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Cn d u. This is a cubic algebraic curve in s;t 2 R (a suggested general reference on this type of curves is 13), which defines the region C in ðAÞ¼ sþi t ;2 R d 2 ÞÞ½ð 1 2þð u 1 Þðv P 0 n o By Theorem 21, it follows that rðAÞ C inðAÞIfs > d 1ðAÞ or s < d 2ðAÞ, then sþit cannot satisfy the defining equation of C ðAÞ(always for s;t 2R), and thus, the curve C lies in the. #è Ê>0 4 >/>>>k ) 8p ) >¸> >» >£>»>¨>¼> ¶ ¡ d 0°6 > >°>»>¢ 8¼ #ÿ %$ Õ $7$ 1DRWDND 6ä B í. ³³tan ln cos cot ln sinu du u C u du u C ³³sec ln sec tan csc ln csc cotu du u u C u du u u C ln u e du e C a du Cu u u a a ³³ 22 22 1 arcsin arctan du u du u CC au a u a a a ³³ 22 1 sec du u arc C u u a aa ³ _____ Definition of a Critical Number.
>©>µ>²> > > >¼> '¨ M d ± %¼ N#ã. #è Ê >/>>>k ± =0°6 $ % £4E ) %T>) ) 8p ) >¸> >» >£>»>¨>¼> ¶ ¡ d 0°6 4 > >°>»>¢ 8¼ p7 M3d. Since U m0 forms a complete orthonormal set Using this form of c in the Schr€odinger equation, one obtains h2 2m 0 r2 þ h2 m 0 kpþ h2k2 2m 0 þVðrÞ U nkðrÞ¼E nðkÞU nkðrÞ ðA11Þ However, U m0 is the wavefunction for k ¼ 0 in the nth band satisfying the equation h2 2m 0 r2 þVðrÞ U m0ðrÞ¼E mð0ÞU m0ðrÞ ðA12Þ We now put Eq (A10) in (A11) and use (A12) to obtain.
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>& Ü6 >' ¦0{ Â « b34 Æ n ¼ M0t 8' Æ ç Á · s è à Å é ´ à Å é s è à Å é ´ à Å é s è à Å é ´ à Å é ´ à Å é. Ç «_>E ¥ ¼ _ ° D b Ýb X Í0 Ò Numerical Analysis of Effects of Outside Air Contro l for Offices Part 1 Basic Analysis of Regional Characteristics o f Effects of Hybrid AirConditioning. 15 ¼ d 33 d 31 ð14 33 ¼ 573 10 11 C/N, d 31 ¼ 237 10 11 C/N and d 15 ¼ 810 10 11 C/N as reported by Berlincourt and Jaffe (1958) Also, the properties reported by Deeg (1980) and Pak (1992) for PZT5H poled ceramic are d 33 ¼ 315 10 10 C/N, d.
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Where F(c) is the Helmholtz free energy and is a positive constant. / 0 1 2 3 4 5 5 / 2 6 7 2 3 5 1 8 7 2 9 2 5 2 9 ;2 < 2 / = 8 2 9 9 , > 5 3 ?. @ ab c bed f , g6 h !" i j * k j l h3 m' n l o j * 3p.
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