'Order approximation' presentation slideshows

Information Theory Ying Nian Wu UCLA Department of Statistics July 9, 2007 IPAM Summer School

Information Theory Ying Nian Wu UCLA Department of Statistics July 9, 2007 IPAM Summer School. Goal: A gentle introduction to the basic concepts in information theory Emphasis: understanding and interpretations of these concepts

520 views • 41 slides

The Application of ARGO Data to BCC-GOADS

For BDCP 20 th session in Chennai. The Application of ARGO Data to BCC-GOADS. Yimin Liu *, Renhe Zhang **, Yonghong Yin ** ( * National Climate Center of China, Beijing, 100081, P. R. China, ** Chinese Academy of Meteorological Science, 100081, P. R. China . E-mail: liuym@cma.gov.)

410 views • 27 slides

The Application of ARGO Data to BCC-GOADS

For BDCP 20 th session in Chennai. The Application of ARGO Data to BCC-GOADS. Yimin Liu *, Renhe Zhang **, Yonghong Yin ** ( * National Climate Center of China, Beijing, 100081, P. R. China, ** Chinese Academy of Meteorological Science, 100081, P. R. China . E-mail: liuym@cma.gov.)

272 views • 27 slides

Double charmonium production in exclusive processes.

Double charmonium production in exclusive processes. V.V. Braguta Institute for High Energy Physics Protvino, Russia. Content:. Introduction Charmonia Distribution Amplitudes Properties of Charmonia Distribution Amplitudes Double Charmonia Production at B-factories

341 views • 26 slides

Anomalous Diffusion, Fractional Differential Equations, High Order Discretization Schemes

Anomalous Diffusion, Fractional Differential Equations, High Order Discretization Schemes. Weihua Deng Lanzhou University. Jointed with WenYi Tian, Minghua Chen, Han Zhou. Email: dengwh@lzu.edu.cn. Robert Brown , 1827. DTRW Model, Diffusion Equation. Albert Einstein, 1905.

442 views • 25 slides

Anomalous Diffusion, Fractional Differential Equations, High Order Discretization Schemes

Anomalous Diffusion, Fractional Differential Equations, High Order Discretization Schemes. Weihua Deng Lanzhou University. Jointed with WenYi Tian, Minghua Chen, Han Zhou. Email: dengwh@lzu.edu.cn. Robert Brown , 1827. DTRW Model, Diffusion Equation. Albert Einstein, 1905.

385 views • 25 slides

Rosseland Mean Opacity

Feb. 2, 2011 Rosseland Mean Absorption Poynting Vector Plane EM Waves The Radiation Spectrum: Fourier Transforms. Rosseland Mean Opacity. Recall that for large optical depth. In a star,. is large, but there is a temperature gradient. Plane parallel atmosphere.

331 views • 22 slides

Haiyan Zhang, Arthur B. Weglein, Robert Keys, Douglas Foster and Simon Shaw

224 views • 22 slides

The Islamic University of Gaza Faculty of Engineering Civil Engineering Department

The Islamic University of Gaza Faculty of Engineering Civil Engineering Department Numerical Analysis ECIV 3306 Chapter 4. Truncation Errors and Taylor Series. Introduction. Truncation errors Result when approximations are used to represent exact mathematical procedure

496 views • 21 slides

Air Quality Impacts from Airport Related Emissions: Atlanta Case Study

409 views • 20 slides

Matthew Woody, Jeffrey Rissman, Frank Binkowski, J. Jason West, Saravanan Arunachalam University of North Carolina at

An Enhanced Sub-grid Scale Approach to Characterize Air Quality Impacts of Aircraft Emissions at the Hartsfield-Jackson Atlanta International Airport. Matthew Woody, Jeffrey Rissman, Frank Binkowski, J. Jason West, Saravanan Arunachalam University of North Carolina at Chapel Hill

324 views • 19 slides

Presenter ???? Number:97662003

Phase-Adjustable Pipelining ROM-Less Direct Digital Frequency Synthesizer With a 41.66-MHz Output Frequency. Presenter ???? Number:97662003. Outline. INTRODUCTION HIGH-SPEED ROM-LESS DDFS IMPLEMENTATION AND PHYSICAL MEASUREMENT CONCLUSION REFERENCES. INTRODUCTION.

345 views • 16 slides

Representation of Hysteresis with Return Point Memory: Expanding the Operator Basis

Representation of Hysteresis with Return Point Memory: Expanding the Operator Basis. Gary Friedman Department of Electrical and Computer Engineering Drexel University. Hysteresis forms. M. D ave. H. D int. Ratchets, swimming, molecular motors, etc.

468 views • 15 slides

~ Numerical Differentiation and Integration ~ Newton-Cotes Integration Formulas Chapter 21

~ Numerical Differentiation and Integration ~ Newton-Cotes Integration Formulas Chapter 21. Differentiation. and Integration. Calculus is the mathematics of change. Since engineers continuously deal with systems and processes that change, calculus is an essential tool of engineering.

946 views • 13 slides

R. Hu is with Asuka Microelectronics Inc., Hsinchu, Taiwan, R.O.C.

Phase-Adjustable Pipelining ROM-Less Direct Digital Frequency Synthesizer With a 41.66-MHz Output Frequency. Chua-Chin Wang , Senior Member, IEEE , Jian-Ming Huang, Yih-Long Tseng, Wun-Ji Lin, and Ron Hu. R. Hu is with Asuka Microelectronics Inc., Hsinchu, Taiwan, R.O.C.

272 views • 13 slides

IV. Kinetics Introduction (Pseudo) First Order Approx. Steady State Approximation

IV. Kinetics Introduction (Pseudo) First Order Approx. Steady State Approximation. Role of Kinetics. Atmosphere is an open system- equilibrium does not apply Determine chemical fate of a species Determine concentration of a species Compare time scales for processes Chemical Physical

889 views • 11 slides

Transient Conduction & Biot Number Calculator

Transient Conduction & Biot Number Calculator. By: Matthew Hunter and Jared Oehring. Transient Conduction. Unsteady, time-dependent, problems often arise when boundary conditions change. There are two main approaches to solve these problems:

281 views • 11 slides

Taylor Polynomial Approximations

190 views • 10 slides

Bunch compression in the ATF2

SLAC Feb 2005. Bunch compression in the ATF2. M. Pivi , A. Seryi, P. T. February 15, 2005. ATF2 Extraction line with chicane and NLC-like final focus optics. FF optics: with IP b x,y = 4.0,0.1mm, L*=1 m. Computing R 56 and T 566 from each position to IP. RF cavity for bunch compression.

140 views • 6 slides

Modeling projectile motion subject to drag forces

Modeling projectile motion subject to drag forces. PHYS 361 Spring, 2011. projectile equations of motion. 2-D motion subject to gravity and drag forces. x component. Separate differential equations of motion. y component. q.

355 views • 4 slides