Magnetic Bearings Theory and Applications Part 3 pot

... Control, Addison-Wesley Longman, Inc., 1998. Magnetic Bearings, Theory and Applications2 4 Figure 32 and Figure 33 show the displacement sensor output and the controller output, respectively, ... 17 and 23, 19 and 25, 21 and 27. The step and step disturbance rejection responses with the designed FLC exhibit smaller steady-state error and overshoot as shown in Figu...

Ngày tải lên: 21/06/2014, 02:20

... publication@sciyo.com Magnetic Bearings, Theory and Applications, Edited by Boštjan Polajžer p. cm. ISBN 978-9 53- 307-148-0 Magnetic Bearings, Theory and Applications4 3. System Identification 3. 1 System ... researchers and engineers in the eld. Editor Boštjan Polajžer University of Maribor, Faculty of Electrical Engineering and Computer Science Slovenia Preface...

Ngày tải lên: 20/06/2014, 06:20

... step reference and step disturbance with controllers C lead (s), C(s), C 1 (s), and C 2 (s), and the designed FLC. Magnetic Bearings, Theory and Applications1 2 Fig. 11. Magnetic bearing ... bearing system to step reference and step disturbance with controllers C lead (s), C(s), C 1 (s), and C 2 (s), and the designed FLC. Magnetic Bearings, Theory and A...

Ngày tải lên: 20/06/2014, 06:20

... pair of electromagnets in the x axis Magnetic Bearings, Theory and Applications3 0 Fig. 3. B-H characteristic for laminated ferromagnetic material 33 0 -35 -A5 The Poisson's equation ... of a pair of electromagnets in the x axis Magnetic Bearings, Theory and Applications2 4 Figure 32 and Figure 33 show the displacement sensor output and the controller o...

Ngày tải lên: 20/06/2014, 06:20

... η 41  1 √ α 41 K ∗  − 4r 4 r 1 α 41  − 1  β 41 K ∗  − 4r 4 r 1 β 41  + 1 √ δ 41 K ∗  − 4r 4 r 1 δ 41  − 1 √ γ 41 K ∗  − 4r 4 r 1 γ 41   + η 32  1 √ α 32 K ∗  − 4r 3 r 2 α 32  − 1  β 32 K ∗  − 4r 3 r 2 β 32  + 1 √ δ 32 K ∗  − 4r 3 r 2 δ 32  − 1 √ γ 32 K ∗  − 4r 3 r 2 γ 32   + η 42  1 √ α 42 K ∗  − 4r 4 r 2 α 42  − 1  β 42 K ∗  − 4r 4 r 2 β 4...

Ngày tải lên: 20/06/2014, 06:20

... pp2125-2127 John R Hull. (2000). Superconducting bearings, Supercond. Sci. Technol, Vol. 13, pp.1-5 Magnetic Bearings, Theory and Applications1 30 Fig. 21. Result of the rotation using the ... a moved magnetic flux was not able to stay on a gradient of the magnetic field, and the magnetic flux pinning were moved to centre of the HTS bulk by the centripetal force,...

Ngày tải lên: 21/06/2014, 02:20

... control system for any load. Magnetic Bearings, Theory and Applications4 6 3. 2 Magnetic Suspension System with Hybrid Magnet In order to reduce power consumption and continuous power supply, ... 2 k 1 k 3 k Table 3 c 1 c Base Fig. 6. A model of vibration isolator that can suppress both tabletop and ground vibrations Magnetic Bearings, Theory and Application...

Ngày tải lên: 21/06/2014, 02:20

... A129-A 137 . Askerzade I. N. (20 03) . Temperature dependence of the London penetration depth of YNi2B2C borocarbids using two-band Ginzburg-Landau theory. Acta Physica Slovaca, V. 53, No. 4, p .32 1 -32 7. ... N. (20 03) . Ginzburg–Landau theory for two-band s-wave superconductors: application to non -magnetic borocarbides LuNi2B2C, YNi2B2C and magnesium diboride MgB2. Physica C,...

Ngày tải lên: 19/06/2014, 21:20

... x T T p pc (11) where V is the eigenvector matrix in (7), and it serves as the transformation matrix: 11 21 31 1 12 22 32 2 12 13 23 33 3 1 23 ,,, T T T T TT T TT N N NN N T N NNN vvv v vvv v vvv ... 93 Fig. 3. 3- D geometry of two reflecting points. where BB’ is the distance between projection points of Rx and Tx on the wall and BC and B’C’ are the distance...

Ngày tải lên: 20/06/2014, 04:20

... these parameters simultaneously. Note that ( 23) can be decoupled as 11 12 11 21 22 23 22 32 33 33 2 21 11 22 2 33 11 11 11 222 11 1 33 33 133 122 2 11 00 00 000 00 0 0 00 () 0 00 0 0 00 0 0 ... 101 and 11 12 21 22 23 24 32 33 42 44 00 0 00 00 bb bbbb bb bb ⎡⎤ ⎢⎥ ⎢⎥ < ⎢⎥ ⎢⎥ ⎣⎦ (26) then 11 14 15 11 12 22 23 21 22 23 24 32 33 36 32 33 41 44 51 55 42 4...

Ngày tải lên: 20/06/2014, 04:20