T1-23
8.0 3-D OBJECT DRIVEN BY VIBRATORY FORCE AND TORQUES
Figure 37 shows an object with its C.G. at C, mounted on 4 flexible mounts and acted upon by a disturbing harmonic
force Fy in the y-direction (vertical) and/or by torques, Tx, Ty and Tz acting singly or in combination about the x, y and z axes,
which are principal inertia axes passing through the C.G. (point C).
The four mounts are symmetrically disposed relative to the C.G., their location defined by distances b
x
, b
y
and b
z
from
the axes, as shown. The mass moments of inertia about the principal inertia axes are I
x
, I
y
and I
z
, respectively. As a result of
the external force and torques, the object motion is (a) a displacement of C.G., maximum values of which are denoted by
translational motions of the C.G. (x, y, z) and (b) rotations of the object (from equilibrium) about the coordinate axes (q
x
, q
y,
qz). These displacements are generally small relative to the major dimensions of the object.
Let:
M
=
mass of object (W/g where W is weight of the object, g = 386 in/sec
2
= 9.8 m/sec
2
);
ky
=
total vertical stiffness of the four supports in lb./in. or N/m; i.e., 4 times the stiffness of each support
if all four supports are identical
ks
=
total horizontal or shear stiffness of the four supports; i.e., 4 times the horizontal stiffness of each
support, if all supports are identical and for each support k
x
= k
z
= k
s
, lb./in. or N/m;
3
=
angular frequency of sinusoidally applied force and torques (rad/sec)
Damping is assumed to be negligible.
8.1 Displacement of the Object
Due to F
y
only:
y = (31)
Due to T
z
only:
x = (32)
qz = (33)
C
x
y
Fy
Tx
Tz
bz
by
bx
q
z
q
x
ky/4
ky/4
ky/4
ky/4
Ty
C
(x, y, z)
y
z
C
z
x
q
y
Fy
________
ky M32
Tzbyks
_____________________________________
IzM34
32
(Izks
+
kybx2
M + ksby2 M) + kyksbx2
Tz(ks M32)
_____________________________________
IzM34
32
(Izks
+
kybx2
M + ksby2 M) + kyksbx2
Figure 37 Solid Body on Vibration Isolators