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27 Nov 2012: multiply by a test function and integrate by parts using the bound-ary conditions in their classical format. ... Hint : start with a classical solu-tion, multiply by a test functionv C1([0, 1]) and integrate by parts).

5 Sep 2012: One of our objectives is to test such a minimal modelagainst experiments in the limit of highly concentrated suspen-sions and to provide systematic guidance for more accurate futuremodels. ... Experiments. We test the T-phase of the SPR model against

22 Aug 2012: days via baroclinic eddy motions in middle latitudes. By contrast, vertical transport through a similar alti- tude range in the stratosphere takes months, indeed a year or more in the lower ... the tropopause but also to push it to higher altitudes and

2 Sep 2012: Two types of tests of the physicist’s approach to flocking are required. ... y. reported above are among the few quantitative tests of active-matter theories.

13 Jan 2012: RPðxj0Þ ndx 1, i.e., a test particle produces a net deficit of. ... Animportant step of the preliminary tests was investigating the link-parameter l between the physical and reciprocal spaces.

2 Sep 2012: 4. Legendre expansion for arbitrary Peclet number. Because the predictions of the previous section wereunexpected when the project was commenced, it wasthought advisable to test them by solving Eqs. ... Hence, though perhaps possible, a definitive

25 Mar 2012: The middle line of expression (4.2) isrelevant for sufficiently small λ. ... 17. Although local calculations provide solutions to the three test problems ofSection 4, the different problems being generated by different choices of X , theLagrange method

31 Oct 2012: 3.13. Chemical and bacterial growth fronts. 1343.14. Front or interface dynamics as a test of the order of a phase transition. ... Middlecolumn: the Swift–Hohenberg equation of Section 2.11.2 (middle) and an extension of it as in Fig.