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托卡马克磁场位形中带电粒子的运动 王中天 核工业西南物理研究院
托卡马克磁场位形中带电粒子的运动 王中天 核工业西南物理研究院

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Document

HW6.2 Drawing Electric Fields Form A
HW6.2 Drawing Electric Fields Form A

... from the readings and what you need to go over in class. Fill out every part carefully.1 Hint: Take a look at Stop and Jot #13 & #14. The stronger the charge, the more arrows you should have. If it is positive the arrow is pointing away from the spherical charge. If it is negative, the arrow is poin ...
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... x x x x x x x x x x x x x x x x x x x x x x x v x B x x x x x x x x x x x x v F q F R • Force is always  to velocity and B. What is path? – Path will be circle. F will be the centripetal force needed to keep the charge in its circular orbit. Calculate R: ...
Lecture 2 - UCF Physics
Lecture 2 - UCF Physics

... What is the total force acting on the dipole? Zero, because the force on the two charges cancel: both have magnitude qE, and are opposite. The center of ...
Chapter 21
Chapter 21

... • The electric field is a vector field. It consists of a distribution of vectors. • We can visualize the electric field by imagining we are carrying around a small positive test charge around and mapping the direction of the force on it. • The electric field E at point P due to a charged object is d ...
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The Electric Dipole - University of Toronto Physics

... the other with –Q placed face-to-face a distance d apart. • This arrangement of two electrodes, charged equally but oppositely, is called a parallel-plate capacitor. • Capacitors play important roles in many electric circuits. ...
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272 First review

... 10. A spherical conducting shell has charge Q. A point charge q is placed at the center of the cavity. The charge on the inner surface of the shell and the charge on the outer surface of the shell, respectively, are: (a) 0, Q (b) q, Q – q (c) Q, 0 (d) – q, Q + q (e) - q, 0 11. Two point charges, sep ...
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Document

... n1 is acting just like a normal refractive index, (note the n1k0 looks like nk0 = k) If we square the E-field (complex so E2=E*E), we get ...
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Electricity and Magnetism Review 3: Units 12-16

... Two infinitely long wires are lying on the ground a distance a apart. A third wire of length L and mass M carries a current I1 and is levitated above them as shown. What current I2 must the infinitely long wires carry so that the three wires form an equilateral triangle? ...
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ELECTRODYNAMICS—lecture notes second semester 2004 Ora Entin-Wohlman

... discontinuity in the normal component of the electric field. The tangential components are continuous. Exercise: The electric field of a uniformly charged (infinite) plane, of charge σ per unit area. By symmetry, (for a plane perpendicular to the z-axis), ...
EE3321 Electromagnetic Field Theory
EE3321 Electromagnetic Field Theory

1. (a) Explain the meanings of Newton`s second and third Laws of
1. (a) Explain the meanings of Newton`s second and third Laws of

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Physics Physics 8E Volume 2 -Cutenll and Johnson (2009) (www

... to compare an experimental or observed valued with a theoretical or accepted value, you should use the following to determine the percent difference: ...
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Printable Activities

PPT - University of Illinois Urbana
PPT - University of Illinois Urbana

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Homework #23 - Shirley Temple dolls

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Field (physics)



In physics, a field is a physical quantity that has a value for each point in space and time. For example, on a weather map, the surface wind velocity is described by assigning a vector to each point on a map. Each vector represents the speed and direction of the movement of air at that point. As another example, an electric field can be thought of as a ""condition in space"" emanating from an electric charge and extending throughout the whole of space. When a test electric charge is placed in this electric field, the particle accelerates due to a force. Physicists have found the notion of a field to be of such practical utility for the analysis of forces that they have come to think of a force as due to a field.In the modern framework of the quantum theory of fields, even without referring to a test particle, a field occupies space, contains energy, and its presence eliminates a true vacuum. This lead physicists to consider electromagnetic fields to be a physical entity, making the field concept a supporting paradigm of the edifice of modern physics. ""The fact that the electromagnetic field can possess momentum and energy makes it very real... a particle makes a field, and a field acts on another particle, and the field has such familiar properties as energy content and momentum, just as particles can have"". In practice, the strength of most fields has been found to diminish with distance to the point of being undetectable. For instance the strength of many relevant classical fields, such as the gravitational field in Newton's theory of gravity or the electrostatic field in classical electromagnetism, is inversely proportional to the square of the distance from the source (i.e. they follow the Gauss's law). One consequence is that the Earth's gravitational field quickly becomes undetectable on cosmic scales.A field can be classified as a scalar field, a vector field, a spinor field or a tensor field according to whether the represented physical quantity is a scalar, a vector, a spinor or a tensor, respectively. A field has a unique tensorial character in every point where it is defined: i.e. a field cannot be a scalar field somewhere and a vector field somewhere else. For example, the Newtonian gravitational field is a vector field: specifying its value at a point in spacetime requires three numbers, the components of the gravitational field vector at that point. Moreover, within each category (scalar, vector, tensor), a field can be either a classical field or a quantum field, depending on whether it is characterized by numbers or quantum operators respectively. In fact in this theory an equivalent representation of field is a field particle, namely a boson.
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