Rotational.Components; | ||
model Clutch2 "Clutch based on Coulomb friction (with interpolation based on CombiTable1Ds)" | ||
extends Modelica.Mechanics.Rotational.Icons.Clutch; | ||
extends Modelica.Mechanics.Rotational.Interfaces.PartialCompliantWithRelativeStates; | ||
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parameter Real mu_pos[:, 2] = [0, 0.5] | ||
"Positive sliding friction coefficient [-] as function of w_rel [rad/s] (w_rel>=0)"; | ||
parameter Real peak(final min=1) = 1 | ||
"Peak for maximum value of mu at w==0 (mu0_max = peak*mu_pos[1,2])"; | ||
parameter Real cgeo(final min=0) = 1 | ||
"Geometry constant containing friction distribution assumption"; | ||
parameter SI.Force fn_max(final min=0, start=1) "Maximum normal force"; | ||
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extends Rotational.Interfaces.PartialFriction; | ||
extends Modelica.Thermal.HeatTransfer.Interfaces.PartialElementaryConditionalHeatPortWithoutT; | ||
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SI.Force fn "Normal force (fn=fn_max*f_normalized)"; | ||
Modelica.Blocks.Interfaces.RealInput f_normalized | ||
"Normalized force signal 0..1 (normal force = fn_max*f_normalized; clutch is engaged if > 0)" | ||
annotation (Placement(transformation(origin={0,110}, extent={{20,-20},{-20,20}}, rotation=90))); | ||
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protected | ||
final parameter Real mu0 = Modelica.Math.Vectors.interpolate(mu_pos[:,1], mu_pos[:,2], 0, 1) | ||
"Friction coefficient for w=0 and forward sliding" annotation(Evaluate = true); | ||
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Real table_signs[2] | ||
"Signs for sliding friction coefficient table interpolation: [sign for w_rel, sign for mu]"; | ||
Modelica.Blocks.Tables.CombiTable1Ds table( | ||
table=mu_pos) "Sliding friction coefficient table"; | ||
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equation | ||
// Relative quantities | ||
w_relfric = w_rel; | ||
a_relfric = a_rel; | ||
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// Normal force and friction torque for w_rel=0 | ||
fn = fn_max*f_normalized; | ||
free = fn <= 0; | ||
tau0 = mu0*cgeo*fn; | ||
tau0_max = peak*tau0; | ||
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// Friction torque | ||
table_signs = if startForward then | ||
{1,1} | ||
elseif startBackward then | ||
{1,-1} | ||
elseif pre(mode) == Forward then | ||
{1,1} | ||
else | ||
{-1,-1}; | ||
table.u = table_signs[1]*w_rel; | ||
tau = if locked then sa*unitTorque elseif free then 0 else cgeo*fn*(table_signs[2]*table.y[1]); | ||
lossPower = tau*w_relfric; | ||
annotation (defaultComponentName="clutch", Icon( | ||
coordinateSystem(preserveAspectRatio=true, | ||
extent={{-100,-100},{100,100}}), | ||
graphics={ | ||
Text(extent={{-150,-110},{150,-70}}, | ||
textString="%name", | ||
textColor={0,0,255}), | ||
Line(visible=useHeatPort, | ||
points={{-100,-100},{-100,-40},{0,-40}}, | ||
color={191,0,0}, | ||
pattern=LinePattern.Dot)}), Documentation(info="<html> | ||
<p> | ||
This component models a <strong>clutch</strong>, i.e., a component with | ||
two flanges where friction is present between the two flanges | ||
and these flanges are pressed together via a normal force. | ||
The normal force fn has to be provided as input signal f_normalized in a normalized form | ||
(0 ≤ f_normalized ≤ 1), | ||
fn = fn_max*f_normalized, where fn_max has to be provided as parameter. Friction in the | ||
clutch is modelled in the following way: | ||
</p> | ||
<p> | ||
When the relative angular velocity is not zero, the friction torque is a | ||
function of the velocity dependent friction coefficient mu(w_rel), of | ||
the normal force \"fn\", and of a geometry constant \"cgeo\" which takes into | ||
account the geometry of the device and the assumptions on the friction | ||
distributions: | ||
</p> | ||
<blockquote><pre> | ||
frictional_torque = <strong>cgeo</strong> * <strong>mu</strong>(w_rel) * <strong>fn</strong> | ||
</pre></blockquote> | ||
<p> | ||
Typical values of coefficients of friction <strong>mu</strong>: | ||
</p> | ||
<ul> | ||
<li>0.2 … 0.4 for dry operation,</li> | ||
<li>0.05 … 0.1 when operating in oil.</li> | ||
</ul> | ||
<p> | ||
When plates are pressed together, where <strong>ri</strong> is the inner radius, | ||
<strong>ro</strong> is the outer radius and <strong>N</strong> is the number of friction interfaces, | ||
the geometry constant is calculated in the following way under the | ||
assumption of a uniform rate of wear at the interfaces: | ||
</p> | ||
<blockquote><pre> | ||
<strong>cgeo</strong> = <strong>N</strong>*(<strong>r0</strong> + <strong>ri</strong>)/2 | ||
</pre></blockquote> | ||
<p> | ||
The positive part of the friction characteristic <strong>mu</strong>(w_rel), | ||
w_rel >= 0, is defined via table mu_pos (first column = w_rel, | ||
second column = mu). Currently, only linear interpolation in | ||
the table is supported. | ||
</p> | ||
<p> | ||
When the relative angular velocity becomes zero, the elements | ||
connected by the friction element become stuck, i.e., the relative | ||
angle remains constant. In this phase the friction torque is | ||
calculated from a torque balance due to the requirement, that | ||
the relative acceleration shall be zero. The elements begin | ||
to slide when the friction torque exceeds a threshold value, | ||
called the maximum static friction torque, computed via: | ||
</p> | ||
<blockquote><pre> | ||
frictional_torque = <strong>peak</strong> * <strong>cgeo</strong> * <strong>mu</strong>(w_rel=0) * <strong>fn</strong> (<strong>peak</strong> >= 1) | ||
</pre></blockquote> | ||
<p> | ||
This procedure is implemented in a \"clean\" way by state events and | ||
leads to continuous/discrete systems of equations if friction elements | ||
are dynamically coupled. The method is described in | ||
(see also a short sketch in <a href=\"modelica://Modelica.Mechanics.Rotational.UsersGuide.ModelingOfFriction\">UsersGuide.ModelingOfFriction</a>): | ||
</p> | ||
<dl> | ||
<dt>Otter M., Elmqvist H., and Mattsson S.E. (1999):</dt> | ||
<dd><strong>Hybrid Modeling in Modelica based on the Synchronous | ||
Data Flow Principle</strong>. CACSD'99, Aug. 22.-26, Hawaii.</dd> | ||
</dl> | ||
<p> | ||
More precise friction models take into account the elasticity of the | ||
material when the two elements are \"stuck\", as well as other effects, | ||
like hysteresis. This has the advantage that the friction element can | ||
be completely described by a differential equation without events. The | ||
drawback is that the system becomes stiff (about 10-20 times slower | ||
simulation) and that more material constants have to be supplied which | ||
requires more sophisticated identification. For more details, see the | ||
following references, especially (Armstrong and Canudas de Wit 1996): | ||
</p> | ||
<dl> | ||
<dt>Armstrong B. (1991):</dt> | ||
<dd><strong>Control of Machines with Friction</strong>. Kluwer Academic | ||
Press, Boston MA.<br></dd> | ||
<dt>Armstrong B., and Canudas de Wit C. (1996):</dt> | ||
<dd><strong>Friction Modeling and Compensation.</strong> | ||
The Control Handbook, edited by W.S.Levine, CRC Press, | ||
pp. 1369-1382.<br></dd> | ||
<dt>Canudas de Wit C., Olsson H., Åström K.J., and Lischinsky P. (1995):</dt> | ||
<dd><strong>A new model for control of systems with friction.</strong> | ||
IEEE Transactions on Automatic Control, Vol. 40, No. 3, pp. 419-425.</dd> | ||
</dl> | ||
<p> | ||
This model of clutch is slightly different to the | ||
<a href=\"modelica://Modelica.Mechanics.Rotational.Components.Clutch\">Clutch</a> component: | ||
</p> | ||
<ul> | ||
<li>The friction coefficient <code>mu0</code> for zero velocity is a constant parameter computed by linear interpolation.</li> | ||
<li>The table interpolation in <code>mu_pos</code> utilizes the interpolation based on <a href=\"modelica://Modelica.Blocks.Tables.CombiTable1Ds\">CombiTable1Ds</a>.</li> | ||
</ul> | ||
<p> | ||
See also the discussion | ||
<a href=\"modelica://Modelica.Mechanics.Rotational.UsersGuide.StateSelection\">State Selection</a> | ||
in the User's Guide of the Rotational library. | ||
</p> | ||
</html>")); | ||
end Clutch2; |
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Original file line number | Diff line number | Diff line change |
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|
@@ -9,6 +9,7 @@ ElastoBacklash2 | |
BearingFriction | ||
Brake | ||
Clutch | ||
Clutch2 | ||
OneWayClutch | ||
IdealGear | ||
LossyGear | ||
|
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