Wheel shimmy suppression through the piecewise nonlinear energy sink: elimination of detrimental isolas - presented by Prof. Giuseppe Habib

Wheel shimmy suppression through the piecewise nonlinear energy sink: elimination of detrimental isolas

Prof. Giuseppe Habib

Prof. Giuseppe Habib
Slide at 07:56
NODYCON 2025
The Proposed Method: P-NES
The feasible parameter domains of P-NES
0.015
0.08
0.02
Conclusion
0.07
Case I
[rad]
0.01
0.06
The upper damping, 2,2, should
-0.02
acr [m]
0.05
preferably be taken as a larger value.
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Fourth International Nonlinear Dynamics Conference
0.04
0.05
0.005
Within the feasible domain (blue region),
Case 2
0 [rad]
0.03
the wheel's rotation angle exhibits a
-0.05
0.02
strongly modulated response, while
t [s]
A2 [Ns/m]
outside this region, the response
The domain of upper damping
Time histories of two cases
disappears.
0.02
0.02
The lower damping, A_1, can range from
0.07
0.07
zero to the maximum damping value of
0.015
0.06
0.015
0.06
the C-NES.
0.05
acr [m]
0.01
0.04
acr [m]
0.05
0.01
A1 31.2
The feasible stiffness domain of the P-
(A₀ 0.03)
0.03
Knes 0.6 107
0.04
0.005
(Ae 0.03)
NES is almost identical to that of the C-
0.02
0.005
0.03
0.01
NES.
0.02
X₁ [Ns/m]
Kₙₑₛ [N/m]
x10⁷
The domain of lower damping
The domain of NES stiffness
6/18/2025
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Summary (AI generated)

The verification diagram for the P-NES and C-NES systems is presented. The P-NES system lacks a high-amplitude branch, which is characteristic of systems utilizing the C-NES. The critical value is significant in determining the performance of the P-NES system, as its stiffness fundamentally influences its effectiveness. Similar to the C-NES, when the shimmy is sustained, the system exhibits a robust veridical response. Consequently, the P-NES effectively mitigates the high-amplitude branch found in C-NES systems. Furthermore, the P-NES outperforms the C-NES in low damping scenarios, where the latter proves to be ineffective.

We also examine the feasible parameter domain of the TNS. It is preferable for the upper lambda 2 to be a large value. Within the feasible domain, the wheel rotational angle shows a strong correlation with the response. However, outside this region, the response diminishes. In low damping conditions, lambda 1 can vary from 0 to the maximum damping value of the C-NES. This indicates a significantly larger range. Notably, the feasible stiffness domain of the P-NES closely resembles that of the C-NES.