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20 Jun 2006: 24. Intriguingly, Filon-type methods (3.11) lend themselves to an alternative interpretation.Comparing (3.11) with (3.1), we observe that. ... Num. Anal.24, 365–391. Iserles, A. & Nørsett, S. P. (2004), ‘On quadrature methods for highly oscillatory

26 Apr 2006: 1.0 [24]. The slope of the linethrough data set (h), for silicon carbide particles in a succino-nitrile melt, is! ... Azouni, W. Kalita, M. Yemmou, J. Crystal Growth. 99 (1990) 201.[24] S.

15 Sep 2006: There is also. [Journal of Petrologf, Vol. 29, P t n 3, pp 599-«24, 1988] Oxford Umvcroty Prcu 19S8. ... FJH,. (24). We determined numerical solutions of (15)—(18) in addition to either (19)—(23) or merely (24).The differences were negligible.

5 May 2006: We areinterested in cases with small C2H because otherwise the distance of propagation issmall, see (3.24), and no real gravity current appears. ... Using the approximations (3.19)–(3.24), we find: (i) for S < 1.

30 May 2006: r 2 ) ( r < 1) 2.94 0.93 1.27 1.00 {(‘i ( r > 1 ). - I Cylindrical Gaussian e-T2 ( f < 00) 3.13 1-12 2.24 0.86. ... If h,R-l > Fmin (2.24) t It is interesting to compare these values with the relationship h0R-l = 2 deduced by.

30 Mar 2006: Examples includequasistatic compression imaging [26, 29], axial shear wave imaging [32] and acoustic radiationforce imaging in both quasistatic/impulsive [24] and dynamic [2] forms. ... We substitute this into Equation 24, and rearrange to produce a

26 Apr 2006: Using equations (3) and (22)–(24), it is possibleto calculate _h, S0 and T0 in terms of far-field properties T1and S1 by eliminating two of the unknowns to obtain aquadratic ... For this simula-tion we used again the values given in Table 1 and Si =

30 May 2006: 24-2. 372 H. E. Huppert and 144. E. Stern. $1. , //,/,////,//////////////,,,/,////// / ///,/I/ // / / / , // , / , / // , / / / / // / /, /' I -. FIGURE 1. An elevation of the channel, bounded by vertical walls at. ... Moh(x/L) e--ikg. (3.24). While in

26 Apr 2006: The boundaryconditions at t'0 are Eq. (12),. h"0 (z"f(t)) (23). [h]ml "0 (z"f(t)), (24). ... Wettlaufer, M.G. Worster, H.E. Huppert, Geophys. Res. Lett. 24 (1997) 1251.[12] D.L.

21 Sep 2006: 21] for upper bodypose estimation. In [24] it is suggested to partition the parameter spaceof a 3D hand model using a multi-resolution grid. ... range. At detection rates of 0.99 the false positiverate for the centre template is 0.24, wheras it is

30 May 2006: a$'(@, SY), DPI = { P } [ 1 , 1 , S&I, (4.23) where yil) = P-1Bi/Ms$2) (4.24 a). ... 4.24 b) = 1 1 8 ) K21og K O ( K 2 ). Truncating a t n = N = 2 , we obtain the second approximation.

22 Feb 2006: 3 173Premotor cortex 6 L 24 6 44 5.6 38Inferior parietal lobule 40 L 52 32 48 4.9 5. ... Cerebellum — R 38 44 24 5.5 32— L 38 52 20 5.1 4— L 38 62 16 4.9 1.

5 Jul 2006: Complementary System Selection (“Random”). • Variability to systems can be obtained by varying for example:– segmentation and clustering [3]– acoustic model decision tree [24]– acoustic model context (tri/quin-phone) [4]– ... Cambridge

16 Jul 2006: 480x360. 289.24 MB. MP3. 44100 Hz. 138.93 MB. Research seminar given by Prof.

27 Apr 2006: 2.18), which can be (2.23) and (2.24) more closely.used in (2.22) to show that Segregation is more sensitive to the value of. ... 4.24)mass reduce to and we use this condition together with (4.21)—.

10 May 2006: energy level). Wojtkowski has pointed out [24, Theorem 2.4] that the dynamics of(17) reparametrized by arc-length defines a flow on SM which coincides with theisokinetic thermostat with external ... Math. Pures Appl. 79 (2000) 953–974.[24] M.P.

30 May 2006: Stability of a large gas bubble rising through liquid 417. 24. ... 1. oo 1.712 1.26 1.42 1.10 1.24. 13.61 1.200 0.79 1.06 1.

22 May 2006: 22. 3.2.2 properties of limits. 24. 3.2.3 l’Hôpital’s rule. 24. 3.2.4 more examples. ... that. |un l| < ǫ for all n > N. 3 ELEMENTARY ANALYSIS 24.

24 Jul 2006: 480x360. 1.24 GB. WebM. 480x360. 441.66 MB. MPEG-4 Video. 480x360. 331.96 MB.

4 May 2006: The newsletter of the CAMBRIDGE QUATERNARY ISSUE 34 EASTER 2006. Professor Sir Nicholas Shackleton FRS 23.06.1937 - 24.01.2006. ... As you all know, Nick Shackleton died at the age of 68 on the 24 January 2006.