Section 3–2 / Mathematical Modeling of Mechanical Systems 65
(a) The force fdue to the dampers is
In terms of the equivalent viscous-friction coefficient beq, force fis given by
Hence
(b) The force fdue to the dampers is
(3–1)
wherezis the displacement of a point between damper b 1 and damper b 2 .(Note that the
same force is transmitted through the shaft.) From Equation (3–1), we have
or
(3–2)
In terms of the equivalent viscous-friction coefficient beq,forcefis given by
By substituting Equation (3–2) into Equation (3–1), we have
Thus,
Hence,
beq=
b 1 b 2
b 1 +b 2
=
1
1
b 1
+
1
b 2
f=beq(y# -x#)=
b 1 b 2
b 1 +b 2
(y# -x#)
=
b 1 b 2
b 1 +b 2
(y# -x#)
f =b 2 (y# -z#)=b 2 cy#-
1
b 1 +b 2
Ab 2 y# +b 1 x#Bd
f=beqAy# -x#B
z# =
1
b 1 +b 2
Ab 2 y# +b 1 x#B
Ab 1 +b 2 Bz# =b 2 y# +b 1 x#
f=b 1 (z# -x#)=b 2 (y# -z#)
beq=b 1 +b 2
f=beq(y# -x#)
f=b 1 (y# -x#)+b 2 (y# -x#)=Ab 1 +b 2 B(y# -x#)
x y
(a)
b 2
x z y
(b)
b 1
b 1
b 2
Figure 3–2
(a) Two dampers
connected in parallel;
(b) two dampers
connected in series.