Question Sheet - Manchester HEP
... energy of particle c is given by Ec* (W 2 mc2 md2 ) / 2W where W is the total centre of mass energy. What is the corresponding expression for the centre of mass energy of particle d? 10. Show that the invariant mass of a pair of photons of energies, E1 , E2 with angle between their direction ...
... energy of particle c is given by Ec* (W 2 mc2 md2 ) / 2W where W is the total centre of mass energy. What is the corresponding expression for the centre of mass energy of particle d? 10. Show that the invariant mass of a pair of photons of energies, E1 , E2 with angle between their direction ...
Fall Exam 1
... showed that an electron could have C. demonstrated the existence of more than one charge. neutrons. B. proved that Thomson’s “plum D. determined the charge on a single pudding” model of the atom’s electron. structure was correct. 19. Nobel prize winner Ernest Rutherford conducted an experiment with ...
... showed that an electron could have C. demonstrated the existence of more than one charge. neutrons. B. proved that Thomson’s “plum D. determined the charge on a single pudding” model of the atom’s electron. structure was correct. 19. Nobel prize winner Ernest Rutherford conducted an experiment with ...
Physical Chemistry 20130517 week 7 Friday May 17 2013
... two masses is r. The angle between the z axis and the radius r is θ. Project r down onto the xy plane gives a vector with length rsinθ. The angle between the x axis and the vector rsinθ is φ. Given that, we know: x=rsinθcosφ ...
... two masses is r. The angle between the z axis and the radius r is θ. Project r down onto the xy plane gives a vector with length rsinθ. The angle between the x axis and the vector rsinθ is φ. Given that, we know: x=rsinθcosφ ...
Electronic structure and spectroscopy
... momentum only. Assume that E = 0, than p = 0, therefore ∆x = ∞, which is a contradiction since ∆x ≤ L, the particle must be in the box. We conclude that the energy can never get zero, since in this case its uncertainty would also be zero which is possible only for very large box where the uncertaint ...
... momentum only. Assume that E = 0, than p = 0, therefore ∆x = ∞, which is a contradiction since ∆x ≤ L, the particle must be in the box. We conclude that the energy can never get zero, since in this case its uncertainty would also be zero which is possible only for very large box where the uncertaint ...
Name: Date: Chemistry 1 – Midterm Review Sheet Unit 1 – Scientific
... 3. The energy levels of the hydrogen atom (and all atoms) are ______________, meaning that only certain discrete energy levels are allowed. a. varied b. quantized c. ramp-like d. continuous e. two of these 4. The form of EMR that has less energy than microwaves is a. microwaves b. radio waves c. ga ...
... 3. The energy levels of the hydrogen atom (and all atoms) are ______________, meaning that only certain discrete energy levels are allowed. a. varied b. quantized c. ramp-like d. continuous e. two of these 4. The form of EMR that has less energy than microwaves is a. microwaves b. radio waves c. ga ...
photoelectric-effect-qrg
... 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 ...
... 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 ...
Problems and Questions on Lecture 2 Useful equations and
... What is the frequency of the emitted photon if an electron makes a transition from the n = 3 level to the n = 2 level? What is the wavelength of the photon for the same transition? Would the emitted photon be visible? ...
... What is the frequency of the emitted photon if an electron makes a transition from the n = 3 level to the n = 2 level? What is the wavelength of the photon for the same transition? Would the emitted photon be visible? ...
chapter 6 sec 2 resonance structure
... H is 2.1 and O is 3.5. 3.5 – 2.1 = 1.4 so the bond between H and O is a polar covalent bond. By definition a neutral group of atoms held together by covalent bonds is a molecule. So, the H2O particle is a molecule H2O is a molecule which makes H2O a molecular compound and a molecular formula. But H2 ...
... H is 2.1 and O is 3.5. 3.5 – 2.1 = 1.4 so the bond between H and O is a polar covalent bond. By definition a neutral group of atoms held together by covalent bonds is a molecule. So, the H2O particle is a molecule H2O is a molecule which makes H2O a molecular compound and a molecular formula. But H2 ...
TEST REVIEW S Valence Electrons TEST REVIEW SHEET 2017
... NOTE: If an element has <4 valence electrons it will give them away during an ionic bond and become a positive ion. If >4, it will take them and become a negative ion For the most part…. metals will give away their valence electrons and nonmetals will take enough valence electrons to fill their oute ...
... NOTE: If an element has <4 valence electrons it will give them away during an ionic bond and become a positive ion. If >4, it will take them and become a negative ion For the most part…. metals will give away their valence electrons and nonmetals will take enough valence electrons to fill their oute ...
HMWK 7
... P29.36. Prepare: Figure P29.36 shows the ground state (with a large number of allowed states) and an excited state (with a large number of allowed states) for a molecule. Even though the ground state has a large number of allowed energy levels, nearly all molecules spend nearly all their time in the ...
... P29.36. Prepare: Figure P29.36 shows the ground state (with a large number of allowed states) and an excited state (with a large number of allowed states) for a molecule. Even though the ground state has a large number of allowed energy levels, nearly all molecules spend nearly all their time in the ...
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.