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Reconcilable Differences. us-French Relations in the New Era. Brenner, Michael et Guillaume Parmentier. Brookings Institution Press, Washington, dc, 2002, 154 p
2004
Études internationales
Preserved Fulltext
Brookings Institution Press, Washington, dc, 2002, 154 p.] . Études internationales, 35 (1), 184-185. https://doi.org/10.7202/008456ar ...
Bruxelles, Bruylant, 2003, 448 p. ...
Sa grande originalité réside dans le fait qu'il est écrit par deux auteurs, dont l'un, américain, Michael Brenner, et l'autre, français, Guillaume Parmentier, nous offrent un regard croisé sur ce partenariat ...
doi:10.7202/008456ar
fatcat:jjqxqfjzvjcztnk4n2k6q4iodq
Spinning jets
[article]
1999
arXiv
pre-print
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The normal stress balance nσn = γκ gives p 0 + p 2 h 2 = γκ − v ′ 0 , where κ is the sum of the principal curvatures. ...
z, r) = p 0 (z) + p 2 (z)r 2 + . . . . (8) Plugging this into the equation of motion for v r , to leading order in r one finds the balance p 2 = 2ℓ 2 π 2 ρh 8 , (9) while the leading balance for the v ...
arXiv:physics/9912009v1
fatcat:7gupuavr3rd7tgjenyev6am6pu
Topological Design of Heterogeneous Self-Assembly
[article]
2021
arXiv
pre-print
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In terms of the spectrum, the propagator and the polylogarithm can be computed as following: D =P (I − Λ) −1 P −1 (A8) Li(T) =P Li(Λ)P −1 , (A9) where the inverse and the polylogarithm of the diagonal ...
From the partition function we can easily extract the correlation in direction of the two adjacent monomer directions: cos(θ) 2 = − 1 β ∂ ln Z (2) wl ∂P = coth(βP ) − 1 βP ≡ c(βP ) (C20) cos(θ) n =c n− ...
To account for the bending entropy, we adopt the worm-like chain model [26] where P is the bending rigidity, n is the length of the chain,t k is the unit vector in the direction of each ...
arXiv:2103.02010v1
fatcat:sidg6orlareohkqtoch7wxwicu
That sinking feeling
2001
Nature
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s Michael P. Brenner and Peter J. ...
Segrè, P. N., Liu, F., Umbanhowar, P. & Weitz, D. A. Nature 409, 594-597 (2001).
response analysis' (Hofmeyr, J.-H. S. & Cornish-Bowden, A. J. Theor. ...
doi:10.1038/35054641
pmid:11214301
fatcat:jgrf3jdiljbenc4ayckfres73a
Jets from a singular surface
2000
Nature
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I Michael P. ...
Finally,
Fluid mechanics Jets from a singular surface
Michael P. ...
doi:10.1038/35000330
pmid:10667775
fatcat:2ng2amq2cnb7tgj7jyab3fchwi
Phase separation in fluids with many interacting components
[article]
2021
bioRxiv
pre-print
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Acknowledgments We thank Ofer Kimchi, Ella King, Jon Henninger, and members of the Brenner lab for helpful discussions. ...
doi:10.1101/2021.05.06.443002
fatcat:afh4qolc35eann5u5vev5msufu
Cavitation in linear bubbles
2009
Journal of Fluid Mechanics
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v inside the bubble and the pressure far away P ∞ . ...
These estimates are consistent with experimental measurements of the properties of light emission characteristics (for a review see Brenner et al. 2002) . ...
doi:10.1017/s0022112009008167
fatcat:psao5wgopneedifdfxnekyktly
Biophysics of Molecular Gastronomy
2015
Cell
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Chefs and scientists exploring biophysical processes have given rise to molecular gastronomy. In this Commentary, we describe how a scientific understanding of recipes and techniques facilitates the development of new textures and expands the flavor palette. The new dishes that result engage our senses in unexpected ways.
doi:10.1016/j.cell.2015.03.002
pmid:25815978
fatcat:o3dwbq447nhrhjqo2lhfopipt4
Diffusion, attraction and collapse
1999
Nonlinearity
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In that case, there exists at least one critical value p c ∈ (p 0 , p 1 ) such that the final states for initial conditions for any p a and p b sufficiently close to p c with p a < p c < p b are different ...
From equation (1) we obtain d dt ρ p (x, t) dx = −p(p − 1) |∇ρ(x, t)| 2 ρ(x, t) p−2 dx + (p − 1) ρ(x, t) p+1 . (4) At p = d 2 the growth term in the rhs can be bound in terms of the dissipation term ...
doi:10.1088/0951-7715/12/4/320
fatcat:lgoa2zzzxvhepdsk5ysreiqnj4
On Spherically Symmetric Gravitational Collapse
1998
Journal of statistical physics
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The
Brenner and Witelski 869 where the gravitational force f = p r is given by corresponding to the evolution equations on the characteristics An important property of equations (5)- (7) is that they ...
= p(t) for r<r(t). ...
doi:10.1023/b:joss.0000033167.19114.b8
fatcat:o35m4a6ksndbddw4oaxd3sszru
Self-assembly based post-translational protein oscillators
[article]
2020
bioRxiv
pre-print
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ρ + k cP ρ )ρ · P dκ p dt = − k bP κ κ p (P +P ) + k uP κ (κ p · P + κ p ·P ) + k cKκ κ · K dρ p dt = − k bP ρ ρ p (P +P ) + k uP ρ (ρ p · P + ρ p ·P ) + k cKρ ρ · K dκ · K dt = k bKκ κK − (k uKκ + k ...
tot = ρ + ρ p + mP + ρK K M Kρ + (m + 1) ρ p P K M P ρ + ρ pP K M P ρ + m κ p P K M P κ (S2) . ...
doi:10.1101/2020.02.12.946145
fatcat:m77lr2jcmbaipagl37uwtwiysm
Single-bubble sonoluminescence
2002
Reviews of Modern Physics
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., 1995; Brenner, Hilgenfeldt, et al., 1996; Hilgenfeldt et al., 1996) . ...
Brenner, Hilgenfeldt, and Lohse: Single-bubble sonoluminescence Rev. Mod. ...
doi:10.1103/revmodphys.74.425
fatcat:ulprjjntjjezvfcxl6jt555qwi
Electrospinning and electrically forced jets. II. Applications
2001
Physics of Fluids
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P. Kadanoff ...
P R O O F C O P Y 0 0 7 1 0 8 P H F we plan on testing these relations with systematic experiments.
IV. ...
PROOF COPY 007108PHF PROOF COPY 007108PHF P R O O F C O P Y 0 0 7 1 0 8 P H F air interface at the axial position where the liquid is attached to the nozzle.'' ...
doi:10.1063/1.1384013
fatcat:ao6db2m57jarbo4rbmcsf6wj7a
Machine learning accelerated computational fluid dynamics
[article]
2021
arXiv
pre-print
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The density ρ is a constant, and the pressure p is a Lagrange multiplier used to enforce (1b). ...
Richardson, Weather prediction by numerical process (Cambridge university press, 2007).[2] P. Bauer, A. Thorpe, and G. ...
arXiv:2102.01010v1
fatcat:rp75forirfe43c5rtifo2qbonm
Programming cell growth into different cluster shapes using diffusible signals
[article]
2020
bioRxiv
pre-print
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To deal with the boundary condition P = 0, we decompose the potential P into 2 components: P =P +P , (S2) whereP (z) = g(z) 2π ln(|z −z|)dz (S3) (which was not certified by peer review) is the author/funder ...
The total cell velocity can therefore also be written as the sum of the two contributions: u =û +ũ, witĥ u = −∇P andũ = −∇P . ...
doi:10.1101/2020.08.29.273607
fatcat:r6qzihzufvf6fi5kxktck74iqy
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