132 Chapter 4 / Mathematical Modeling of Fluid Systems and Thermal Systems
+–
(a) (b) (c)
q R
P 2 P 1
A
k
y
y
z
z
t
t
Y(s) Z(s)
1
Ts
T=RA
(^2) r
k
The transfer function between yandebecomes a constant. Thus, the hydraulic controller
shown in Figure 4–20(a) acts as a proportional controller, the gain of which is Kp. This gain
can be adjusted by effectively changing the lever ratio b/a. (The adjusting mechanism is
not shown in the diagram.)
We have thus seen that the addition of a feedback link will cause the hydraulic
servomotor to act as a proportional controller.
Dashpots. The dashpot (also called a damper) shown in Figure 4–21(a) acts as a
differentiating element. Suppose that we introduce a step displacement to the piston po-
sitiony. Then the displacement zbecomes equal to ymomentarily. Because of the spring
force, however, the oil will flow through the resistance Rand the cylinder will come back
to the original position. The curves yversustandzversustare shown in Figure 4–21(b).
Let us derive the transfer function between the displacement zand displacement y.
Define the pressures existing on the right and left sides of the piston as and
respectively. Suppose that the inertia force involved is negligible. Then the
force acting on the piston must balance the spring force. Thus
whereA=piston area, in.^2
k=spring constant, lbfin.
The flow rate qis given by
where q=flow rate through the restriction, lbsec
R=resistance to flow at the restriction, lbf-secin.^2 -lb
Since the flow through the restriction during dtseconds must equal the change in the
mass of oil to the left of the piston during the same dtseconds, we obtain
wherer=density, lbin.^3. (We assume that the fluid is incompressible or r=constant.)
This last equation can be rewritten as
dy
dt
-
dz
dt
=
q
Ar
=
P 1 - P 2
RAr
=
kz
RA^2 r
qdt=Ar(dy-dz)
q=
P 1 - P 2
R
AAP 1 - P 2 B=kz
P 2 (lbfin.^2 ),
P 1 (lbfin.^2 )
Figure 4–21
(a) Dashpot; (b) step change in yand the corresponding change in zplotted versus t; (c) block
diagram of the dashpot.
Openmirrors.com