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Electron Discovery Thompson and Millikan
Electron Discovery Thompson and Millikan

Semiclassical motion in a perpendicular uniform electric
Semiclassical motion in a perpendicular uniform electric

Notes 2 for June 18 prepared by Melanie Smith Shusaku discussed
Notes 2 for June 18 prepared by Melanie Smith Shusaku discussed

History of the Atom
History of the Atom

Example 16-6 Where Is the Electric Field Zero?
Example 16-6 Where Is the Electric Field Zero?

Straight-forward derivation of Kittel Eq. 9.37 It is possible to derive
Straight-forward derivation of Kittel Eq. 9.37 It is possible to derive

Physics 30 Forces and Fields Concept Check 15
Physics 30 Forces and Fields Concept Check 15

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Quantum ElectroDynamics

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Physics Lecture #25

7th Homework Due December 4, 2009 1. Consider a
7th Homework Due December 4, 2009 1. Consider a

here - UNSW Physics
here - UNSW Physics

Work done by electric force (source: fixed charges) on a test charge
Work done by electric force (source: fixed charges) on a test charge

... (You can see this easily for a single fixed charge… it holds in general because of superposition.) Electric forces are “conservative” - We can define a potential energy. When a + charge moves “down the field”, the electric force does work on it, increasing its kinetic energy (or putting energy elsew ...
UNIVERSITY OF CALIFORNIA, SANTA BARBARA
UNIVERSITY OF CALIFORNIA, SANTA BARBARA

SMART Notebook
SMART Notebook

... Four point charges are at the corners of a square of side a as shown in the figure. Determine the magnitude and direction of the resultant electric force on q, with ke, q and a in symbolic form. ...
Revisiting moving electric charges
Revisiting moving electric charges

... A 20 μF parallel plate capacitor stores 300 μC of charge. The plates are 6 cm apart. An electron enters the region between the plates along the midpoint with a speed of 1 x 106 m/s as shown. What is the magnitude and direction of the force that acts on the electron (Neglect gravity). Sketch the path ...
Page 1 Problem An electron is released from rest in a uniform
Page 1 Problem An electron is released from rest in a uniform

... and negative charges are of the same magnitude and placed symmetrically about the point  where we are to find the field, the F components of both electric fields  and   are of the same magnitude but opposite direction. However, the G components are of the two electric fields are of the same ma ...
Chapter 22 Problem 66 † Given V (x)=3x - 2x 2
Chapter 22 Problem 66 † Given V (x)=3x - 2x 2

Homework 1 Solutions
Homework 1 Solutions

Discussion Session 14 1 Conceptual Questions
Discussion Session 14 1 Conceptual Questions

... r − ~v , and ~a is the acceleration of the charge. (a) Using these results, determine the exact electric and magnetic fields at the center of the orbit of a point charge, for which ~r = −Rˆ r (the minus sign is because we ˆ and ~a = −Rω 2 rˆ. Here R is want the fields at the center of the orbit), ~v ...
Lecture-15
Lecture-15

... 1. Electric field lines are in the direction of the electric force on a positive charge, but magnetic field lines are perpendicular to the magnetic force on a moving charge. 2. Electric field lines begin on positive charges and end on negative charges; magnetic field lines neither begin nor end. ...
Lecture-15
Lecture-15

... 1. Electric field lines are in the direction of the electric force on a positive charge, but magnetic field lines are perpendicular to the magnetic force on a moving charge. 2. Electric field lines begin on positive charges and end on negative charges; magnetic field lines neither begin nor end. ...
Chapter14
Chapter14

PracticeQuiz F&E
PracticeQuiz F&E

Electric field = force per charge
Electric field = force per charge

Magnetostatics The force on a moving charged particle A particle
Magnetostatics The force on a moving charged particle A particle

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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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