2008 American Control Conference 2008
DOI: 10.1109/acc.2008.4587122
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Motion planning and tracking for tip displacement and deflection angle for flexible beams

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Cited by 6 publications
(9 citation statements)
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“…Setting ξ = 0 in (53), multiplying (53) by ε 2 (0), and using the facts that K vv (x, 0) = 0 for all x ∈ [0, 1] (see relation (31) in [34]) and that f is defined by 24, we get that f satisfies (51) for q = 0. The rest of the proof is similar to the case q = 0.…”
Section: Remarkmentioning
confidence: 99%
See 1 more Smart Citation
“…Setting ξ = 0 in (53), multiplying (53) by ε 2 (0), and using the facts that K vv (x, 0) = 0 for all x ∈ [0, 1] (see relation (31) in [34]) and that f is defined by 24, we get that f satisfies (51) for q = 0. The rest of the proof is similar to the case q = 0.…”
Section: Remarkmentioning
confidence: 99%
“…Our approach is different than the one in [34], in that we use backstepping for trajectory generation rather than stabilization, and the one in [26], in that we employ a different conceptual idea to a different class of systems. The idea of the backstepping-based trajectory generation for PDEs, which was conceived in [23], is applied to a beam PDE in [31] and the Navier-Stokes equations in [4], and is recently extended to general n × n linear hyperbolic systems in [22]. We apply this methodology to a wave PDE with indefinite in-domain and boundary damping by transforming (see, for example, [3]) the wave PDE to a 2 × 2 linear hyperbolic system coupled with a first-order ODE (Section 2.2).…”
Section: Introductionmentioning
confidence: 99%
“…(6), (7), and (4), respectively (to be exact, Àq :f(u(0,t), c 1 : c 0 and c 2 : c 1 ). When f is constant, the closedloop system (45), (46), and (49) is equivalent to the exponentially stable target system [27][28][29][30][31][32][33][34]…”
Section: Application To a String Pdementioning
confidence: 99%
“…We then turn our attention to some relevant basic mechanical PDE systems-the string and shear beam PDEs with Kelvin-nonlinearities. These designs are the extensions of results for the string [27][28][29][30] and shear beam [29][30][31][32]. The merits of these designs are highlighted by simulation.…”
Section: Introductionmentioning
confidence: 97%
“…More recently, a number of control techniques have emerged which use Lyapunov-based approaches to derive controllers for PDEs directly, without resorting to finite order approximations of the PDE [5], [6], [7], [10], [16], [17], [18]. These methods tend to do away with some limitations of the ODE-based approach, such as the occasional necessity for large order approximations, and the risk of spillover instabilities.…”
Section: Introductionmentioning
confidence: 99%