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Grade 12 Unit 9 - Amazon Web Services
Grade 12 Unit 9 - Amazon Web Services

... explains why waves are not observed for large objects. The momentum must be small compared to h for the wavelength to be appreciable. Particles at times have the properties of a wave; at other times they exhibit the properties of a particle. As in the case of electromagnetic radiation, the particle ...
Sections 4 - Columbia Physics
Sections 4 - Columbia Physics

... The value j = ½ is obtained from l = 0,1. There are two terms. The value j =  is obtained from l = 1 only (one term here). There are also two matrix elements: ...
Topic 4 Part 1 Review Questions student 2015
Topic 4 Part 1 Review Questions student 2015

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QUANTUM NUMBERS
QUANTUM NUMBERS

... The Bohr model of the atom was based on the line spectra of the Hydrogen atom. The model also incorporated the concept developed by Einstein regarding the particle behaviour of light during emission or absorption (photon or quanta of energy). Postulates: 1. Energy Levels  an electron can only have ...
Simulation of a High Energy Detector
Simulation of a High Energy Detector

... The Magnetic Spectrometer consists of 10 drift chambers inside a uniform magnetic field. A chamber dimensions are 3×62×60 cm3 and the distance between two chambers is 8 cm. It consists of two planes of 5 anode and 6 cathode wires made of tungsten with a thickness of 100 µm and 30 µm respectively. Th ...
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Experimental nonlocal and surreal Bohmian trajectories
Experimental nonlocal and surreal Bohmian trajectories

... its own Bohmian degrees of freedom. Although a single particle’s trajectory cannot be directly observed, a set of trajectories of an ensemble of particles can be mapped out. This can be done by making a so-called weak measurement of the momentum of a particle at a given instant in time. The weakness ...
Solution 1: mg=GMm/r2, so GM=gR2. At the equator, mV2/R=GMm
Solution 1: mg=GMm/r2, so GM=gR2. At the equator, mV2/R=GMm

... For small oscillations, let x = -a + x', where x' << a. Then the equation of motion is: m d2x/dt2 = - cx'(2a-x')/[(x'-a)2 + a2]2 ≈ - cx'/2a3 . So, T = 2π/ω = 2π √(2ma3/c) = 2πa √(2ma/c). b) Starting at x = -a, the total energy of the particle is: E=mv2/2 + V(-a) = mv2/2 – c/2a. 1) For confinement, E ...
Fulltext PDF
Fulltext PDF

... Some concepts essential to CP are discarded in QP, e.g., the idea of the trajectory itself is no longer meaningful in QP. Concepts that are completely different in CP come together in QP, e.g., wave and particle. Some concepts become much deeper in QP, such as the principle of linear superposition. ...
PPT
PPT

... The differential equation that describes the HO is too difficult for us to solve here. Here are the important features of the ...
Classical Dynamics - Department of Theoretical Physics
Classical Dynamics - Department of Theoretical Physics

... The fundamental principles of classical mechanics were laid down by Galileo and Newton in the 16th and 17th centuries. In 1686, Newton wrote the Principia where he gave us three laws of motion, one law of gravity and pretended he didn’t know calculus. Probably the single greatest scientific achievem ...
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n - Valdosta State University

Optics, Light and Lasers: The Practical Approach to RIAO/OPTILAS
Optics, Light and Lasers: The Practical Approach to RIAO/OPTILAS

... state nanostructures. One of the major goals of the book is to introduce the reader to this topic from an experimental point of view. The authors take great pains to motivate and explain illustrative experiments in mesoscopic transport and the underlying physical principles. This is very helpful and ...
Einstein`s Postulate of Relaavity
Einstein`s Postulate of Relaavity

Matter and antimatter: very similar, but not exactly - Physik
Matter and antimatter: very similar, but not exactly - Physik

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Wave and Particle Properties of Light Video Script

... It’s a relief to have a solution. All that arguing with myself was exhausting. So now that we know more about the nature of light, let’s talk about sources of light. We’ll start with the sun and the moon. They both look like they give off light, but one does and the other does not. Better get this i ...
Lecture 10
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... You need to know three things at this point: 1. Every allowed electron state has a unique Ψ 2. Specific Ψ’s are called orbitals 3. An orbital is NOT the same as a Bohr orbit ...
Conservation Laws
Conservation Laws

... (LVe will also make the stronger assumption that ...
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wall_summer_2011_poster

... observed. The normal Zeeman effect was discovered and explained in 1896 by Pieter Zeeman, but it took until 1925 for a theory that could explain the anomalous Zeeman effect. This theory stated that electrons have intrinsic angular momentum, called spin. The spin of the electron contributes to the ma ...
Animator Help Session
Animator Help Session

... Interpolating splines are cool because keyframing the parameter values that you want is more intuitive… But what about the time instances not keyed? Without control of curve tension, you may not get the parameter values that you would really like, and your animation could suffer ...
Quantum Imaging I
Quantum Imaging I

... ∫obj dρo |t(ρo)|2 |somb (R/so 2/ |ρo + ρi/m|)|2 Incoherent somb(x) = 2J1(x) / x  “point-spread function” (resolution) The resolution is constrained by the Rayleigh diffraction limit: /2 !!! ...
Lecture 18_Anal_Tech_Part1
Lecture 18_Anal_Tech_Part1

... The Hard Part - Interpreting Spectra Learning how an NMR machine works is straightforward. What is less straightforward is learning how to use the data we get from an NMR machine. That’s because each NMR spectrum is a puzzle, and there’s no single fact that you simply have to memorize to solve thes ...
Name: ENVR 373 Methods in Microscopy Lab Assignment: Electron
Name: ENVR 373 Methods in Microscopy Lab Assignment: Electron

NEWTON`S SECOND LAW FROM QUANTUM PHYSICS
NEWTON`S SECOND LAW FROM QUANTUM PHYSICS

... One would expect that for a free packet or for one in a constant force field, where classical mechanics holds, the right hand side of Eq. (2) would be ...
Quantum systems in one-dimension and quantum transport
Quantum systems in one-dimension and quantum transport

... IPCMS – Institut de Physique et Chimie des Matériaux de Strasbourg Quantum systems confined to low dimensions, such as spin chains, carbon nanotubes or cold atoms in optical lattices, often behave in a universal way that is efficiently described in terms of simple effective theories. These introduct ...
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Double-slit experiment

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