'Kinetic energies' diaporamas de présentation

Rotational motion

Rotational motion. Chapter 9. Rigid objects. A rigid object has a perfectly definite and unchanging shape and size. In this class, we will approximate everything as a rigid object. Radians. In describing rotational motion, we will use angles in radians, not degrees. q in radians.

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Chapter 7: Quantum Theory and Atomic Structure

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CHAPTER 12 The Atomic Nucleus

CHAPTER 12 The Atomic Nucleus. 12.1 Discovery of the Neutron 12.2 Nuclear Properties 12.3 The Deuteron 12.4 Nuclear Forces 12.5 Nuclear Stability 12.6 Radioactive Decay 12.7 Alpha, Beta, and Gamma Decay 12.8 Radioactive Nuclides.

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Chapter 8

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An Introduction To The Health Effects of Radiation

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AGN Feedback at the Parsec Scale

AGN Feedback at the Parsec Scale. Feng Yuan Shanghai Astronomical Observatory, CAS. with: F. G. Xie (SHAO) J. P. Ostriker (Princeton University) M. Li (SHAO). OUTLINE. Intermittent activity of compact radio sources Outburst: 10^4 years Quiescent: 10^5 years

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Rotational Kinematics

Rotational Kinematics . Angular Position, Velocity, and Acceleration. Angular Position, Velocity, and Acceleration. Degrees and revolutions:. Angular Position, Velocity, and Acceleration. Arc length s , measured in radians:. 10-1 Angular Position, Velocity, and Acceleration.

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Quantum Theory

Quantum Theory. But if an electron acts as a wave when it is moving, WHAT IS WAVING ? When light acts as a wave when it is moving, we have identified the ELECTROMAGNETIC FIELD as waving. But try to recall: what is the electric field ? Can we directly measure it?.

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Systems of Particles

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Biomedical Applications of Particle Accelerators

Biomedical Applications of Particle Accelerators. Introduction to Accelerators Superconducting Magnets - MRI Hadron Therapy Radioactive Isotopes for Nuclear Medicine Synchrotron Light Sources The Future. Why Accelerate?.

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introduction to photoemission application to layered oxides

introduction to photoemission application to layered oxides. Amal Al- Wahish Course: Solid state 672 Prof. Dagotto Department of Physics, UTK. OutLine. What is the photoemission? Why we need it? Present a Historical Introduction ARPES and Mathematical Formulas Three-Step Model

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Simple Harmonic Motion

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Molecular Beam Epitaxy

Molecular Beam Epitaxy. 09/26/2008 MSE 576: Thin Films. Deepak Rajput. Graduate Research Assistant Center for Laser Applications Materials Science & Engineering University of Tennessee Space Institute Tullahoma, Tennessee 37388-9700 Email: drajput@utsi.edu Web: http://drajput.com.

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THE BALLISTIC PENDULUM

THE BALLISTIC PENDULUM. Students: Pedro N. Placido, Jr. Aziz Kenz. Ryan Ramnarine. SC 441H Spring 2002, Dr. Roman Kezerashvili. OBJECTIVES:. Study one-dimensional Inelastic Collision between two objects. Determine the Linear Momentum.

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Thin Film Growth

Thin Film Growth. Lecture 12 G.J. Mankey gmankey@mint.ua.edu. Factors Influencing Film Growth. Surface energy. Interfacial energy. Substrate temperature. Interface crystallography. Type of deposition source. Background gas. Surfactants.

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Chapter 6 Gases

Chapter 6 Gases. 6.1 Properties of Gases 6.2 Gas Pressure. Kinetic Theory of Gases. A gas consists of small particles that move rapidly in straight lines. have essentially no attractive (or repulsive) forces. are very far apart.

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Physics 2

Physics 2. Chapter 13 problems. Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.

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Basic Physics

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Review: Energy Changes, Rates of Reaction and Nuclear Energy

Review: Energy Changes, Rates of Reaction and Nuclear Energy. Questions 1 - 3. a) exothermic b) endothermic c) exothermic d) exothermic e) exothermic (in the forward direction) q = cm D T = 4.1796 J/g ? C x 500 g x 0.4 ? C = 835.92 J = 0. 8 3592 kJ

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RADIATION PROTECTION IN DIAGNOSTIC AND INTERVENTIONAL RADIOLOGY

IAEA Training Material on Radiation Protection in Diagnostic and Interventional Radiology. RADIATION PROTECTION IN DIAGNOSTIC AND INTERVENTIONAL RADIOLOGY. L 2: Radiation units and dose quantities. Introduction. Subject matter: the basic dosimetric quantities

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