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N xx Therefore, the positive equilibrium point is globally asymptotically stable References 1 D Li, P Li, X Li, Dynamical Properties for a Class of FourthOrder Nonlinear Difference Equation, Advances in Difference Equations, Volume 08, Article ID. Mar 04, 17 · N xx = M xx = 0 _ at y=0 and y=b u 0= w 0 =φ x = 0 N yy = M yy = 0 _ 0 5 10 15 25 30 35 40 45 50 a/h 0004 0006 0008 0010 0012 0014 0016 0018 00 D e f l e c t i o n, w _ Figure 115–3 TSDT 3D Elasticity Solution FSDT CLPT Bending of a symmetric cross ply (0/90/90/0) laminate under uniformly distributed load E 1=25E 2 , G 12=G. May 04, 21 · µ¶ŸâÍ m ·ªë *p%lJÁ ò¡ —6pM põÔDáPŒáJyÏvÕ@,©a#Ö AÁR”@>î^ú oD Vè›X!.
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Ã’’1ëÍKå— zð 9¤B% ´DèOZ 1·8Î R% îíaFág GPN DÄ Íƒ Ž HÌ^2Ø (Ë/õ©Å«yM Äܤž‚‹¤L ÊÖåCB\ã ßž n'Ý €¸ gf?ÆÃÿAåû¢»0ýO 3^ô~g;w#,Ò û» ÁúT€ ÜzmÇþ *Ë #£ êTöÍK eMݨ’\«A Þ~b Œ tïU !’$’E;” 1ëÏ4óæ;&åi 2Ù9ÆNzÓc ŒR ÀŒ œ“M"Õ5 ®f1 “ ô. (8) The Fourier series coefficients R(n) xx (¿) are referred to as the cyclic autocorrelation function The DC Fourier coefficient in particular is called the time averaged ACF and is determined via R˜(o) XX(¿) = ˆ 1 T(2) o!Z T(2) o 2 ¡T (2) o 2 RXX(t;t¡¿)dt (9) The corresponding timeaveraged power spectrum is defined via the. í;— î öð½ WŸ>þÑ ïß{üù{1„ÿõGŸ\ßh–i _šWyº Ú{ì³Ç>{ìÛôØóe†ŒÏW 2>âÙc¿ =ŸMl¿ö>»Ÿ¨ÙdÅ;>{'ÊgQðø}öÓEÐÎ>ûì³Ï>û–}v.
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