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  2. Lister Publications

    www.itg.cam.ac.uk/people/John/pubs.html
    9 Nov 2017: Falling plumes of point particles in viscous fluid. Phys. Fluids 24, 123101.
  3. J. Fluid Mech. (2017), vol. 820, pp. 400–423. c© ...

    www.itg.cam.ac.uk/people/heh/Paper258.pdf
    18 May 2017: on the y-axis,with τ of (a) 0.085, (b) 0.24, (c) 0.39, (d) 0.55, (e) 0.71, ( f ) 0.87, (g) 1.00 and ... mUmH. 3F10 , (4.23). q= UmH2. sin2/3 θE2/3eq D1F1/30 , (4.24).
  4. 18 May 2017: 23 DECEMBER 2016. 0031-9007=16=117(26)=268001(5) 268001-1 2016 American Physical Society. the crack, and a Nikon D7100 camera (1920 1080 pixels,frame rate 24 fps) is
  5. J. Fluid Mech. (2016), vol. 802, pp. 750–759. c© ...

    www.itg.cam.ac.uk/people/heh/Paper256.pdf
    18 May 2017: 1γ). 1H(L). (p11/γD p11/γS. )(2.23). (. γ. 1γ). 1H(L). p11/γD. (2.24).
  6. 18 May 2017: x = h(y) = 16 y3 c1y c2, (4.24)where c1 and c2 are constants. ... angles. SIAM J. Appl. Math. 49, 1009–1028. (doi:10.1137/0149061)24. Vogel TI. 2013 Liquid bridges between balls: the small volume instability.
  7. J. Fluid Mech. (2016), vol. 791, pp. 329–357. c© ...

    www.itg.cam.ac.uk/people/heh/Paper254.pdf
    18 May 2017: Note that (2.24) implies thatui is independent of z in the interior of each isopycnal layer, hi1 < z < hi. ... that theflow is independent of the vertical coordinate z in the interior of each layer, ui/z=0,as implied by (2.24).

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