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16 Feb 2005: 24 cm5 g2 K7/2. These opacity laws hold fairly well in ionized accretion discs, Kramers opacity in the outer.

15 Feb 2005: A. (1973), Astron. Astrophys. 24, 337]. It is motivated by the dimensional concept that whatever physical process gives.

3 Feb 2005: Accretion Discs Mathematical Tripos, Part III. Dr G. I. Ogilvie Lent Term 2005. Linear case. In the linear case, the general solution may be found as a linear superposition of elemen-. tary solutions. One may look for elementary solutions in which

6 Jul 2005: PERGAMON. Journal of the Mechanics and Physics of Solids36 "0888# 186Ð213. S9911Ð4985:88:,! see front matter Þ 0888 Elsevier Science Ltd[ All rights reservedPII ] S 9 9 1 1 Ð 4 9 8 5 " 8 7 # 9 9 9 7 0 Ð 6. Strain gradient crystal plasticity]

4 Aug 2005: Revised 24 March 1998. the Cosserat and Toupin—Mindlin theories were developed for linear elastic materials. ... 1and u. 2at each ‘mid-side’ node. The total number of degrees of freedom per element is 24.

31 Aug 2005: N NI I [!L'jjpqT11C(0)(N-1)op)!L',skJ. (2.24)0-1 P-I. In the foregoing we have assumed that uo) is afunction of £<!).

6 Jul 2005: The structures were formed using a through-mask-plating technology [24, 25]. Figure 4 shows the processflow. ... 24] Shenoy R V and Datta M 1996 Effect of mask wall angle onshape evolution during through-mask electrochemicalmicromachining J.

6 Jul 2005: The brief process can alsobe found in [24], but the detailed process and electrical testswill be reported in the future. ... Microelectromech. Syst. submitted. [24] Luo J K, Fu Y Q, Flewitt A J, Spearing S M, Fleck N A andMilne W I 2005 Large

20 Mar 2005: s 1. 24. 35; and (15a). T̄ 1 T 1. Lffiffiffiffiffiffiffiffiffiffiffiffiffiffiffirf =sf Y. ... 2. M0H. s 1. 24. 35, (23a). and. w1 þ w2 v0T 2 H.

18 Sep 2005: pr2ðx; tÞ rwcw _w t þx. cw. , (24). ARTICLE IN PRESS.