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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

Bernard Labatut
2004 Études internationales  
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]

Jens Eggers, Michael P. Brenner
1999 arXiv   pre-print
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]

Andrei A. Klishin, Michael P. Brenner
2021 arXiv   pre-print
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

Michael P. Brenner, Peter J. Mucha
2001 Nature  
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

Michael P. Brenner
2000 Nature  
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]

Krishna Shrinivas, Michael P Brenner
2021 bioRxiv   pre-print
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

MICHAEL P. BRENNER
2009 Journal of Fluid Mechanics  
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

Michael P. Brenner, Pia M. Sörensen
2015 Cell  
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

Michael P Brenner, Peter Constantin, Leo P Kadanoff, Alain Schenkel, Shankar C Venkataramani
1999 Nonlinearity  
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

Michael P. Brenner, Thomas P. Witelski
1998 Journal of statistical physics  
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]

Ofer Kimchi, Carl P Goodrich, Alexis Courbet, Agnese I Curatolo, Nicholas B Woodall, David Baker, Michael P Brenner
2020 bioRxiv   pre-print
ρ + k cP ρ )ρ · Pp 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

Michael P. Brenner, Sascha Hilgenfeldt, Detlef Lohse
2002 Reviews of Modern Physics  
., 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

Moses M. Hohman, Michael Shin, Gregory Rutledge, Michael P. Brenner
2001 Physics of Fluids  
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]

Dmitrii Kochkov, Jamie A. Smith, Ayya Alieva, Qing Wang, Michael P. Brenner, Stephan Hoyer
2021 arXiv   pre-print
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]

Yipei Guo, Mor Nitzan, Michael P Brenner
2020 bioRxiv   pre-print
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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