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10 Jun 2024: Received 10 October 2023; revised 27 December 2023; accepted 24 February 2024). ... F(Z, ζ ) = 13ζ. Z0. H(Z̃) dZ̃. (3.25). We note that solutions (3.24) satisfy the matching conditions between theinner and outer regions.

2 Jan 2024: Open Sci. 10:230223. https://doi.org/10.1098/rsos.230223. Received: 24 February 2023. Accepted: 30 May 2023. ... Existing theoretical literature onsquirmers echoes the significant influence of boundaries and confinement on their dynamics [24].

1 Dec 2023: J. Fluid Mech. (2018), vol. 837, pp. 520–545. c Cambridge University Press 2018doi:10.1017/jfm.2017.829. 520. The dynamics of miscible viscous fingering fromonset to shutdown. Japinder S. Nijjer1,†, Duncan R. Hewitt1 and Jerome A. Neufeld1,2,3.

1 Dec 2023: 1/4ε. 0. dζ|X ′1|. log ε1]ε0. 1. (3.12). For the sinusoidal waveform, J 1.24, and the predictions from (3.11) are included infigure 3(d).

27 Apr 2024: 2.2.3 General Charge Distributions 20. 2.2.4 Field Lines 23. 2.2.5 Electrostatic Equilibrium 24.

12 Jun 2024: 1.3.3 An Application: Work and Potential Energy 24. 1.3.4 A Subtlety 25. ... 24 –. We learn that a conservative force, one that can be written as (1.18), has a conserved.

23 Aug 2023: 24. 3.6 Stokes Phenomena in the Complex Plane. 27. 3.6.1 Terminology. ... 0 Perturbation Methods (16 Lectures). 0.1 Introduction. • 24 lectures prised into 16. •

20 Nov 2023: Brown [27–29]) and Toeplitztheory (see A. Böttcher & B. Silberman [24–26]).

1 Dec 2023: Received 24 February 2017; revised 22 May 2017; accepted 10 July 2017;first published online 30 August 2017).

1 Dec 2023: u = 0. (2.1). In place of the Navier–Stokes equations for an unconfined fluid, in a porous medium the Darcyvelocity u is governed by Darcy’s Law [23,24], which