'Body forces' diaporamas de présentation

AOSS 401, Fall 2013 Lecture 2 Forces September 5 , 2013

AOSS 401, Fall 2013 Lecture 2 Forces September 5 , 2013. Richard B. Rood (Room 2525, SRB) rbrood@umich.edu 734-647-3530 Cell: 301-526-8572. Class News. Ctools site ( AOSS 401 001 F13 ) Syllabus Lectures Homework (and solutions) New Postings to site Homework 1: Due September 12

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Continuity Equation

Continuity Equation. Continuity Equation. Net outflow in x direction. Continuity Equation. net out flow in y direction,. Continuity Equation. Net out flow in z direction. Net mass flow out of the element. Continuity Equation. Time rate of mass decrease in the element.

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What have we learned about three-nucleon forces at intermediate energies?

What have we learned about three-nucleon forces at intermediate energies?. Nasser Kalantar-Nayestanaki Kernfysisch Versneller Instituut, RuG Strong interactions: From methods to structures February 14, 2011. Three-body forces and Wikipedia.

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What have we learned about three-nucleon systems at intermediate energies?

What have we learned about three-nucleon systems at intermediate energies?. Nasser Kalantar-Nayestanaki Kernfysisch Versneller Instituut (KVI), Univ. Of Groningen 18th International Symposium on Spin Physics (SPIN 2008) Charlottesville, Virginia, October 6, 2008. Nijmegen I Nijmegen II

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What have we learned about three-nucleon systems at intermediate energies?

What have we learned about three-nucleon systems at intermediate energies?. Nasser Kalantar-Nayestanaki Kernfysisch Versneller Instituut (KVI), Univ. Of Groningen 18th International Symposium on Spin Physics (SPIN 2008) Charlottesville, Virginia, October 6, 2008. Nijmegen I Nijmegen II

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R. Machleidt, University of Idaho

The explosion of chiral many-body forces: How to deal with it?. R. Machleidt, University of Idaho. Outline. Nuclear forces from chiral EFT: Basic ideas and overview Two-nucleon forces (2NF) Three-nucleon forces (3NF ) H igher orders: The explosion of contributions Conclusions.

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AOSS 321, Winter 2009 Earth System Dynamics Lecture 6 & 7 1/27/2009 1/29/2009

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Nuclear Force General principles Examples: quantitative

Nuclear structure III (theory) Witek Nazarewicz (UTK/ ORNL ) National Nuclear Physics Summer School 2014 William & Mary, VA. Nuclear Force General principles Examples: quantitative nuclear theory; p redictive capability Realities of high-performance computing. The Force.

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Reynolds Transport Theorem for Fluid Flows

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MEEN 5330 Continuum Mechanics , all references from Continuum Mechanics by Frederick & Chang unless noted

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Modeling Turbulent Flows

Modeling Turbulent Flows. What is Turbulence?. Unsteady, irregular (aperiodic) motion in which transported quantities (mass, momentum, scalar species) fluctuate in time and space Identifiable swirling patterns characterizes turbulent eddies.

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Low-momentum interactions for nuclei

Low-momentum interactions for nuclei. Achim Schwenk Indiana University Nuclear Forces and the Quantum Many-Body Problem Institute for Nuclear Theory, Oct. 7, 2004 with Scott Bogner, Tom Kuo and Andreas Nogga supported by DOE and NSF. Introduction and motivation

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Introduction to Strength of Materials

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EQUILIBRIUM OF A RIGID BODY & FREE-BODY DIAGRAMS

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Brian J. Kirby, PhD Sibley School of Mechanical and Aerospace Engineering, Cornell University, Ithaca, NY

Powerpoint Slides to Accompany Micro- and Nanoscale Fluid Mechanics: Transport in Microfluidic Devices . Chapter 6. Brian J. Kirby, PhD Sibley School of Mechanical and Aerospace Engineering, Cornell University, Ithaca, NY. Ch 6 : Electroosmosis.

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Application of the Momentum Equation We will consider the following examples:

Application of the Momentum Equation We will consider the following examples: 1. Force due to the flow of fluid round a pipe bend. 2. Force on a nozzle at the outlet of a pipe. 3. Impact of a jet on an inclined plane surface. 4. Force due to flow round a curved vane.

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Force due to a jet hitting an inclined plane

Force due to a jet hitting an inclined plane. We want to find the reaction force normal to the plate so we choose the axis system as above so that is normal to the plane. The diagram may be rotated to align it with these axes and help comprehension, as shown below Rotated.

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Chapter 6 Strain Energy and Related Principles

T n. F. Work Done by Surface and Body Forces on Elastic Solids Is Stored Inside the Body in the Form of Strain Energy. Chapter 6 Strain Energy and Related Principles. U. Elasticity Theory, Applications and Numerics M.H. Sadd , University of Rhode Island. ?. y. ?. dy. ?. dz. dx.

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Chapter 6 Strain Energy and Related Principles

T n. F. Work Done by Surface and Body Forces on Elastic Solids Is Stored Inside the Body in the Form of Strain Energy. Chapter 6 Strain Energy and Related Principles. U. Elasticity Theory, Applications and Numerics M.H. Sadd , University of Rhode Island. ?. y. ?. dy. ?. dz. dx.

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Chapter 6 Strain Energy and Related Principles

T n. F. Work Done by Surface and Body Forces on Elastic Solids Is Stored Inside the Body in the Form of Strain Energy. Chapter 6 Strain Energy and Related Principles. U. ?. y. ?. dy. ?. dz. dx. ? x. u. x. U = Area Under Curve. z. e. e x. Uniaxial Extensional Deformation.

224 views • 9 slides