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Lecture 9
Lecture 9

... As the particle penetrates in the medium, its energy loss per unit length will change. The energy loss increases towards the end of the range. Close to the end it reaches a maximum and then abruptly drops to zero. This maximum of the energy loss of charged particles close to the end of their range i ...
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... magnetic force on a moving charge: F = qv x B 1. The force is perpendicular to both the velocity v of the charge q and the magnetic field B. 2. The magnitude of the force is F = qvB sin where is the angle < 180 degrees between the velocity and the magnetic field. This implies that the magnetic force ...
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... magnetic force on a moving charge: F = qv x B 1. The force is perpendicular to both the velocity v of the charge q and the magnetic field B. 2. The magnitude of the force is F = qvB sin where is the angle < 180 degrees between the velocity and the magnetic field. This implies that the magnetic force ...
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... Until the mid-18th century, when an improved compass was invented, mariners on long voyages had to carry with them a piece of magnetite, or lodestone, to restore the magnetism of the compass needle. The soft iron then used for the needle could carry only a weak magnetism, which faded quite quickly. ...
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L10_EM_Induction

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AP® Physics C: Electricity and Magnetism 2011

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Magnetic Fields and Forces - Doane College Physics Web Server

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... attraction. Since this would be just for review, students should be able to complete this task quickly and with very little guidance. Next, students can calculate the electrical attraction between these same two particles. Although this calculation is new they should have no difficulty because of th ...
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Physics 272: Electricity and Magnetism

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Electron motion in electric and magnetic fields

... particle) will be helical as shown in figure 3. Such motion occurs above the poles of the earth where charges particles from the Sun spiral through the Earth’s field to produce the aurorae. Figure 2 ...
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AP Physics 2: Algebra-Based 2015 Free

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PHYS 102 Midterm Exam 2 (09.04.2016) Solutions

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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.
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