Electromagnetism 2 - K
... magnetic field does not exert a force on a current moving parallel to the direction of the magnetic field. (This would make sinθ = 0 in our formula, cancelling the force out). The magnetic force is greatest when the current moves perpendicular to the magnetic field. (sinθ = 1). ...
... magnetic field does not exert a force on a current moving parallel to the direction of the magnetic field. (This would make sinθ = 0 in our formula, cancelling the force out). The magnetic force is greatest when the current moves perpendicular to the magnetic field. (sinθ = 1). ...
Currents and Magnetism
... A long straight wire is carrying current from left to right. Near the wire is a charge q with velocity v v v ...
... A long straight wire is carrying current from left to right. Near the wire is a charge q with velocity v v v ...
Particle detectors measuring fluxes of cosmic rays on Earth´s surface.
... In this mechanism, avalanches of runaway electrons emit bremsstrahlung x rays that may either Compton backscatter or pair produce in the gas medium. If the backscattered photons propagate to the start of the avalanche region and produce another runaway electron, either via Compton scattering or phot ...
... In this mechanism, avalanches of runaway electrons emit bremsstrahlung x rays that may either Compton backscatter or pair produce in the gas medium. If the backscattered photons propagate to the start of the avalanche region and produce another runaway electron, either via Compton scattering or phot ...
sample paper i - Outlaw Online
... 20. A charge Q located at a point is in equilibrium under the combined electric field of three charges q1,q2, q3. If the charges q1, q2 are located at points and respectively, find the direction of the force on Q, due to q3 in terms of q1,q2, . 3 21. 12 cells, each of emf 1.5V and internal resistanc ...
... 20. A charge Q located at a point is in equilibrium under the combined electric field of three charges q1,q2, q3. If the charges q1, q2 are located at points and respectively, find the direction of the force on Q, due to q3 in terms of q1,q2, . 3 21. 12 cells, each of emf 1.5V and internal resistanc ...
Final Paper - University of Calgary
... concerning DC circuit problems (Planinic, et al., 2006). Despite their acquaintance, however, they have been found to possess stronger alternative conceptions in mechanics as well. Therefore, when teaching electricity, it is suggested to start by introducing key terms and their relations, followed b ...
... concerning DC circuit problems (Planinic, et al., 2006). Despite their acquaintance, however, they have been found to possess stronger alternative conceptions in mechanics as well. Therefore, when teaching electricity, it is suggested to start by introducing key terms and their relations, followed b ...
Electrostatics
Electrostatics is a branch of physics that deals with the phenomena and properties of stationary or slow-moving electric charges with no acceleration.Since classical physics, it has been known that some materials such as amber attract lightweight particles after rubbing. The Greek word for amber, ήλεκτρον electron, was the source of the word 'electricity'. Electrostatic phenomena arise from the forces that electric charges exert on each other. Such forces are described by Coulomb's law.Even though electrostatically induced forces seem to be rather weak, the electrostatic force between e.g. an electron and a proton, that together make up a hydrogen atom, is about 36 orders of magnitude stronger than the gravitational force acting between them.There are many examples of electrostatic phenomena, from those as simple as the attraction of the plastic wrap to your hand after you remove it from a package, and the attraction of paper to a charged scale, to the apparently spontaneous explosion of grain silos, the damage of electronic components during manufacturing, and the operation of photocopiers. Electrostatics involves the buildup of charge on the surface of objects due to contact with other surfaces. Although charge exchange happens whenever any two surfaces contact and separate, the effects of charge exchange are usually only noticed when at least one of the surfaces has a high resistance to electrical flow. This is because the charges that transfer to or from the highly resistive surface are more or less trapped there for a long enough time for their effects to be observed. These charges then remain on the object until they either bleed off to ground or are quickly neutralized by a discharge: e.g., the familiar phenomenon of a static 'shock' is caused by the neutralization of charge built up in the body from contact with insulated surfaces.