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Subcritical Hopf Bifurcation in the Delay Equation Model for Machine ...

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134 T. Kalmár-Nagy et al.Figure 4. <strong>Bifurcation</strong> diagram.s<strong>in</strong>usoidal <strong>in</strong>itial functions of different amplitudes. The growth or decay of <strong>the</strong> solution (aftersome transient) decides whe<strong>the</strong>r <strong>the</strong> solution is ‘outside’ or ‘<strong>in</strong>side’ of <strong>the</strong> unstable limitcycle. Us<strong>in</strong>g a bisection rout<strong>in</strong>e allows <strong>the</strong> computation of <strong>the</strong> location of <strong>the</strong> unstable limitcycle with good accuracy. The bifurcation diagram (present<strong>in</strong>g <strong>the</strong> amplitude of <strong>the</strong> unstablelimit cycle vs <strong>the</strong> normalized bifurcation parameter) is shown <strong>in</strong> Figure 4, toge<strong>the</strong>r with <strong>the</strong>analytical approximation (solid l<strong>in</strong>e). The agreement is excellent.8. ConclusionsThe existence and nature of a <strong>Hopf</strong> bifurcation <strong>in</strong> <strong>the</strong> delay-differential equation <strong>for</strong> selfexcitedtool vibration is presented and proved analytically with <strong>the</strong> help of <strong>the</strong> Center Manifoldand <strong>Hopf</strong> <strong>Bifurcation</strong> Theory. The simple results are due to <strong>the</strong> special structure of <strong>the</strong> nonl<strong>in</strong>earitiesconsidered <strong>in</strong> <strong>the</strong> cutt<strong>in</strong>g <strong>for</strong>ce dependence on <strong>the</strong> chip thickness. On <strong>the</strong> o<strong>the</strong>r handthis analysis is local <strong>in</strong> <strong>the</strong> sense that it does not account <strong>for</strong> nonl<strong>in</strong>ear phenomena as <strong>the</strong> toolleaves <strong>the</strong> material. In this case <strong>the</strong> regenerative effect disappears, and <strong>the</strong> result of <strong>the</strong> localanalysis is not valid anymore [3, 9].F<strong>in</strong>ally, <strong>the</strong> semi-analytical and numerical results of Nayfeh et al. [13] show some caseswhere a slight supercritical bifurcation appears be<strong>for</strong>e <strong>the</strong> birth of <strong>the</strong> unstable limit cycle, and<strong>the</strong>y present also some robust supercritical <strong>Hopf</strong> bifurcations. These results were calculatedat critical parameter values somewhat away from <strong>the</strong> ‘notches’ of <strong>the</strong> stability chart chosen <strong>in</strong>this study. The model considered <strong>the</strong>re also conta<strong>in</strong>ed structural nonl<strong>in</strong>earities.AppendixCANONICAL FORM FOR ORDINARY AND DELAY DIFFERENTIAL EQUATIONSIn this Appendix we will show an analogy between ord<strong>in</strong>ary and delay differential equationsthus motivat<strong>in</strong>g <strong>the</strong> def<strong>in</strong>itions of <strong>the</strong> differential operator, its adjo<strong>in</strong>t and <strong>the</strong> bil<strong>in</strong>ear <strong>for</strong>mused to <strong>in</strong>vestigate <strong>Hopf</strong> bifurcation <strong>in</strong> delay equations.In particular it is shown that <strong>the</strong> time-delay problem leads to an operator that is <strong>the</strong> generalizationof <strong>the</strong> def<strong>in</strong><strong>in</strong>g matrix <strong>in</strong> a system of ODEs with constant coefficients.

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