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On two‐phase modeling of dewatering pulp suspensions
www.damtp.cam.ac.uk/user/drh39/2021_pulp.pdf1 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 -
Dr A. Hansen Mathematical Tripos Part II: Michaelmas Term ...
www.damtp.cam.ac.uk/research/afha/lectures/Part_II_NumAn/b10.pdf26 Oct 2020: Thus,. with k = t,. Euler: yn = (I kA)ny0, 1 z = e. -
Preprint typeset in JHEP style - HYPER VERSION Lent ...
www.damtp.cam.ac.uk/user/tong/aqm/aqm.pdf31 May 2023: Preprint typeset in JHEP style - HYPER VERSION Lent Term, 2017. Applications of Quantum MechanicsUniversity of Cambridge Part II Mathematical Tripos. David Tong. Department of Applied Mathematics and Theoretical Physics,. Centre for Mathematical -
ELIFE06088 1..31
www.damtp.cam.ac.uk/user/gold/pdfs/Drosophila_axis.pdf23 Sep 2015: along the anterior (kA = 1000 μm, hA0 = 0:8) and strongly along the posterior-lateral cortex (kP = 150 μm, hP0 = 0, see ‘Materials and methods’ MT nucleation. ... the inset of panel C (yellow circles). In all panels, parameter values for anterior -
flm563.dvi
www.damtp.cam.ac.uk/user/mem/papers/RECOIL/remote-recoil.pdf19 Oct 2013: Another importantwave activity measure is given by the pseudomomentum vector,. p = kA =h′ u′. ... Because of the ray-invariance of absolute frequency we have that |kA| = |kB | asympto-tically. -
Publications | Cantab Capital Institute for the Mathematics of…
www.damtp.cam.ac.uk/research/ccimi/publications?page=1814 Jun 2024: KA Bacik, S Lovett, C-CP Caulfield, NM Vriend. – Phys Rev Lett. -
Publications | Astrophysics
www.damtp.cam.ac.uk/research/astro/publications?page=5214 Jun 2024: MR Bate, SH Lubow, GI Ogilvie, KA Miller. (2003). (doi: 10.48550/arxiv.astro-ph/0301154). -
solidstate
www.damtp.cam.ac.uk/user/tong/aqm/solid3.pdf7 Apr 2021: structure. E = C cos(ka). Then the velocity in a constant electric field oscillates as. ... v(k) =Ca. sin(ka) = Ca. sineEa. t. The Bloch frequency is! = -
dblp.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/dblp.pdf1 Sep 2011: On Lp-boundedness of the L2-projectoronto nite element spacesA. Yu. Shadrin1. IntroductionIn [Sh] we proved that, for p suciently close to 2, the Lp-norm of the L2-projector P onto the space S of polynomial splines of order k on a knot-sequence is -
SHA.dvi
www.damtp.cam.ac.uk/user/na/people/Alexei/papers/dmrus.pdf1 Sep 2011: TO KA-SAETSQ PORQDKA POLIGARMONINOSTI (g) = @(f)=@xj, TO, POSKOLXKU OPERACIQ DIFFERENCIRO-WANIQ SOHRANQET TOT PORQDOK, IMEEMr2(g) = 0; = m1 1 2m1 = m:pREDLOVENIE 1a0, A S NIM I SLUAJ 1a)
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