t r tr t t s tr s rt s q t
play

t r trt t - PowerPoint PPT Presentation

Mar 29, 2023 •334 likes •1.09k views

qt t qt s t r trt t s

  1. ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ❖♥ t❤❡ ✉♥✐❢♦r♠ ❝♦♥tr♦❧❧❛❜✐❧✐t② ♦❢ t❤❡ ♦♥❡✲❞✐♠❡♥s✐♦♥❛❧ tr❛♥s♣♦rt✲❞✐✛✉s✐♦♥ ❡q✉❛t✐♦♥ P✐❡rr❡ ▲✐ss② ▲❛❜♦r❛t♦✐r❡ ❏❛❝q✉❡s✲▲♦✉✐s ▲✐♦♥s✱ ❯♥✐✈❡rs✐té P✐❡rr❡ ❡t ▼❛r✐❡ ❈✉r✐❡ ◆❡✇ tr❡♥❞s ✐♥ ▼♦❞❡❧✐♥❣✱ ❈♦♥tr♦❧ ❛♥❞ ■♥✈❡rs❡ Pr♦❜❧❡♠s✱ ❈■▼■✱ ❚♦✉❧♦✉s❡✱ ❏✉♥❡ ✶✽✱ ✷✵✶✹

  2. ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ❚❤❡ tr❛♥s♣♦rt✲❞✐✛✉s✐♦♥ ❡q✉❛t✐♦♥ ❝♦♥tr♦❧❧❡❞ ♦♥ ♦♥❡ s✐❞❡ ✶ ■♥tr♦❞✉❝t✐♦♥ ❚❤❡ tr❛♥s♣♦rt ❡q✉❛t✐♦♥ ❯♥✐❢♦r♠ ❝♦♥tr♦❧❧❛❜✐❧✐t② ✐♥ t❤❡ ✈❛♥✐s❤✐♥❣ ✈✐s❝♦s✐t② ❧✐♠✐t ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❝♦♥tr♦❧❧❡❞ ♦♥ ♦♥❡ s✐❞❡ ✷ ■♥tr♦❞✉❝t✐♦♥ ▲✐♥❦ ❜❡t✇❡❡♥ ❤❡❛t ❛♥❞ tr❛♥s♣♦rt✲❞✐✛✉s✐♦♥ ❡q✉❛t✐♦♥ ❆♥♦t❤❡r ❛♣♣r♦❛❝❤✿ ✐♥t❡❣r❛❧ ♦❜s❡r✈❛❜✐❧✐t② ✐♥❡q✉❛❧✐t✐❡s ❈♦♥❝❧✉s✐♦♥ ✸ ❈♦♥❝❧✉s✐♦♥

  3. ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ❚❤❡ tr❛♥s♣♦rt✲❞✐✛✉s✐♦♥ ❡q✉❛t✐♦♥ ❝♦♥tr♦❧❧❡❞ ♦♥ ♦♥❡ s✐❞❡ ✶ ■♥tr♦❞✉❝t✐♦♥ ❚❤❡ tr❛♥s♣♦rt ❡q✉❛t✐♦♥ ❯♥✐❢♦r♠ ❝♦♥tr♦❧❧❛❜✐❧✐t② ✐♥ t❤❡ ✈❛♥✐s❤✐♥❣ ✈✐s❝♦s✐t② ❧✐♠✐t ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❝♦♥tr♦❧❧❡❞ ♦♥ ♦♥❡ s✐❞❡ ✷ ■♥tr♦❞✉❝t✐♦♥ ▲✐♥❦ ❜❡t✇❡❡♥ ❤❡❛t ❛♥❞ tr❛♥s♣♦rt✲❞✐✛✉s✐♦♥ ❡q✉❛t✐♦♥ ❆♥♦t❤❡r ❛♣♣r♦❛❝❤✿ ✐♥t❡❣r❛❧ ♦❜s❡r✈❛❜✐❧✐t② ✐♥❡q✉❛❧✐t✐❡s ❈♦♥❝❧✉s✐♦♥ ✸ ❈♦♥❝❧✉s✐♦♥

  4. ▼ ✵ s♣❡❡❞✱ ❞✐✛✉s✐♦♥ ❝♦❡✣❝✐❡♥t ✵ ✭❞❡st✐♥❡❞ t♦ t❡♥❞ t♦ ✵✮✱ ❧❡♥❣t❤ ▲ ✵✱ ▲ ✷ ✵ ▲ ✐♥✐t✐❛❧ ❝♦♥❞✐t✐♦♥ ✭♦r ❍ ✶ ✵ ▲ ✮✱ ② ✵ ▲ ✷ ✵ ❚ ✱ ❝♦♥tr♦❧ ✈ ◗ ✵ ❚ ✵ ▲ ✳ ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ◆♦t❛t✐♦♥s ❚ > ✵ t✐♠❡✱

  5. ❞✐✛✉s✐♦♥ ❝♦❡✣❝✐❡♥t ✵ ✭❞❡st✐♥❡❞ t♦ t❡♥❞ t♦ ✵✮✱ ❧❡♥❣t❤ ▲ ✵✱ ▲ ✷ ✵ ▲ ✐♥✐t✐❛❧ ❝♦♥❞✐t✐♦♥ ✭♦r ❍ ✶ ✵ ▲ ✮✱ ② ✵ ▲ ✷ ✵ ❚ ✱ ❝♦♥tr♦❧ ✈ ◗ ✵ ❚ ✵ ▲ ✳ ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ◆♦t❛t✐♦♥s ❚ > ✵ t✐♠❡✱ ▼ � = ✵ s♣❡❡❞✱

  6. ❧❡♥❣t❤ ▲ ✵✱ ▲ ✷ ✵ ▲ ✐♥✐t✐❛❧ ❝♦♥❞✐t✐♦♥ ✭♦r ❍ ✶ ✵ ▲ ✮✱ ② ✵ ▲ ✷ ✵ ❚ ✱ ❝♦♥tr♦❧ ✈ ◗ ✵ ❚ ✵ ▲ ✳ ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ◆♦t❛t✐♦♥s ❚ > ✵ t✐♠❡✱ ▼ � = ✵ s♣❡❡❞✱ ❞✐✛✉s✐♦♥ ❝♦❡✣❝✐❡♥t ε > ✵ ✭❞❡st✐♥❡❞ t♦ t❡♥❞ t♦ ✵✮✱

  7. ▲ ✷ ✵ ▲ ✐♥✐t✐❛❧ ❝♦♥❞✐t✐♦♥ ✭♦r ❍ ✶ ✵ ▲ ✮✱ ② ✵ ▲ ✷ ✵ ❚ ✱ ❝♦♥tr♦❧ ✈ ◗ ✵ ❚ ✵ ▲ ✳ ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ◆♦t❛t✐♦♥s ❚ > ✵ t✐♠❡✱ ▼ � = ✵ s♣❡❡❞✱ ❞✐✛✉s✐♦♥ ❝♦❡✣❝✐❡♥t ε > ✵ ✭❞❡st✐♥❡❞ t♦ t❡♥❞ t♦ ✵✮✱ ❧❡♥❣t❤ ▲ > ✵✱

  8. ▲ ✷ ✵ ❚ ✱ ❝♦♥tr♦❧ ✈ ◗ ✵ ❚ ✵ ▲ ✳ ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ◆♦t❛t✐♦♥s ❚ > ✵ t✐♠❡✱ ▼ � = ✵ s♣❡❡❞✱ ❞✐✛✉s✐♦♥ ❝♦❡✣❝✐❡♥t ε > ✵ ✭❞❡st✐♥❡❞ t♦ t❡♥❞ t♦ ✵✮✱ ❧❡♥❣t❤ ▲ > ✵✱ ② ✵ ∈ ▲ ✷ ( ✵ , ▲ ) ✐♥✐t✐❛❧ ❝♦♥❞✐t✐♦♥ ✭♦r ❍ − ✶ ( ✵ , ▲ ) ✮✱

  9. ◗ ✵ ❚ ✵ ▲ ✳ ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ◆♦t❛t✐♦♥s ❚ > ✵ t✐♠❡✱ ▼ � = ✵ s♣❡❡❞✱ ❞✐✛✉s✐♦♥ ❝♦❡✣❝✐❡♥t ε > ✵ ✭❞❡st✐♥❡❞ t♦ t❡♥❞ t♦ ✵✮✱ ❧❡♥❣t❤ ▲ > ✵✱ ② ✵ ∈ ▲ ✷ ( ✵ , ▲ ) ✐♥✐t✐❛❧ ❝♦♥❞✐t✐♦♥ ✭♦r ❍ − ✶ ( ✵ , ▲ ) ✮✱ ❝♦♥tr♦❧ ✈ ∈ ▲ ✷ ( ✵ , ❚ ) ✱

  10. ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ◆♦t❛t✐♦♥s ❚ > ✵ t✐♠❡✱ ▼ � = ✵ s♣❡❡❞✱ ❞✐✛✉s✐♦♥ ❝♦❡✣❝✐❡♥t ε > ✵ ✭❞❡st✐♥❡❞ t♦ t❡♥❞ t♦ ✵✮✱ ❧❡♥❣t❤ ▲ > ✵✱ ② ✵ ∈ ▲ ✷ ( ✵ , ▲ ) ✐♥✐t✐❛❧ ❝♦♥❞✐t✐♦♥ ✭♦r ❍ − ✶ ( ✵ , ▲ ) ✮✱ ❝♦♥tr♦❧ ✈ ∈ ▲ ✷ ( ✵ , ❚ ) ✱ ◗ := ( ✵ , ❚ ) × ( ✵ , ▲ ) ✳

  11. ❉❡✜♥✐t✐♦♥ ▲❡t ❚ ▲ ▼ ❜❡ ✜①❡❞✳ ❊q✉❛t✐♦♥ ✭❚✲❉✮ ✐s ♥✉❧❧✲❝♦♥tr♦❧❧❛❜❧❡ ❛t t✐♠❡ ▲ ✷ ✵ ▲ ✱ t❤❡r❡ ❡①✐sts ✈ ▲ ✷ ✵ ❚ ❚ ✐❢ ❛♥❞ ♦♥❧② ✐❢ ❢♦r ❡✈❡r② ② ✵ s✉❝❤ t❤❛t ② ❚ ✵ ✳ ◆✉❧❧✲❝♦♥tr♦❧❧❛❜✐❧✐t② ✐♥ ❛r❜✐tr❛r② s♠❛❧❧ t✐♠❡✿ ✇❡❧❧✲❦♥♦✇♥ ❢♦r ❛ ❧♦♥❣ t✐♠❡ ✐♥ t❤❡ ♦♥❡✲❞✐♠❡♥s✐♦♥❛❧ ❝❛s❡ ✭❋❛tt♦r✐♥✐✲❘✉ss❡❧❧❵✼✶✮✳ ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ❚❤❡ ❡q✉❛t✐♦♥ ❚❤❡ tr❛♥s♣♦rt✲❞✐✛✉s✐♦♥ ❡q✉❛t✐♦♥  ② t − ε ② ①① + ▼② ① = ✵ ✐♥ ◗ ,    ② ( ., ✵ ) = ✈ ( t ) ✐♥ ( ✵ , ❚ ) ,   ✭❚✲❉✮ ② ( ., ▲ ) = ✵ ✐♥ ( ✵ , ❚ ) ,   ② ( ✵ , . ) = ② ✵ ✐♥ ( ✵ , ▲ ) .   

  12. ❚❤❡ ❚✲❉ ❡q✉❛t✐♦♥ ❚❤❡ ❤❡❛t ❡q✉❛t✐♦♥ ❈♦♥❝❧✉s✐♦♥ ■♥tr♦❞✉❝t✐♦♥ ❚❤❡ ❡q✉❛t✐♦♥ ❚❤❡ tr❛♥s♣♦rt✲❞✐✛✉s✐♦♥ ❡q✉❛t✐♦♥  ② t − ε ② ①① + ▼② ① = ✵ ✐♥ ◗ ,    ② ( ., ✵ ) = ✈ ( t ) ✐♥ ( ✵ , ❚ ) ,   ✭❚✲❉✮ ② ( ., ▲ ) = ✵ ✐♥ ( ✵ , ❚ ) ,   ② ( ✵ , . ) = ② ✵ ✐♥ ( ✵ , ▲ ) .    ❉❡✜♥✐t✐♦♥ ▲❡t ❚ , ▲ , ▼ , ε ❜❡ ✜①❡❞✳ ❊q✉❛t✐♦♥ ✭❚✲❉✮ ✐s ♥✉❧❧✲❝♦♥tr♦❧❧❛❜❧❡ ❛t t✐♠❡ ❚ ✐❢ ❛♥❞ ♦♥❧② ✐❢ ❢♦r ❡✈❡r② ② ✵ ∈ ▲ ✷ ( ✵ , ▲ ) ✱ t❤❡r❡ ❡①✐sts ✈ ∈ ▲ ✷ ( ✵ , ❚ ) s✉❝❤ t❤❛t ② ( ❚ ) = ✵ ✳ ◆✉❧❧✲❝♦♥tr♦❧❧❛❜✐❧✐t② ✐♥ ❛r❜✐tr❛r② s♠❛❧❧ t✐♠❡✿ ✇❡❧❧✲❦♥♦✇♥ ❢♦r ❛ ❧♦♥❣ t✐♠❡ ✐♥ t❤❡ ♦♥❡✲❞✐♠❡♥s✐♦♥❛❧ ❝❛s❡ ✭❋❛tt♦r✐♥✐✲❘✉ss❡❧❧❵✼✶✮✳

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend

McCaskill: Efficient Base Pair Probabilities Idea: Compute p kl := Pr[( k , l ) | S ] recursively

McCaskill: Efficient Base Pair Probabilities Idea: Compute p kl := Pr[( k , l ) | S ] recursively

McCaskill: Efficient Base Pair Probabilities Idea: Compute p kl := Pr[( k , l ) | S ] recursively (DP!), recurse from long base pairs (outside) to small ones (inside) 1) simple case (external base pair) Definition (Probability of external base

480 views • 9 slides
Sharp interface limit of the Stochastic Allen-Cahn equation in one space- dimension Simon Weber

Sharp interface limit of the Stochastic Allen-Cahn equation in one space- dimension Simon Weber

Sharp interface limit of the Stochastic Allen-Cahn equation in one space- dimension Simon Weber PhD student of Martin Hairer Warwick Mathematics Institute Introduction Allen Cahn equation in one space-dimension: - is negative derivative of

560 views • 16 slides
Web Dynamics http://www.mpi inf.mpg.de/departments/d5/teaching/ss09/dyn/ Summer Term 2009 Web

Web Dynamics http://www.mpi inf.mpg.de/departments/d5/teaching/ss09/dyn/ Summer Term 2009 Web

Web Dynamics http://www.mpi inf.mpg.de/departments/d5/teaching/ss09/dyn/ Summer Term 2009 Web Dynamics 0 1 Lecturers Dr. Ing. Ralf Schenkel Group Leader, MMCI Associated Senior Researcher, MPI INF Dr. Marc Spaniol Postdoc, MPI

510 views • 7 slides
FY 2021 & FY 2022 Unified Planning Work Program Overview and Projects Discussion MPO

FY 2021 & FY 2022 Unified Planning Work Program Overview and Projects Discussion MPO

FY 2021 & FY 2022 Unified Planning Work Program Overview and Projects Discussion MPO Planning Tasks & Budget April 14, 2020 p l a n h i l l s b o r o u g h . o r g Required Biennial Update Effective July 1, 2020 June 30,

321 views • 13 slides
Lecture 24: Magnetism (Kittel Ch. 11-12) Magnetism Quantum Electron-Electron Mechanics

Lecture 24: Magnetism (Kittel Ch. 11-12) Magnetism Quantum Electron-Electron Mechanics

Lecture 24: Magnetism (Kittel Ch. 11-12) Magnetism Quantum Electron-Electron Mechanics Interactions Physics 460 F 2006 Lect 24 1 Outline Magnetism is a purely quantum phenomenon! Totally at variance with the laws of classical physics

476 views • 34 slides
Simple Quantum Paramagnet, Canonical Ensemble Origin of magnetic moments: Electron spin

Simple Quantum Paramagnet, Canonical Ensemble Origin of magnetic moments: Electron spin

Simple Quantum Paramagnet, Canonical Ensemble Origin of magnetic moments: Electron spin and orbital angular momentum + L J S = g J e h/ 2 m e c J B B Nuclear angular momentum

389 views • 28 slides
A Holographic Realization of Ferromagnets Masafumi Ishihara ( AIMR, Tohoku University)

A Holographic Realization of Ferromagnets Masafumi Ishihara ( AIMR, Tohoku University)

A Holographic Realization of Ferromagnets Masafumi Ishihara ( AIMR, Tohoku University) Collaborators: Koji Sato ( AIMR, Tohoku University) Naoto Yokoi ( IMR, Tohoku University) Eiji Saitoh ( AIMR, IMR, Tohoku University

610 views • 18 slides
Quasi-stationary measures and metastability Alessandra Bianchi Department of Mathematics,

Quasi-stationary measures and metastability Alessandra Bianchi Department of Mathematics,

Fifth Workshop on Random Dynamical Systems University of Bielefeld, 4-5 October 2012 Quasi-stationary measures and metastability Alessandra Bianchi Department of Mathematics, University of Padova in collaboration with A. Gaudilli` ere

1.04k views • 43 slides
Schemes with Well-Controlled Dissipation (WCD) Jan Ernest Seminar of Applied Mathematics (SAM),

Schemes with Well-Controlled Dissipation (WCD) Jan Ernest Seminar of Applied Mathematics (SAM),

Schemes with Well-Controlled Dissipation (WCD) Jan Ernest Seminar of Applied Mathematics (SAM), ETH Z urich, Switzerland Jan Ernest WCD Schemes Joint work with Siddhartha Mishra Center of Mathematics for Applications (CMA),

1.55k views • 50 slides
Magnetism at finite temperature: molecular field, phase transitions - The Heisenberg model in

Magnetism at finite temperature: molecular field, phase transitions - The Heisenberg model in

Magnetism at finite temperature: molecular field, phase transitions - The Heisenberg model in molecular field approximation: ferro, antiferromagnetism. Ordering temperature; thermodynamics - Mean field for itinerant systems - Landau theory of

1.13k views • 56 slides
Soutenance dHabilitation Diriger des Recherches Thorie

Soutenance dHabilitation Diriger des Recherches Thorie

Soutenance dHabilitation Diriger des Recherches Thorie spatiale des extrmes et proprits des processus max-stables C LMENT D OMBRY Laboratoire de Mathmatiques et Applications, Universit de Poitiers.

515 views • 39 slides
Monte Carlo simulations of diffusive phase transformations: time-scale problems F. Soisson

Monte Carlo simulations of diffusive phase transformations: time-scale problems F. Soisson

Beyond Molecular Dynamics: Long Time Atomic-Scale Simulations Dresden, March 26 - 29, 2012 Monte Carlo simulations of diffusive phase transformations: time-scale problems F. Soisson Service de recherches de Mtallurgie Physique CEA Saclay

1.68k views • 15 slides
Network-Assisted MPTCP IETF#98, Chicago, March 2017 M. Boucadair (Orange) C. Jacquenet (Orange)

Network-Assisted MPTCP IETF#98, Chicago, March 2017 M. Boucadair (Orange) C. Jacquenet (Orange)

Network-Assisted MPTCP IETF#98, Chicago, March 2017 M. Boucadair (Orange) C. Jacquenet (Orange) O. Bonaventure (Tessares) W. Henderickx (ALU/Nokia) R. Skog (Ericsson) D. Behaghel (OneAccess) S. Secci (Universite Pierre et Marie Curie) S.

677 views • 35 slides
Quantum gravity from the point of view of locally covariant QFT Katarzyna Rejzner 1 INdAM (Marie

Quantum gravity from the point of view of locally covariant QFT Katarzyna Rejzner 1 INdAM (Marie

Introduction Classical theory Quantization Quantum gravity from the point of view of locally covariant QFT Katarzyna Rejzner 1 INdAM (Marie Curie) fellow University of Rome Tor Vergata Wuppertal, 01.06.2013 1 Based on the joint work with

1.06k views • 82 slides
MPTCP Hackathon 2016 curl Arnaud Dethise Jacob Eliat-Eliat Curl File transfer tool (similar

MPTCP Hackathon 2016 curl Arnaud Dethise Jacob Eliat-Eliat Curl File transfer tool (similar

MPTCP Hackathon 2016 curl Arnaud Dethise Jacob Eliat-Eliat Curl File transfer tool (similar to wget) Also has a nice application-level API Supports several common file transfer protocols (HTTP, FTP, IMAP, SCP) MPTCP awareness

706 views • 11 slides
Curl: an important differential operator on vector fields. 1 2 3 4 5 6 7 8 9 10 11 12

Curl: an important differential operator on vector fields. 1 2 3 4 5 6 7 8 9 10 11 12

Curl: an important differential operator on vector fields. 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 Green's Theorem in vector form 18 * Green's Theorem relates the integral of the tangential part of the field along C to the

577 views • 41 slides
21. Potential Functions Suppose that F = M + N = f is a gradient vector field.

21. Potential Functions Suppose that F = M + N = f is a gradient vector field.

21. Potential Functions Suppose that F = M + N = f is a gradient vector field. Then M y = f xy = f yx = N x . So, if F is a gradient vector field then M y = N x . Theorem 21.1. Let F = M + N be a vector

182 views • 3 slides
Last time: Greens theorem Let D R 2 be such that D is formed of one or more simple

Last time: Greens theorem Let D R 2 be such that D is formed of one or more simple

Last time: Greens theorem Let D R 2 be such that D is formed of one or more simple closed curves. Suppose F = P , Q is a vector field such that P and Q have continuous first order partial derivatives. Then

461 views • 5 slides
Troubleshooting AWS App Workshop Splunk Add-on for AWS 4.3+ Kamilo Amir | Splunk Cloud Architect

Troubleshooting AWS App Workshop Splunk Add-on for AWS 4.3+ Kamilo Amir | Splunk Cloud Architect

Troubleshooting AWS App Workshop Splunk Add-on for AWS 4.3+ Kamilo Amir | Splunk Cloud Architect ______________________________________________________________________________ Table of Contents 4 TROUBLESHOOTING SPLUNK APP / ADD-ON FOR AWS 4 P

296 views • 8 slides
CSCI 2133 Rapid Programming Techniques for Innovation A Python based framework Django Crash

CSCI 2133 Rapid Programming Techniques for Innovation A Python based framework Django Crash

CSCI 2133 Rapid Programming Techniques for Innovation A Python based framework Django Crash Lesson CSCI 2133 2 Previous Lecture Python Data Manipulation CSCI 2133 Agenda Django Overview Learn Django by examples

661 views • 50 slides
Micromorphic Crystal Plasticity Samuel Forest, Nicolas Cordero, Ana s Gaubert , Esteban

Micromorphic Crystal Plasticity Samuel Forest, Nicolas Cordero, Ana s Gaubert , Esteban

Micromorphic Crystal Plasticity Samuel Forest, Nicolas Cordero, Ana s Gaubert , Esteban Busso Mines ParisTech / CNRS Centre des Mat eriaux/UMR 7633 BP 87, 91003 Evry, France Samuel.Forest@mines-paristech.fr ONERA, 29, Av. de la

763 views • 60 slides
Non-browser TLS Woes Dan Boneh Joint work with M.

Non-browser TLS Woes Dan Boneh Joint work with M.

Non-browser TLS Woes Dan Boneh Joint work with M. Georgiev, S. Iyengar, S. Jana, R. Anubhai, and V. Shma?kov Proc. ACM CCS 2012 30

220 views • 18 slides
Edge Elements and Coercivity Ralf Hiptmair Seminar f ur Angewandte Mathematik ETH Z urich

Edge Elements and Coercivity Ralf Hiptmair Seminar f ur Angewandte Mathematik ETH Z urich

Edge Elements and Coercivity Ralf Hiptmair Seminar f ur Angewandte Mathematik ETH Z urich (email: hiptmair@sam.math.ethz.ch) (Homepage: http://www.sam.math.ethz.ch/ hiptmair) Sep 25-27, 2006 19th Chemnitz FEM Symposium Variational

398 views • 17 slides
Energy Equation 2 | u | 2 + , we have Recall that for H = p + 1 u t + (

Energy Equation 2 | u | 2 + , we have Recall that for H = p + 1 u t + (

Energy Equation 2 | u | 2 + , we have Recall that for H = p + 1 u t + ( u ) u = H . Taking scalar product with u and integrating over a fixed volume V , u t u + (

301 views • 6 slides

More recommend