Pattern formation in plastic liquid films on elastomers by ratcheting
See our newly discovered phenomena, Pattern formation in plastic liquid films on elastomers by ratcheting
Here is the abstract:
See our newly discovered phenomena, Pattern formation in plastic liquid films on elastomers by ratcheting
Here is the abstract:
B. Tavakol and D.P. Holmes, Appl. Phys. Lett., 108, 112901, (2016).
ASCE announced the winners of six of its prestigious Society awards administered by its Engineering Mechanics Institute (EMI):
2016 Maurice A. Biot Medal: Ronaldo I. Borja, Ph.D., A.M.ASCE, Stanford University
2016 Jack E. Cermak Medal: Qiusheng Li, Ph.D., City University of Hong Kong
2016 Alfred M. Freudenthal Medal: Bruce R. Ellingwood, Ph.D., P.E., F.SEI, Dist.M.ASCE, NAE, Georgia Institute of Technology
Dear Colleague,
I kindly inform you that the XXI National Congress of Computational Mechanics and the VIII Meeting of the AIMETA Mechanics of Materials Group will take place from 27th to 29th of June 2016 at the IMT School for Advanced Studies Lucca, Lucca, Italy.
With great pleasure we announce that the plenary lectures will be delivered by Prof. Dr.-Ing. Christian Miehe (University of Stuttgart) and Prof. Vikram Deshpande (University of Cambridge).
Important deadlines for participation:
15 April 2016: Submission of abstracts.
Hi everyone,
I am to determine eigenstrains from a given result. Anyone can guide me along?
In the present work, we study morphologies arising due to competing substrate interaction, electric field, and confinement effects on a symmetric diblock copolymer. We employ a coarse-grained nonlocal Cahn-Hilliard phenomenological model taking into account the appropriate contributions of substrate interaction and electrostatic field. The proposed model couples the Ohta-Kawasaki functional with Maxwell equation of electrostatics, thus alleviating the need for any approximate solution used in previous studies.
W. Gregory Sawyer, University of Florida, USA will be the Plenary Speaker at ICoBT2016
Keynote Speakers include:
Dan Bader, University of Southampton, UK
David L. Burris, University of Delaware, USA
Simon Johnson, Unilever, UK
Mark Rainforth, University of Sheffield, UK
Feng Zhou, Lanzhou Institute of Chemical Physics, China
The post is funded through a recently awarded four year European H2020 research project SINTBAT (Silicon based materials and new processing technologies for improved lithium-ion batteries), and coordinated by VARTA.
Dear Researchers
Can you please make a correction in my Code of MATLAB
X1=[1,2,3,4]';
X2=[5,6,7,8]';
U1=[9,10,11,12]';
U2=[13,14,15,16]';
for i=1:1:4
EPS1(i,1)= U1(i,1)/X1(i,1);
EPS2(i,1)= U2(i,1)/X2(i,1);
EPS12(i,1)= 0.5*((U1(i,1)/X2(i,1))+(U2(i,1)/X1(i,1)));
defG(i)=[1+U1(i,1)/X1(i,1) 0+U1(i,1)/X2(i,1); 0+U2(i,1)/X1(i,1) 1+U2(i,1)/X2(i,1)];
end
EPS11
EPS22
EPS12
are right but for defoarmation gradient i am getting error of
Atomistic simulations have now become commonplace in the study of the deformation and failure of materials. Increase in computing power in recent years has made large-scale simulations with billions, or even trillions, of atoms a possibility. Nevertheless, most simulations to-date, are still performed with quasi-2D geometries or rather simplistic 3D setups. Although controlled studies on such well-defined structures are often required to obtain quantitative information from atomistic simulations, for qualitative studies focusing on e.g. the identification of mechanisms, researchers would greatly benefit from a methodology that helps realize more realistic configurations. The ideal scenario would be a one-on-one reconstruction of experimentally observed structures. NanoSCULPT allows you to do precisely this for both crystalline and amorphous structures.