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9 Mar 2004: J. Fluid Mech. (2003), vol. 483, pp. 165–197. c 2003 Cambridge University PressDOI: 10.1017/S0022112003004129 Printed in the United Kingdom. 165. A model for diffusion-controlled solidification ofternary alloys in mushy layers†. By D. M.

21 Oct 2004: Since K S, we have Ka Sa. On the other hand, ifb Sa then b L for some special chain L and each of the three possiblerelationships given in our key ... Thus Sa Ka, soSa = Ka and Sa is a special chain.).

7 Jul 2004: Mater Sci Forum 1996;217}222:1883.[7] Lankford J, Dannemann KA. Strain rate e!ects in porous materials.

18 Jun 2004: The NuMI ν beam : III. protons. π+. • Horn pulsed with 200 kA • Toroidal Magnetic field B I/r between.

3 Jun 2004: very rapid (1g ka).

23 Nov 2004: fitted to the data using the ORIGIN program supplied by themanufacturer yielding the stoichiometry N, the binary equilibrium constant Ka (= Kd-1)and the enthalpy of binding. ... Peptide binding to a-adaptin wild-type appendagePeptide Sequence Kd(mM)

6 May 2004: 5] Seffen KA, Pellegrino S. “Deployment dynamics of tape springs”. Proceedings of the RoyalSociety of London, Part A, 1999;455:1003-1048.

10 Dec 2004: yQ;pv7uw{NÃ<JKLd8; I#BH<U?M <VOQXYSL> X;DOQU?RT;Xrq s7 [ yQ;GrU?BC; KÃ<JKLd8; I#BH<U?Me'Se> X#;DOQUVRC;X>]SmZts#KmtI|Pq7687µE7

6 Jan 2004: tKP -3K’h+’ (h zP)3. Wp - Ka)e’zp 2. 01. (h Q3Cr W, - l)y,'l - (h zJ3y;(K, - K,) _d2 W 24.

8 Oct 2004: He found that, provided ka 1, where a is the core radius,σ2 =. ( κ2πh2. )2 [1 khK1(kh) 12(kh). 2ω(akδ)]. [1 khK1(kh) (kh)2K0(kh) ... Classical Crow instability. Crow used the cut-off method to determine the growth rate, σ , of the instability in