Lecture Two
... perturbation from the k=0 state, the energy correction is Dijkikj= <|kipi|><|kjpj|>/[E-E] In a magnetic field, k is replaced p-eA/c. The equation for u becomes H’u=Eu; H’= Dij(pi-eAi/c)(pj-eAj/c)-B¢ B). Since A=r£ B/2, the Dij term also contains a contribution proportional to B. ...
... perturbation from the k=0 state, the energy correction is Dijkikj= <|kipi|><|kjpj|>/[E-E] In a magnetic field, k is replaced p-eA/c. The equation for u becomes H’u=Eu; H’= Dij(pi-eAi/c)(pj-eAj/c)-B¢ B). Since A=r£ B/2, the Dij term also contains a contribution proportional to B. ...
Nanomaterials
... Small (d<<λ) metal particles exhibit a phenomenon called plasma resonance, i.e. plasma-polariton resonance of the free electrons in the metal surface. A resonant metal particle can capture light over a region of many wavelengths in dimension even if the particle itself is only a fraction of a wavele ...
... Small (d<<λ) metal particles exhibit a phenomenon called plasma resonance, i.e. plasma-polariton resonance of the free electrons in the metal surface. A resonant metal particle can capture light over a region of many wavelengths in dimension even if the particle itself is only a fraction of a wavele ...
Fields/Forces
... During all charging processes, the total charge before the process equals the total charge after the process. Conductors are substances that have electrons free to move. Insulators have electrons involved in chemical bonds and are not free to move. The magnitude of the force between two electric cha ...
... During all charging processes, the total charge before the process equals the total charge after the process. Conductors are substances that have electrons free to move. Insulators have electrons involved in chemical bonds and are not free to move. The magnitude of the force between two electric cha ...
Practice Exams II
... Please enter your last name and university ID number on the optically scanned answer sheet. Fill in the circles darkly. Also sign your name in the space provided at right. Before you begin the exam, fill in the ID information requested on all pages of the solution papers. Directions: The exam consis ...
... Please enter your last name and university ID number on the optically scanned answer sheet. Fill in the circles darkly. Also sign your name in the space provided at right. Before you begin the exam, fill in the ID information requested on all pages of the solution papers. Directions: The exam consis ...
7. Magnetic Fields
... 1. To familiarize your self with the magnitude of the magnetic field expected in this experiment, measure the diameter of the coil, count the number of turns, and calculate the magnetic field strength at the center assuming a 100mA current running in the coil. Express your answer in µT. 2. Set up a ...
... 1. To familiarize your self with the magnitude of the magnetic field expected in this experiment, measure the diameter of the coil, count the number of turns, and calculate the magnetic field strength at the center assuming a 100mA current running in the coil. Express your answer in µT. 2. Set up a ...
Handout Topic 5 and 10 -11 NEW Selected Problems 3
... Diagram 1 below shows two long, parallel vertical wires each carrying equal currents in the same direction. The wires pass through a horizontal sheet of card. Diagram 2 shows a plan view of the wires looking down onto the card. ...
... Diagram 1 below shows two long, parallel vertical wires each carrying equal currents in the same direction. The wires pass through a horizontal sheet of card. Diagram 2 shows a plan view of the wires looking down onto the card. ...
Superconductivity
Superconductivity is a phenomenon of exactly zero electrical resistance and expulsion of magnetic fields occurring in certain materials when cooled below a characteristic critical temperature. It was discovered by Dutch physicist Heike Kamerlingh Onnes on April 8, 1911 in Leiden. Like ferromagnetism and atomic spectral lines, superconductivity is a quantum mechanical phenomenon. It is characterized by the Meissner effect, the complete ejection of magnetic field lines from the interior of the superconductor as it transitions into the superconducting state. The occurrence of the Meissner effect indicates that superconductivity cannot be understood simply as the idealization of perfect conductivity in classical physics.The electrical resistivity of a metallic conductor decreases gradually as temperature is lowered. In ordinary conductors, such as copper or silver, this decrease is limited by impurities and other defects. Even near absolute zero, a real sample of a normal conductor shows some resistance. In a superconductor, the resistance drops abruptly to zero when the material is cooled below its critical temperature. An electric current flowing through a loop of superconducting wire can persist indefinitely with no power source.In 1986, it was discovered that some cuprate-perovskite ceramic materials have a critical temperature above 90 K (−183 °C). Such a high transition temperature is theoretically impossible for a conventional superconductor, leading the materials to be termed high-temperature superconductors. Liquid nitrogen boils at 77 K, and superconduction at higher temperatures than this facilitates many experiments and applications that are less practical at lower temperatures.