When both ends of an elastic continuous rotor are supported simply by double-row self-aligning ball bearings, the geometrical nonlinearity appears due to the stiffening effect in the elongation of the rotor if the movement of the bearings in the longitudinal direction is restricted. As the rotor becomes more slender, the geometrical nonlinearity becomes stronger. In this paper, we study on unique nonlinear phenomena caused by both of the nonlinear spring characteristics and an initial axial force in the vicinity of the major critical speed ωc and twice ωc in a very slender continuous rotor. When the rotor is supported horizontally, the difference in support stiffness and the asymmetrical nonlinearity appear as a result of shifting from the equilibrium position. By the influences of the internal resonance and the initial axial force, the nonlinear resonance phenomena become very complicated. For example, the peak resonance splits into two peaks, and these two peaks leave each other and then one becomes a hard spring type while the other becomes a soft spring type, respectively. Moreover, almost periodic motions and chaotic vibrations appear. In this paper, we prove the above phenomena theoretically and experimentally.

1.
Lee
,
A. C.
,
Kang
,
Y.
, and
Liu
,
S. L.
, 1993, “
Steady-State Analysis of a Rotor Mounted on Nonlinear Bearings by the Transfer Matrix Method
,”
Int. J. Mech. Sci.
0020-7403,
35
(
6
), pp.
479
490
.
2.
Ji
,
Z.
and
Zu
,
J. W.
, 1998, “
Method of Multiple Scales for Vibration Analysis of Rotor-Shaft Systems with Nonlinear Bearing Pedestal Model
,”
J. Sound Vib.
0022-460X,
218
(
2
), pp.
293
305
.
3.
Shabaneh
,
N.
, and
Zu
,
J. W.
, 2003, “
Nonlinear Dynamic Analysis of a Rotor Shaft System With Viscoelastically Supported Bearings
,”
ASME J. Vibr. Acoust.
0739-3717,
125
, pp.
290
298
.
4.
Shaw
,
J.
, and
Shaw
,
S. W.
, 1989, “
Instabilities and Bifurcations in a Rotating Shaft
,”
J. Sound Vib.
0022-460X,
132
(
2
), pp.
227
244
.
5.
Shaw
,
J.
, and
Shaw
,
S. W.
, 1991, “
Nonlinear Resonance of an Unbalanced Rotating Shaft With Internal Damping
,”
J. Sound Vib.
0022-460X,
147
(
3
), pp.
435
451
.
6.
Shaw
,
S. W.
, 1988, “
Chaotic Dynamics of a Slender Beam Rotating About Its Longitudinal Axis
,”
J. Sound Vib.
0022-460X,
124
(
2
), pp.
329
343
.
7.
Ishida
,
Y.
,
Nagasaka
,
I.
,
Inoue
,
T.
, and
Lee
,
S.
, 1996, “
Forced Oscillations of a Vertical Continuous Rotor With Geometric Nonlinearity
,”
Nonlinear Dyn.
0924-090X,
11
(
2
), pp.
107
120
.
8.
Ishida
,
Y.
,
Nagasaka
,
I.
, and
Lee
,
S.
, 1997, “
Forced Oscillations of a Continuous Rotor With Geometric Nonlinearity (Internal Resonance Phenomena at Harmonic and Subharmonic Resonances)
,”
Proceedings of the ASME DETC97
, Paper No. VIB-4697, pp.
1
15
.
9.
Ishida
,
Y.
,
Nagasaka
,
I.
, and
Lee
,
S.
, 1997, “
Forced Oscillations of a Horizontal Continuous Rotor With Geometric Nonlinearity (Internal Resonance Phenomena at Harmonic Resonances and at Subharmonic Resonances of Order 1/3)
,”
Trans. Japan Soc. Mech. Eng.
,
63
(
605
), pp.
10
15
. 0387-5024
10.
Nagasaka
,
I.
,
Ishida
,
Y.
, and
Liu
,
J.
, 2008, “
Forced Oscillations of a Continuous Asymmetrical Rotor With Geometric Nonlinearity (Major Critical Speed and Secondary Critical Speed)
,”
ASME J. Vibr. Acoust.
0739-3717,
130
(
3
), p.
031012
.
11.
Eshleman
,
R. L.
, and
Eubanks
,
R. A.
, 1969, “
On the Critical Speeds of a Continuous Rotor
,”
ASME J. Eng. Ind.
0022-0817,
91
, pp.
1180
1188
.
12.
Bolotin
,
V. V.
, 1964,
The Dynamic Stability of Elastic Systems
,
Holden-Day
,
San Francisco, CA
.
13.
Stoker
,
J. J.
, 1966,
Nonlinear Vibrations (in Mechanical and Electrical Systems)
,
Wiley
,
New York
.
14.
Yamamoto
,
T.
, and
Ishida
,
Y.
, 2001,
Linear and Nonlinear Rotordynamics
,
Wiley
,
New York
.
15.
Yamamoto
,
T.
,
Yasuda
,
K.
and
Nagasaka
,
I.
, 1976, “
Ultra-Subharmonic Oscillations in a Nonlinear Vibratory System
,”
Bull. JSME
0021-3764,
19
(
138
), pp.
1442
1447
.
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