By Sheng Jin, Byung-Jae Choi (auth.), Tai-hoon Kim, Hojjat Adeli, Adrian Stoica, Byeong-Ho Kang (eds.)
This ebook includes chosen papers of the overseas meetings, CA and CES3 2011, held as a part of the longer term iteration info know-how convention, FGIT 2011, at the side of GDC 2011, Jeju Island, Korea, in December 2011. The papers offered have been rigorously reviewed and chosen from a variety of submissions and focuse at the numerous points of keep watch over and automation, and circuits, regulate, communique, electrical energy, electronics, power, process, sign and simulation.
Read Online or Download Control and Automation, and Energy System Engineering: International Conferences, CA and CES3 2011, Held as Part of the Future Generation Information Technology Conference, FGIT 2011, in Conjunction with GDC 2011, Jeju Island, Korea, December 8-10, 2011. PDF
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Additional resources for Control and Automation, and Energy System Engineering: International Conferences, CA and CES3 2011, Held as Part of the Future Generation Information Technology Conference, FGIT 2011, in Conjunction with GDC 2011, Jeju Island, Korea, December 8-10, 2011.
2. Components for installing encoded disc Because, encoded disc assembling process is performed visually, eye fatigue and operator error are matter. 01 mm and it is so coarse to measure code pattern runout which is order of micrometers. Using microscope table (where toolmaker microscope is used) for measuring code pattern runout is time and labor intensive and inaccurate, so we need an accurate and quick instrument for measuring code pattern runout and installation of encoded disk. 3 Design of Purposed Instrument In this paper an instrument is described for installing encoded disc that can measure runout of encoded disc easily and precisely during the installation or after temporary A High Accuracy Method for Rapid Measurement of Resulted Code Pattern Radial Runout 39 installation process.
By U 2 ∈ L∞ and (13), ( x2 − x2* ) ∈ L∞ and x2 ∈ L∞ . Inductively, we can prove xi ∈ L∞ , i = 3, 4, , n and so do x(t ) . Thus, all the solutions x(t ) of the closed-loop system (8) and (14) are well-defined and globally bounded on [ 0, + ∞ ) . Next, it will be shown that y (t ) − yr (t ) = z1 (t ) − yr (t ) < ε , ∀t ≥ T > 0 . (18) This is easily shown from (13), (17) and by tuning the parameter δ as follows: σ n y (t ) − yr (t ) = x1 (t ) ≤ Vn ( x(t )) ≤ 6nσ −1 δ vi−1 + pi μi < ε . i =1 Therefore, for any ε > 0 , there is δ (ε ) > 0 such that (18) is satisfied.
If we call optimum S as S opt . , then we have: Fig. 9. K opt. and S opt . = 2eσ S K min . σe e , for different values of S Fig. 10. Accuracy of determination Sσ U versus σe, Uσ S and variable S with different K values fixed component versus average code pattern line space `(31) component A High Accuracy Method for Rapid Measurement of Resulted Code Pattern Radial Runout 47 Table 1 and 2 describe in brief different usage of recommended instrument for measuring radial runout of disc code pattern and installation of encoder disc.