Find a set of state-variable equations and develop the input–output differential equation relating the output pressure P_{3r} to the input pressure P_{s} for the fluid system shown in Fig. 9.9.
Find a set of state-variable equations and develop the input–output differential equation relating the output pressure P_{3r} to the input pressure P_{s} for the fluid system shown in Fig. 9.9.
The elemental equations are as follows: For the fluid resistor,
P_{12} =R_{f} Q_{R} . (9.13)
For the inertor,
P_{23} =I\frac{dQ_{R} }{dt} . (9.14)
For the fluid capacitor,
Q_{R} =C_{f} \frac{dP_{3r} }{dt} . (9.15)
Continuity is satisfied by use of Q_{R} for Q_{I} and Q_{c}. To satisfy compatibility.
P_{s} =P_{1r} =P_{12}+P_{23}+P_{3r}. (9.16)
Combining Eqs. (9.13), (9.14), and (9.16) to eliminate P_{12} and P_{23} yields
I\frac{dQ_{R} }{dt} =P_{s} -R_{f} Q_{R}-P_{3r}. (9.17)
Rearranging Eq. (9.17) yields the first state-variable equation:
\frac{dQ_{R} }{dt} =-\frac{R_{f} }{I} Q_{R}-\frac{1}{I} P_{3r} +\frac{1}{I} P_{s}. (9.18)
Rearranging Eq. (9.15) yields the second state-variable equation:
\frac{dP_{3r} }{dt} =\frac{1}{C_{f} } Q_{R}. (9.19)
Combining Eqs. (9.18) and (9.19) to eliminate Q_{R} and multiplying all terms by I yields the input–output system differential equation:
C_{f} I\frac{d^{2}P_{3r} }{dt^{2} } +R_{f}C_{f}\frac{dP_{3r} }{dt} +P_{3r}=P_{s}. (9.20)