'Quasi static' diaporamas de présentation

W.B.Mori UCLA F.S.Tsung CK. Huang V.K.Decyk D.Bruhwiler TechX D.Dimitrov E.Esarey LBNL

UCLA. SciDAC plasma-based team:. W.B.Mori UCLA F.S.Tsung CK. Huang V.K.Decyk D.Bruhwiler TechX D.Dimitrov E.Esarey LBNL B.Shadwick G.Fubiani T.Katsouleas USC S.Deng. Advanced accelerator effort is highly leveraged: Big bang for the buck. Why and what is plasma-based acceleration.

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W.B.Mori UCLA F.S.Tsung CK. Huang V.K.Decyk D.Bruhwiler TechX D.Dimitrov E.Esarey LBNL

UCLA. SciDAC plasma-based team:. W.B.Mori UCLA F.S.Tsung CK. Huang V.K.Decyk D.Bruhwiler TechX D.Dimitrov E.Esarey LBNL B.Shadwick G.Fubiani T.Katsouleas USC S.Deng. Advanced accelerator effort is highly leveraged: Big bang for the buck. Why and what is plasma-based acceleration.

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??????. ??? 10/13/2005. Design Considerations Environmental Loads Configuration Design Structure Analysis Design Verification Contest Problem #1 Homework Problems. Design Considerations. Structure exists everyplace in our life; building, bridge, car,

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Lecture 9 Heat Engines

Thermodynamic processes and entropy Thermodynamic cycles Extracting work from heat How do we define engine efficiency? Carnot cycle --- best possible. Reference for Lect. 10: Elements Ch 10. References for this Lecture: Elements Ch 4D-F. Lecture 9 Heat Engines.

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Chengkun Huang UCLA

Quasi-static modeling of beam/laser plasma interactions for particle acceleration. Chengkun Huang UCLA. Zhejiang University 07/14/2009. Collaborations. V. K. Decyk, M. Zhou, W. Lu, M. Tzoufras, W. B. Mori, K. A. Marsh, C. E. Clayton, C. Joshi

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Separation of Scales in Wave - Particle Interactions

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Separation of Scales in Wave - Particle Interactions

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Valentin Pricop

Valentin Pricop. PhD review. Introduction. Development of advanced methods for the measurement of soft magnetic material characteristic. The ramping rate of normal conducting particle accelerator magnets is usually in the order of 1 T/s.

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Lecture 13 Heat Engines

? Thermodynamic processes and entropy ? Thermodynamic cycles ? Extracting work from heat - How do we define engine efficiency? - Carnot cycle: the best possible efficiency. Lecture 13 Heat Engines. Reading for this Lecture: Elements Ch 4D-F. Reading for Lecture 14: Elements Ch 10.

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Chapter 4 Macroscopic Parameters & Their Measurement

Chapter 4 Macroscopic Parameters & Their Measurement. The Laws of Thermodynamics: Overview. 0 th Law : Defines Temperature ( T ) 1 st Law : Defines Energy (Internal Energy ? & Mechanical Work W ) 2 nd Law : Defines Entropy ( S )

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Chapter 2

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Self-Consistent Simulations of the Interaction of Electron-Clouds and Beams with WARP-POSINST

Self-Consistent Simulations of the Interaction of Electron-Clouds and Beams with WARP-POSINST. Jean-Luc Vay Lawrence Berkeley National Laboratory Heavy Ion Fusion Science Virtual National Laboratory E-cloud 07, 9-12 April 2007, Daegu, Korea. Collaborators.

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Lecture 8. Thermodynamic Identities (Ch. 3)

Lecture 8. Thermodynamic Identities (Ch. 3).

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Coronal Heating of an Active Region Observed by XRT on May 5, 2010

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Work and heat

Work and heat. When an object is heated and its volume is allowed to expand, then work is done by the object and the amount of work done depends generally on the pressure ( P ) and change of volume ( ? V ).

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Granular flows confined between flat, frictional walls

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Three Regions of Auroral Acceleration

Three Regions of Auroral Acceleration.

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Abstract

Abstract. We simulate the twisting of an initially potential coronal flux tube by photospheric vortex motions. The flux tube starts to evolve slowly(quasi-statically) and possess helical shape. There exists a critical twist, above which the flux tube would be observed as an eruption.

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Systems Problem 4 Lecture Notes

payload. Systems Problem 4 Lecture Notes. Learning objectives. After completing this SP4 and SP5 you will have: Applied material from 8.01, (Unified thermodynamics) and Unified fluid mechanics to develop a model for a single stage water rocket

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HIGH-STRAIN-RATE BEHAVIOR OF POLYCRYSTALLINE a -IRON

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