Physics
... between two point charges, forces between multiple charges; superposition principle and continuous charge distribution. Electric field, electric field due to a point charge, electric field lines, electric dipole, electric field due to a dipole, torque on a dipole in uniform electric field. Electric ...
... between two point charges, forces between multiple charges; superposition principle and continuous charge distribution. Electric field, electric field due to a point charge, electric field lines, electric dipole, electric field due to a dipole, torque on a dipole in uniform electric field. Electric ...
Magnetism, Electromagnetism, & Electromagnetic Induction
... Magnetic Field around a current-carrying wires • A current moving through a wire creates a magnetic field around that wire. • The magnetic field forms concentric circles around the wire. • Use the right hand rule shown to predict the direction of the field. ...
... Magnetic Field around a current-carrying wires • A current moving through a wire creates a magnetic field around that wire. • The magnetic field forms concentric circles around the wire. • Use the right hand rule shown to predict the direction of the field. ...
phy_1304 - WordPress.com
... (b)Are these surfaces equidistant from each other ? If not , explain why. OR A test charge q is moved without acceleration from A to C along the path from A to B and then from B to C in electric field where the co-ordinates of points A , B and C are (2, -1) (-2 , 2) , (-2, -1 ) respectively . calcul ...
... (b)Are these surfaces equidistant from each other ? If not , explain why. OR A test charge q is moved without acceleration from A to C along the path from A to B and then from B to C in electric field where the co-ordinates of points A , B and C are (2, -1) (-2 , 2) , (-2, -1 ) respectively . calcul ...
CHAPTER 21 ELECTROMAGNETIC INDUCTION
... How much work to bring current through inductor from zero to 0? To calculate the work integrate from zero current to current I ...
... How much work to bring current through inductor from zero to 0? To calculate the work integrate from zero current to current I ...
Syllabus_APHY112
... Electric potential: Electric potential and electric field, Potential difference and electric potential, Potential differences in a uniform electric field, Electric potential and potential energy due to point charges Capacitance and Dielectrics: Capacitance, Combinations of capacitors, dielectrics, c ...
... Electric potential: Electric potential and electric field, Potential difference and electric potential, Potential differences in a uniform electric field, Electric potential and potential energy due to point charges Capacitance and Dielectrics: Capacitance, Combinations of capacitors, dielectrics, c ...
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.