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@@ -80,7 +80,7 @@ partial model Power2Torque "Converts a power signal to a torque in the rotationa
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Modelica.Mechanics.Rotational.Components.IdealGear toSysSpeed(ratio=2/p) "Converts to system speed based on p = 2"annotation (Placement(transformation(extent={{24,-6},{36,6}})));
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Modelica.Blocks.Sources.RealExpression nominalSpeed(y=w_0*p/2) if enable_nomSpeed annotation (Placement(transformation(extent={{-12,-70},{8,-50}})));
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Modelica.Blocks.Interfaces.RealInput w_in if enable_w_in andnot enable_nomSpeed
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"Angular velocity input of the aggregate [pu]"annotation (Placement(transformation(
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"Angular velocity input of the unit [pu]"annotation (Placement(transformation(
Copy file name to clipboardExpand all lines: OpenHPL/Resources/Documents/UsersGuide_src/UsersGuide.tex
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@@ -917,7 +917,7 @@ \subsection{Pelton}
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\subsection{Simple Generator}
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Here, a simple model of an ideal generator with friction is considered. This model has inputs as electric power available on the grid and the turbine shaft power. This model is based on the angular momentum balance which depends on the turbine shaft power, the friction loss in the aggregate rotation, and the power taken up by the generator. The rotor angular velocity mainly depends on its inertia, internal friction and available power. The kinetic energy stored in the rotating generator is $ K_a=\frac{1}{2}J_a\omega_a^2$, where $\omega_a$ is the angular velocity of the rotor and $J_a$ is its moment of inertia. The kinetic energy $K_a$ is changed by the power terms operating on the generator axis, e.g., the turbine shaft power $\dot{W}_s$ produced by the turbine, friction power $\dot{W}_{f,a}$, and the power taken up by the generator, $\dot{W}_g$, \cite{LieL:18}, and from energy the balance can be expressed as follows:
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Here, a simple model of an ideal generator with friction is considered. This model has inputs as electric power available on the grid and the turbine shaft power. This model is based on the angular momentum balance which depends on the turbine shaft power, the friction loss in the unit rotation, and the power taken up by the generator. The rotor angular velocity mainly depends on its inertia, internal friction and available power. The kinetic energy stored in the rotating generator is $ K_a=\frac{1}{2}J_a\omega_a^2$, where $\omega_a$ is the angular velocity of the rotor and $J_a$ is its moment of inertia. The kinetic energy $K_a$ is changed by the power terms operating on the generator axis, e.g., the turbine shaft power $\dot{W}_s$ produced by the turbine, friction power $\dot{W}_{f,a}$, and the power taken up by the generator, $\dot{W}_g$, \cite{LieL:18}, and from energy the balance can be expressed as follows:
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