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The hydraulic mill is consists of two main part; servo valve and hydraulic cylinder.

We will consider flow-control servo valve. The dynamics of the servo valve is \begin{equation} \label{1}\tag{1} Q_s=C_Q\pi dx\sqrt{\frac{2}{\rho}(P_s-P_1)} \end{equation} Here,

  • $Q_s$=supply flow,
  • $C_Q$=flow coefficient,
  • $\rho$=oil density,
  • $x$=servo-valve displacement,
  • $P_s$=supply pressure,
  • $P_1$=output pressure of the valve.

The equation for the flow of oil to the hydraulic cylinder, \begin{equation} \label{2}\tag{2}Q_s=a\dot{y}+\frac{V_1}{\beta}\dot{P_1} \end{equation} Here,

  • $a$=area of the cylinder,
  • $y$=hydraulic piston displacement,
  • $V_1$=volume of the primary side of the cylinder,
  • $\beta$=bulk modulus of the oil,
  • $P_1$=cylinder pressure on primary side.

Schematic: Hydraulic servo system

Equation \eqref{1} needs to be linearized for both input-flow & output-flow to the cylinder according to valve displacement $x$.

Help me find the ODE for rate of change in cylinder Pressure $\dot{P_1}$ and $\dot{P_2}$.

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1 Answer 1

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Assuming an operating point at $x_0,P_{s_0},P_{1_0}$ we have

regarding $K_0x\sqrt{P_s-P_1}$

$$ K_0 x \sqrt{P_s-P_1} = K_0 x_0\sqrt{P_{s_0}-P_{1_0}}+K_0\sqrt{P_{s_0}-P_{1_0}} (x-x_0)-\frac{K_0 x_0 (P_1-P_{1_0})}{2 \sqrt{P_{s_0}-P_{1_0}}}+\frac{K_0 x_0 (P_s-P_{s_0})}{2 \sqrt{P_{s_0}-P_{1_0}}}+O_1(|x-x_0|^2)+O_2(|P_s-P_{s_0}|^2)+O_3(|P_1-P_{1_0}|^2) $$

so near the operating point we have

$$ a\dot{y}+\frac{V_1}{\beta}\dot{P_1} = K_0 x_0\sqrt{P_{s_0}-P_{1_0}}+K_0\sqrt{P_{s_0}-P_{1_0}} (x-x_0)-\frac{K_0 x_0 (P_1-P_{1_0})}{2 \sqrt{P_{s_0}-P_{1_0}}}+\frac{K_0 x_0 (P_s-P_{s_0})}{2 \sqrt{P_{s_0}-P_{1_0}}} $$

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