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This chapter deals with conservation of energy, momentum and
This chapter deals with conservation of energy, momentum and

... We begin with energy conservation and obtain the Poynting vector which you have had exposure to in Physics 212. Poynting was Maxwell’s graduate student. The Poynting vector S is very similar to the current density J. Just like the current density gives the current per unit area flowing into a regio ...
Magnetism
Magnetism

... where  is the angle between the direction of v and B. This angle is often (but not always) 90 degrees. We will find that the maximum amount of force will be found when the angle = 90 (or 270) degrees; conversely, we find that there is zero force when the angle is 0 (or 180) degrees. o The direction ...
worksheet of IB questions for Electromagnetic
worksheet of IB questions for Electromagnetic

Wave theory of positive and negative electrons - Neo
Wave theory of positive and negative electrons - Neo

chapter25_p
chapter25_p

... If a continuous charge distribution is given  Use integrals for evaluating the total potential at some point  Each element of the charge distribution is treated as a point charge If the electric field is given  Start with the definition of the electric potential  Find the field from Gauss’ Law ( ...
Modelling natural electromagnetic interference in man
Modelling natural electromagnetic interference in man

Which of the above statements is/are correct?
Which of the above statements is/are correct?

... from the same height. Assuming that the first ball bounces perfectly,( i.e., reversing only the direction of its velocity when it strikes the ground), at what height from the ground do the balls strike each other? a) ...
Lesson #5 – Electric Potential
Lesson #5 – Electric Potential

Force on a Current-Carrying Wire in a Magnetic Field F = ILB
Force on a Current-Carrying Wire in a Magnetic Field F = ILB

SOLID-STATE PHYSICS 3, Winter 2008 O. Entin-Wohlman
SOLID-STATE PHYSICS 3, Winter 2008 O. Entin-Wohlman

... by the contribution of −k) and consequently there is no average current in the system described by the free Hamiltonian. ♣Exercise. Find the thermal average of the density in a system described by the free Hamiltonian (6.18). We wish to study the way in which a system responds to a certain perturbat ...
Activity 1
Activity 1

Static Electric Field and Potential
Static Electric Field and Potential

Maxwell`s Sea of Molecular Vortices
Maxwell`s Sea of Molecular Vortices

... Lines of Force II. Magnetic lines of force are solenoidal. However, as explained above, they are riddled with positron sources and electron sinks that form a double helix along each magnetic line of force. Electric current causes magnetic lines of force to form closed loops around it, and it then ac ...
Electromagnetic force computation with the Eggshell method
Electromagnetic force computation with the Eggshell method

Lecture 27 - MSU Physics
Lecture 27 - MSU Physics

... Planar capacitor containing a dielectric Consider a parallel plate capacitor of area A and plate separation d that has dielectric material with dielectric permittivity  between the places. (i) Find the electric field between the plates when a charge Q is placed on the capacitor. Find the voltage ac ...
Document #05
Document #05

St. Elmo`s Fire - University of Waterloo
St. Elmo`s Fire - University of Waterloo

... analyzed samples of explosives to determine their water content (6). These job opportunities, while providing the necessary finances, also occupied Faraday's time that he would rather have spent on research. Scientists today may resonate with his feeling that, "Much of [my time] is unfortunately occ ...
Physics 122B Electromagnetism - Institute for Nuclear Theory
Physics 122B Electromagnetism - Institute for Nuclear Theory

... This is the Biot-Savart Law. It is an inverse-square law, like Coulomb’s Law, but it is more complicated because it depends on the angle between the velocity v and radius vector r from the moving charge to the point of observation. The force constant 0/4 = 10-7 T m/A, where Tesla or T are the magn ...
11. electromagnetic waves
11. electromagnetic waves

Magnetism - Norwell Public Schools
Magnetism - Norwell Public Schools

Electric Potential
Electric Potential

Handout 8 - Cornell University
Handout 8 - Cornell University

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ch24

Magnetism - Stevens Institute of Technology
Magnetism - Stevens Institute of Technology

... 3. The magnetic field exerts forces on magnetic poles: •  A N pole feels a force in the direction (parallel) of the field. •  A S pole feels a force opposite to the direction (anti-parallel) of the field. A compass needle can be used to find the direction of the magnetic field. ...
Handout - Notes - 4 - Electric Potential and Voltage
Handout - Notes - 4 - Electric Potential and Voltage

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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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