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21 Apr 2004: Ann. Rev. Fluid Mech. 24, 313-358, 1992. 76. Tutty, O.R. & Pedley, T.J.

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.

7 Jan 2004: Thereforeexpression (2.23) is the symmetric outer product. (β̂β̌) (σ̂ σ̌)1{. α (etHv) τ H et} {. α (etHv) τ H et}T. (2.24). Moreover, equations (2.12) and

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.

23 Jan 2004: 24 h(1. 14 cos 2ωh). 8ω2+. 5 sin 2ωh. 64ω3,. θ4 =h4.

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

23 Apr 2004: Fibres (and platelets, although they are less well studied) are used in compositematerials because a small volume fraction can have a large effect on the properties(see chapter 24 by Shaqfeh). ... Shaqfeh describes in chapter 24 how fibres can have avery

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

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.

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