'Characteristic length' presentation slideshows

Amauri Pereira de Oliveira

Summer School Rio de Janeiro March 2009 3. PBL MODELING. Amauri Pereira de Oliveira. Group of Micrometeorology. Topics. Micrometeorology PBL properties PBL modeling Modeling surface-biosphere interaction Modeling Maritime PBL Modeling Convective PBL. Part 3. PBL MODELLING. Model.

654 views • 56 slides

Passive Properties of Axons: The neuron described as a wire.

Passive Properties of Axons: The neuron described as a wire. Passive processing or cable properties. Power point taken (in part) from Fundamental Neuroscience, 3 rd Ed. Squires, Berg, Bloom, du Lac, Ghosh & Spitzer, Academic Press (Elsevier), 2008. Areas of Neural Processing.

1.02k views • 47 slides

Mixed order phase transitions

Mixed order phase transitions. David Mukamel. Amir Bar, DM (PRL, 122, 01570 (2014)) . Phase transitions of mixed order . (a) diverging length as in second order transitions or (b) discontinuous order parameter as in first order transitions.

609 views • 38 slides

CE 261 Open Channel Flow uvm/~imohamme/ce261/

CE 261 Open Channel Flow http://www.uvm.edu/~imohamme/ce261/. Ibrahim Mohammed http://www.uvm.edu/~imohamme imohamme@uvm.edu. Who Am I?. I am a Post Doctorate Associate at the EPSCoR Vermont

868 views • 31 slides

Measurements of characteristic pressure profile lengths and comparison to turbulence

Measurements of characteristic pressure profile lengths and comparison to turbulence scale lengths in RFX-mod edge. P.Scarin , M.Agostini, R.Cavazzana, F. Sattin, G.Serianni, M. Spolaore, N. Vianello. Consorzio RFX, Associazione EURATOM-ENEA sulla fusione, C.so Stati Uniti 4, Padova, Italy.

446 views • 30 slides

Covalent Bonding

Covalent Bonding. Chemistry 5th Edition McMurry/Fay. Electronegativity. ? = (E i + E ea )/2 Usually converted to a unitless number between 0 and 4. Low ? ? form cation High ? ? form anion. Electronegativity. Bond polarity is due to electronegativity differences between atoms.

503 views • 24 slides

Diffraction

Diffraction.

438 views • 21 slides

NATURE | VOL 408 | 23 NOVEMBER 2000 |www.nature.com Optical gain in silicon nanocrystals

457 views • 19 slides

Spintronics with topological insulator

Spintronics with topological insulator. Takehito Yokoyama, Yukio Tanaka * , and Naoto Nagaosa Department of Applied Physics, University of Tokyo, Japan * Department of Applied Physics, Nagoya University, Japan. arXiv:0907.2810. Edge state s. From http://www.physics.upenn.edu/~kane/.

404 views • 16 slides

Adaptive optics

451 views • 16 slides

Correlation Length of Energy at the Base of Coronal Holes

261 views • 15 slides

Lecture Objectives:

Lecture Objectives:. Compare Navier Stokes equations and Reynolds Averaged Navier Stokes equations Define Reynolds stresses, Kinetic energy and Dissipation Solve example CFD software. Time Averaged Momentum Equation. Instantaneous velocity. Average velocities. Reynolds stresses.

325 views • 11 slides

Calculations of the h eat transfer coefficients for the TM0

176 views • 5 slides

MOTIVATION.

101 views • 1 slides