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Suppressing Regenerative Chatter Instability by Means of Targeted ...

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ENOC 2011, 24-29 July 2011, Rome, Italy<br />

indicate quasiperiodic responses or recurrent burst-outs and suppressions <strong>of</strong> chatter instability. Typical time responses<br />

are depicted in Fig. 3, where instantaneous frequency (as wavelet transform spectra) and modal energy exchange are<br />

considered. Indeed, all the three suppression mechanisms studied in aeroelastic applications [2] can be observed, and<br />

therefore, similar interpretation <strong>of</strong> dynamics can be made.<br />

(a) (b)<br />

Figure 2. Effects <strong>of</strong> NES: (a) Shift-up <strong>of</strong> stability boundary (i.e., Hopf bifurcation point); (b) bifurcation diagram <strong>of</strong> the tool and NES<br />

displacements for 2.6 and the NES parameters 0.2, 1<br />

0.1, C 0.5 (H, LPC and NS denote Hopf, limit point cycle,<br />

Neimark-Sacker bifurcation points, respectively; DDEBIFTOOL was implemented).<br />

Figure 3. Typical responses for recurrent burst-outs and suppressions <strong>of</strong> chatter instability for the NES parameters in Fig. 2b. Zero<br />

initial conditions except for the tool displacement <strong>of</strong> 0.5 were used.<br />

Concluding Remarks<br />

<strong>Suppressing</strong> chatter instabilities <strong>by</strong> means <strong>of</strong> targeted energy transfers was studied <strong>by</strong> applying an ungrounded<br />

nonlinear energy sink to a single-DOF machine tool model with truncated regenerative nonlinearities. Three<br />

suppression mechanisms were identified, which are closely related with the topological structure <strong>of</strong> bifurcation<br />

phenomena. An example for the suppression mechanism involving recurrent burst-outs and suppressions <strong>of</strong> chatter<br />

instability was presented, where the instantaneous frequency and energy evidenced nonlinear modal interactions (i.e., a<br />

series <strong>of</strong> 1:1 transient resonance captures and escapes from resonance) between the tool and the NES.<br />

Acknowledgment<br />

This work was supported in part <strong>by</strong> National Science Foundation <strong>of</strong> United States, Grant Numbers CMMI-0928062 (YL)<br />

and CMMI-0846783 (TK).<br />

References<br />

[1] Kalmár-Nagy T., Stépán G., Moon F.C. (2001) Subcritical Hopf Bifurcation in the Delay Equation Model for Machine Tool Vibrations. Nonlinear<br />

Dynamics 26:121-142.<br />

[2] Lee Y.S., Vakakis A.F., Bergman L.A. McFarland D.M., Kerschen G. (2007) Suppression <strong>of</strong> Aeroelastic <strong>Instability</strong> <strong>by</strong> <strong>Means</strong> <strong>of</strong> Broadband Passive<br />

<strong>Targeted</strong> Energy Transfers, Part I: Theory. AIAA Journal 45(3): 693-711.<br />

[3] Engelborghs K., Luzyanina T., Roose D. (2002) Numerical Bifurcation Analysis <strong>of</strong> Delay Differential Equations using DDE-BIFTOOL. ACM<br />

Transactions on Mathematical S<strong>of</strong>tware 28(1): 1-21.

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