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2 Sep 2012: are close (a) to each other; and (b) to the predictionsof continuum diffusion. ... Dk T. a= B. eff6ph. D Mµ -1 3. t pspreading = ( )a D2 22.

15 Aug 2012: For any ω and any finite box B, we denote by ωB the followingconfiguration:. ... and b,where the symmetric function κN = κN,ω,C is given by.

28 Aug 2012: Hydrological Processes, v. 25, p. 1361-1372. García, M., Ercilla, G., Alonso, B., Casas, D. ... Georgina Cronin began a postgraduate qualification in Information and Library Management by distance learning from Northumbria University which has been

7 Mar 2012: B]ecause this is the rate of profits which is being realised in the present …, it is also the rate of profits which that present experience will lead entrepreneurs in general

10 May 2012: Recall that. φ(x, k) = a(k, t)eikx b(k, t)eikx as x. ... anda(k, t) = a(k, 0), b(k, t) = b(k, 0)e8ik. 3t.

27 Nov 2012: Then b is a scalar multiple of a, say b = ta witht R. ... So b′ = b ka is also in Λ and has.

15 Jan 2012: It is worth notingthat conditions A and B resulted in the same number of assignedmain-chain resonances. ... examined the chemical shift values in the spectra under con-ditions A and B (Fig.

30 Oct 2012: Roberts with Peter (cat) on ‘Penola’ Reference: P51/8/R009 Reference: P51/8/R009 Title: B.B. ... He has […] div class='image-page' div class='top-metadata' pspan class='mdk-Title'Title: /spanspan class='mdv-Title'B.B.

28 Nov 2012: Forexample if a,b C and x,y,z V , then. (x,ay bz) =1. ... Then 〈Pa,Pb〉 = (a,b) for a,b V. So for each g G.

1 Oct 2012: van Ruymbeke V. Vergiani N. Vidro, ED†R. B. B. Wardy, CTH R. ... B. B. Wardy, CTH J. I. Warren, CC C. Weiss, CL C.

28 Mar 2012: 75 APPENDIX B DERIVATION OF THE UPPER BOUNDS OF THE SUBOPTIMALITY OF SOLUTIONS PRODUCED BY THE MARKET BASED. ... 18. CHAPTER 2 BACKGROUND. computations and communicating with each other (refer to sectors B and D in Figure 5).

2 Sep 2012: 69, part 3 Plate 3. ( b ) FIGURE 3. Patterns in layers of C. ... b ) (%)sc-iip of a polka-dot piittcrn wit11 sonic t o n.

27 Aug 2012: Figure 1. Sketches of microscopic swimmers, to scale. (a) E. coli.(b) C. ... local direction of motion of the filament and(b) a filament can deform in a time-periodic way and yet createnon-zero time-averaged propulsion.

27 Aug 2012: external body force F per unit mass, (b) an external couple L, and (c) intrinsic swimming motions. ... 2 1 mm for an algal cell with B = 3.4 s, Vs = 63 pm S-I.

24 Feb 2012: Every set Hb occurs in the numbering exactly once. More precisely, all b B areindices of sets Hb occurring in the numbering F0,F1,F2,. ; ... The class {B : B m A} is calledthe many-one degree of A.

3 Dec 2012: 3.8.5 B-B mixing 28. 4. Processes 29. 4.1 Beams 29. 4.1.1 Parton distributions 29. ... Using this procedure, we find that the predicted angular distribution for secondary b.

24 Feb 2012: 1935 Colonel Michael H Cobb (d)Professor Sheppard S FrereMr Richard J B Walker CVO (d). ... R StylesMr Charles L T Temple-RichardsMr edward D B WayMr Simon P C WhitakerMr Christopher M Wright.

2 Sep 2012: b e r a n d the zone of inactive cells is abolished. ... Also note the lack of boundary-imposed symmetry. (b) Taken near the centre.

19 Oct 2012: Gould, A L Gregory, A Ozornin, K S Siencnik, B B Sun, J Y Tan, E Tsiaulouski. ... Medical Sciences: Y Y Chua, T J Hargreaves, M Roshen, F W B Sanders (Iris Rushton Prize), B B Sun (Iris Rushton Prize).

30 Oct 2012: Ryder and B.B. Roberts Reference: P51/8/G061 Reference: P51/8/G061 Title: Pram by beach, Penguin Island, South Shetlands, with L.C.D. ... Ryder and B.B. Roberts Description: plastic negative Collection: British Graham Land Expedition 1934-37 Summary text: