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9 Feb 2004: r = (F/πV )1/2. (2.24)In contrast to the instantaneous, fixed volume release of the last section, there is not a finite radius at whichthe mass of particulate matter ... Applying these concepts to the relationship for the density of deposit for a single

9 Mar 2004: e-mail: grae@esc.cam.ac.uk; heh1@esc.cam.ac.uk. (Received 24 July and in revised form 27 March 1997). ... 24/3λRa1/3 (3.1). between the Nusselt number Nu for thermal convection in the liquid region and theRayleigh number.

25 Jun 2004: 2 ( a 2 1 ),where the parameters a and l were determined by numericalanalysis as a' 1.24 @17# and l' 1.2 @6#. ... JETP Lett. 67, 521 1998!#.@23# B.V. Svistunov, Phys. Lett. A 287, 169 2001!@24# M.J.

19 Jan 2004: 2iUψ. z= 2ψ (1 |ψ|2)ψ (24). subject to the boundary condition ψ 1 as |x|. ... The expansion of equation (24) about zero to O(2) gives four equations on seven unknownsU, m, a00, b00, c20, c10, c01.

19 Nov 2004: VpLp dV = 2iσ. V. p[ψ 20 p. 2iσp] dV. (24)Re-arranging this equation and using (15) again, we find that. ... S′ = 12zR. ′ v00 R′, (B.24). or, after simplification,. 2.

8 Oct 2004: EP/Uk. 2 =(κ. 2πh. )2k2. [lnh. 2aδ+. 1. 2. ](24). which differs from (18) by 12.

25 Jun 2004: 1.24 for U = 0.63 andh , dy1.62 for U. = 0.69.

14 Nov 2004: n. }. (4.24). Therefore v is the opt-th column of the matrix W , so expression (3.12) impliesHv = eopt in theory, where eopt is the opt-th coordinate vector in

11 Oct 2004: invited editorial), Eur. J. Nucl. Med. 24, 713 (1997). [21] F.J.T. ... 24] A.S. Fokas, R.G. Novikov, Discrete Analogues of –Equations and of Radon Trans-form, C.

14 Jul 2004: Appl. Prob. 24 (1992),. 509–531. School of Economics, Mathematics and Statistics, Birkbeck College, University of.