'2 2m' presentation slideshows

Unit 8: Linear Momentum

What is implied?. Unit 8: Linear Momentum. Work on Unit 8 HW asap Demos: Collision carts and track U7b: All students get perfect Score - answers online. Agenda. Review Dynamics for exam Operational Definitions momentum units Momentum Motion Map Elastic and Inelastic Collisions

931 views • 73 slides

Quantum Confinement

2.65k views • 57 slides

ECE 802-604: Nanoelectronics

ECE 802-604: Nanoelectronics. Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University ayresv@msu.edu. Lecture 04, 10 Sep 13. In Chapter 01 in Datta: Two dimensional electron gas (2-DEG) DEG goes down, mobility goes up Define mobility

596 views • 50 slides

Non-Exponential Two-Body Beta Decay of Stored Hydrogen-Like Ions

568 views • 43 slides

The Use of Dispersion Relations in Hard Exclusive Processes

The Use of Dispersion Relations in Hard Exclusive Processes. Gary R. Goldstein Tufts University Simonetta Liuti University of Virginia Presentation for Hard Meson and Photon Production ECT* Oct, 2010. Titian (1543)- Pope Paul III presided over Council of Trent. 10/14/2010.

450 views • 37 slides

Observation of non-exponential orbital electron-capture

Observation of non-exponential orbital electron-capture decay of hydrogen-like 140 Pr and 142 Pm ions. Yuri Litvinov, GSI Darmstadt, Germany, for the SMS-Collaboration. Bound-state beta decay first observed at GSI fifteen years ago ?. Outline.

447 views • 32 slides

? 5-1 ??????????????????? ?? ?????? t = 0 ? x o = 0 ? v o = 0 ?

? 5-1 ??????????????????? ?? ?????? t = 0 ? x o = 0 ? v o = 0 ? ????? a = F/m ? v =at ? x = at 2 /2. ????. 1 ???. t ? ? ? v ? c ? P = F t ? ?. v. x. v = Ft/m o. x = Ft 2 /2m o. c. x = ct - m o c 2 /F. o. t. t. o. 2 ???.

418 views • 29 slides

Quantum Confinement BW, Chs. 15-18, YC, Ch. 9; S, Ch. 14; outside sources

Quantum Confinement BW, Chs. 15-18, YC, Ch. 9; S, Ch. 14; outside sources. Overview of Quantum Confinement. Brief History In 1970 Esaki & Tsu proposed fabrication of an artificial structure, which would consist of alternating layers of 2 different semiconductors with Layer Thicknesses

493 views • 28 slides

442 views • 27 slides

EE 5340 Semiconductor Device Theory Lecture 2 - Fall 2010

EE 5340 Semiconductor Device Theory Lecture 2 - Fall 2010. Professor Ronald L. Carter ronc@uta.edu http://www.uta.edu/ronc. Quantum Concepts. Bohr Atom Light Quanta (particle-like waves) Wave-like properties of particles Wave-Particle Duality. Wave-particle duality.

304 views • 20 slides

Physics 101: Lecture 12 2D Collisions and Center of mass

424 views • 18 slides

Jack Simons , Henry Eyring Scientist and Professor Chemistry Department University of Utah

287 views • 15 slides

The physics of electron backscatter diffraction Maarten Vos

The physics of electron backscatter diffraction Maarten Vos AMPL, RSPHYSSE, Australian National University, Acton 0200, Canberra Aimo Winkelmann Max Planck Institute for Microstructure Physics, Halle, Germany. We are here (John Curtin Medical School). Our Laboratory

270 views • 14 slides

? 2 ?? ??????

302 views • 13 slides

Lecture 4: Diffraction

Lecture 4: Diffraction. PHYS 430/603 material Laszlo Takacs UMBC Department of Physics. How to determine the atomic structure of materials?.

274 views • 12 slides

Zero-point Energy

Zero-point Energy. Minimum energy corresponds to n=1 n=0 => ? n (x)=0 for all x => P(x)=0 => no electron in the well zero-point energy never at rest!

927 views • 12 slides

Introduction to relativistic kinematics and the concept of mass

245 views • 8 slides

The Variational Principle

The Variational Principle. Scott Riggs. Expectation Values. Basic Statistics P ab = ? p(x) dx (limits a to b) The probability that x lies between a & b Where p(x) dx is the probability that individual (randomly chosen) lies between x and x+dx

464 views • 7 slides

234 views • 4 slides

210 views • 1 slides