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CHAPTER 4: ARRANGEMENT OF ELECTRONS IN ATOMS
CHAPTER 4: ARRANGEMENT OF ELECTRONS IN ATOMS

Chapter 8 Notes
Chapter 8 Notes

... There are two main factors effecting the amount of lattice energy. Lattice energy increases with decreasing ionic radii. This makes sense if you think about it. After-all the smaller the ion, the closer the positive nucleus is to the valence electrons responsible for bonding. So Magnesium compounds ...
CHEM 121
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... where R = 10 973 731.568 539 m and nlower and nupper are integers. b. What conclusion is drawn from the observation that the emission and absorption spectra of atoms are line spectra? Only certain energy levels must be available to the electrons in an atom. 13. What do we mean when we say that somet ...
Learning Goals
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... accepting both the totally non-intuitive quantum ideas, and an approach to understanding the physical world by the use of mathematical models that match experiment, and then figure out what math implies, rather than in the reverse order has had previously been used. You will confront this intellectu ...
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... 5. The limit voltage U0 is much bigger for violet than for yellow light. 6. The intensity of the light does not influence the limit voltage. With classical wave theory of light we would expect that the emission of electrons does not depend on the wavelength of the light. The photoelectric effect (an ...
SAMPLE midterm with solutions
SAMPLE midterm with solutions

... 7. Explain why the quantum Hall effect is robust. The quantum Hall effect is robust because it exists so long as there are edge states at opposite sides of the sample, which carry current in one direction only and are in separate equilibrium. The states on a single edge are chiral, that is, they pro ...
Activity 2 - hrsbstaff.ednet.ns.ca
Activity 2 - hrsbstaff.ednet.ns.ca

... (c) Each filter absorbs 96% of the photons. How many photons per second pass through after seven filters? (d) Compare the time taken by each photon to travel 0.30 m with the time between successive photons emerging from the final filter (assume the photons are equally spaced). Express your answer as ...
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... (c) What is the penetration length δ for the wave function in (b)? (Hint: the penetration length is the length at which the wave function is equal to 1/e.) (d) Compute the penetration length δ, using E = 1 eV, V0 = 1.1 eV, a = 0.1 nm, and me = 511 keV. (e) The transmission coefficient in this region ...
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... 103) Compare the elements Li, K, C, N a) Which has the largest atomic radius? K b) Place the elements in order of increasing ionization energy. K < Li < C < N 109) Which group of the periodic table has elements with high first ionization potentials and very negative electron affinities? Explain this ...
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... start out with de Broglie’s equation for momentum, because it is easy to see why only certain orbits are allowed. In de Broglie’s picture, we should treat the electrons as particle waves traveling in a circle around the nucleus. Each orbit, these waves return on themselves, and if they are not in ph ...
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... • Once two atoms exchange an electron, one is positively charged (lost the electron) and the other is negatively charged (gained the electron), the opposite charges attract forming an ionic bond • Ion: An atom or molecule that has gained or lost one or more electrons and has a negative or ...
Copyright © 2014 Edmentum - All rights reserved. AP Physics
Copyright © 2014 Edmentum - All rights reserved. AP Physics

... II. The energy of atomic oscillations occurs in exact multiples of a discrete unit. III. Electrons, atoms, and all particles with momentum also exist as waves. IV. No two electrons in an atom may have the same set of quantum numbers A. I-Heisenberg, II-Planck, III-de Broglie, IV-Pauli B. I-Planck, I ...
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... The orbital with the lowest (n + l) value is filled first. When two or more orbitals have the same (n + l) value, the one with the lowest ‘n’ value is preferred in filling. Consider two orbitals 3d and 4s. The n + l value of 3d = 3 + 2 = 5 and of 4s = 4 + 0 = 4. Since 4s has lowest (n + l) value, it ...
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X-ray photoelectron spectroscopy



X-ray photoelectron spectroscopy (XPS) is a surface-sensitive quantitative spectroscopic technique that measures the elemental composition at the parts per thousand range, empirical formula, chemical state and electronic state of the elements that exist within a material. XPS spectra are obtained by irradiating a material with a beam of X-rays while simultaneously measuring the kinetic energy and number of electrons that escape from the top 0 to 10 nm of the material being analyzed. XPS requires high vacuum (P ~ 10−8 millibar) or ultra-high vacuum (UHV; P < 10−9 millibar) conditions, although a current area of development is ambient-pressure XPS, in which samples are analyzed at pressures of a few tens of millibar.XPS is a surface chemical analysis technique that can be used to analyze the surface chemistry of a material in its as-received state, or after some treatment, for example: fracturing, cutting or scraping in air or UHV to expose the bulk chemistry, ion beam etching to clean off some or all of the surface contamination (with mild ion etching) or to intentionally expose deeper layers of the sample (with more extensive ion etching) in depth-profiling XPS, exposure to heat to study the changes due to heating, exposure to reactive gases or solutions, exposure to ion beam implant, exposure to ultraviolet light.XPS is also known as ESCA (Electron Spectroscopy for Chemical Analysis), an abbreviation introduced by Kai Siegbahn's research group to emphasize the chemical (rather than merely elemental) information that the technique provides.In principle XPS detects all elements. In practice, using typical laboratory-scale X-ray sources, XPS detects all elements with an atomic number (Z) of 3 (lithium) and above. It cannot easily detect hydrogen (Z = 1) or helium (Z = 2).Detection limits for most of the elements (on a modern instrument) are in the parts per thousand range. Detection limits of parts per million (ppm) are possible, but require special conditions: concentration at top surface or very long collection time (overnight).XPS is routinely used to analyze inorganic compounds, metal alloys, semiconductors, polymers, elements, catalysts, glasses, ceramics, paints, papers, inks, woods, plant parts, make-up, teeth, bones, medical implants, bio-materials, viscous oils, glues, ion-modified materials and many others.XPS is less routinely used to analyze the hydrated forms of some of the above materials by freezing the samples in their hydrated state in an ultra pure environment, and allowing or causing multilayers of ice to sublime away prior to analysis. Such hydrated XPS analysis allows hydrated sample structures, which may be different from vacuum-dehydrated sample structures, to be studied in their more relevant as-used hydrated structure. Many bio-materials such as hydrogels are examples of such samples.
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