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10 May 2024: A Atoufi, KA Scott, ML Waite. – Physical Review Fluids. (2020).

12 Aug 2016: Representing the resonance between the modes @n,o,ka and by the label (n, k,, k,,), the solid circles represent (n, 1,l) resonances; the solid squares (n, 2,2) resonances;

10 Apr 2011: 2 6 ) - ( 2 8 ) to order 1/(Ka) 2 the following expression for the surface potential:. ... 1 2 ( q - 1) 1 ( q - 1)2(2q 1) 3 3 , (29) = 2 l n ( p q) Ka p q ( K a ) 2 p q.

4 Oct 2010: 11) should be replaced by lep 23ee0m f. (Hückel limit ka 1), explaining the decreasing trend [25].

20 Jan 2011: 2.12)Consider a complex tetrad of 1-forms. Ka = i(α̂AβA′ αAβ̂A′ ), Xa = α̂AβA′ αAβ̂A′ , Za = αAβA′. ... We now use(2.16) to find. φAB = 2|K|2 KA′B AA′. (1.

28 Nov 2013: J. Fluid Mech. (2013), vol. 737, pp. 205–231. c Cambridge University Press 2013 205doi:10.1017/jfm.2013.559. Stability of columnar convection in a porousmedium. Duncan R. Hewitt1,†, Jerome A. Neufeld1,2,3 and John R. Lister1. 1Institute of

31 Dec 2018: and, for small ka, the sin function is approximately linear. This means that we get.

27 Nov 2007: 0 ikeika ikeika k̃ek̃a.  = 0which yields. tan ka =2kk̃.

24 Dec 2014: Emacs Lisp List. Last updated: Wed 24 Dec 2014 11:36:00 GMT. 1270 entries. Return to ELL. c-includes.el --- Find all header files included by a source file. John Wiegley. 2014-11. plimode.el --- [Electric PLI mode: indenting and flashing and filling]

1 Dec 2023: T R A N S P O R T P H E N O M E N A A N D F L U I D M E C H A N I C S. On two-phase modeling of dewatering pulp suspensions. Daniel T. Paterson1 | Tom S. Eaves2 | Duncan R. Hewitt3 | Neil J. Balmforth4 |. D. Mark Martinez1. 1Department of Chemical