Vacation Packet - Manhasset Schools
... ii. Calculate the minimum thickness of the film for which the intensity of the reflected red ray is near zero. ...
... ii. Calculate the minimum thickness of the film for which the intensity of the reflected red ray is near zero. ...
Electricity and Magnetism
... repel other magnets. They can also attract pieces of iron that are not magnetic (magNEH-tick). These pieces of iron will become magnetized (MAG-nuh-tized), or made into magnets. Every magnet has two ends called poles. These poles are called north and south. Poles behave like electrical charges in ma ...
... repel other magnets. They can also attract pieces of iron that are not magnetic (magNEH-tick). These pieces of iron will become magnetized (MAG-nuh-tized), or made into magnets. Every magnet has two ends called poles. These poles are called north and south. Poles behave like electrical charges in ma ...
Lecture 14
... E-M Cannon • Connect solenoid to a source of alternating voltage. • The flux through the area ^ to axis of solenoid therefore changes in time. • A conducting ring placed on top of the solenoid will have a current induced in it opposing this change. • There will then be a force on the ring since it c ...
... E-M Cannon • Connect solenoid to a source of alternating voltage. • The flux through the area ^ to axis of solenoid therefore changes in time. • A conducting ring placed on top of the solenoid will have a current induced in it opposing this change. • There will then be a force on the ring since it c ...
CTFinal
... A charge q is released from rest at point in empty space were there may be E- and/or B-fields. There are no forces on the charge except for the forces due to the E and/or Bfields (no gravity, etc.). The charge is observed for a short while and is seen to move along a curved path. Which one statement ...
... A charge q is released from rest at point in empty space were there may be E- and/or B-fields. There are no forces on the charge except for the forces due to the E and/or Bfields (no gravity, etc.). The charge is observed for a short while and is seen to move along a curved path. Which one statement ...
SUMMARY
... (Section 19.8) When a capacitor is charged by a battery in series with a resistor, the current and capacitor charge are not constant. The charge varies with time as q 5 Qfinal 1 1 2 e 2t/RC 2 (Equation 19.17). In a time t 5 RC, there is a significant change in the charge on the capacitor. This time ...
... (Section 19.8) When a capacitor is charged by a battery in series with a resistor, the current and capacitor charge are not constant. The charge varies with time as q 5 Qfinal 1 1 2 e 2t/RC 2 (Equation 19.17). In a time t 5 RC, there is a significant change in the charge on the capacitor. This time ...
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.