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4 Mar 2016: ux0 þ rðtÞ; t uðx0; tÞþ rðtÞu xðx0; tÞ: (24). As the velocity field, the distance x and the displacement rare made dimensionless using n0x, k.

23 Jul 2016: 24). Finally, inserting (24) into (22) and (23) yields. ‖u(tn1) un1‖ t2r4‖f(2r2)t. ... 24 C. Liu, A. Iserles, X. Wu. For the time integrators Brik1 and Brik2 derived in this paper we use thetolerance 1015 and choose m = 2 in the waveform relaxation

19 Oct 2016: This paper is based on an invited lecture given by Keith Moffatt at the 68th Annual Meeting of the APSDivision of Fluid Dynamics, which was held 22–24 November 2015 in

6 Oct 2016: 24. 2.2.4 Proof of the factorization theorem for SDP lifts. We now give a proof of Theorem 3.

11 Jan 2016: leakage rate predicted by (2.24) is then unphysical because there is no fluidabove the outlet to draw. ... Generally, this assumptionis invalid if the current delivers a smaller flux towards the outlet than is predicted toleak according to (2.24).

26 Nov 2016: φ(x, y) = (2 2x y) e2xy sin(2x y) (y 2) ex , (9.24).

1 Jun 2016: Received 2 December 2015; revised 13 April 2016; accepted 24 April 2016). ... 6 ms 12 ms 18 ms 24 ms. 2000. –2000. 2000.

30 Oct 2016: What is the physical meaning of Ψ in 3.1 and 3.24? ... What are the meanings of Ẋc and Ṙ in 3.24? 2.

10 Feb 2016: ZΛZsΛ. ]1/2= 1. [d 22. γφ. ]δs (5.24). with γφ as in (5.16).

21 Jan 2016: Although this issue has been quite widely recognized [24, 56, 60], there have been few attempts madethus far to extend the existing theory to infinite-dimensional models (see 1.4).