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Lecture Notes in Control and Information Sciences
DOI: 10.1007/3-540-45606-6_1
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Controlling an Inverted Pendulum with Bounded Controls

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Cited by 14 publications
(18 citation statements)
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“…where ϕ 1 is the angle of the arm (ϕ 1 = 0 at the upright position), ϕ 2 is the angular velocity of the arm, ϕ 3 is the angular velocity of the disk with respect to arm, u is the control input (voltage applied to the motor), and q 1 , q 2 , q 3 and ρ > 0 are constant coefficients, derived from physical parameters [21]. Here, we note that the disk position is not considered as a stable variable, because it is irrelevant for the stabilization of the pendulum in the inverted position.…”
Section: Problem Formulationmentioning
confidence: 99%
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“…where ϕ 1 is the angle of the arm (ϕ 1 = 0 at the upright position), ϕ 2 is the angular velocity of the arm, ϕ 3 is the angular velocity of the disk with respect to arm, u is the control input (voltage applied to the motor), and q 1 , q 2 , q 3 and ρ > 0 are constant coefficients, derived from physical parameters [21]. Here, we note that the disk position is not considered as a stable variable, because it is irrelevant for the stabilization of the pendulum in the inverted position.…”
Section: Problem Formulationmentioning
confidence: 99%
“…when the disk velocity is zero. Thus, according to [21], we consider an auxiliary control in the form:…”
Section: Problem Formulationmentioning
confidence: 99%
“…Other more complex control strategies reveal the great interest of the inverted pendulum in the field of control, as it is the case of control strategies based on space-state methods [9][10][11], control stabilization around homoclinic orbits [12], energy methods [13], passivity control [14] and bounded control [15] among others. However, the use of a simple control law to obtain chaotic behavior has been less used.…”
Section: Introductionmentioning
confidence: 99%
“…1 shows the layout of the pendulum system as well as the notation used to deduce the Lagrangian of the system. The pendulum is modeled by a mass m hanging at the end of a rod of negligible mass and length l, which is fixed to a support O [4][5][6], [7][8][9][10][11][12][13][14][15][16]. Let O'XY be an inertial frame and …”
Section: Introductionmentioning
confidence: 99%
“…Alonso et al [Alonso et al, 2005] used the bifurcation theory to classify different dynamical behaviors arising in the IWIP sub-20 ject to bounded continuous state feedback control law. To limit the maximum amplitude of the control action, the control law is subject to a smooth saturation function, which was first introduced in [Alonso et al, 2002] in order to stabilize the IWIP at the inverted position. The authors showed that the global dynamics of the IWIP change from a stable equilibrium point to a stable limit cycle via a Hopf bifurcation as certain control gains change.…”
mentioning
confidence: 99%