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Magnetic Field due to a Current
Magnetic Field due to a Current

Gauss`s Law
Gauss`s Law

direction of magnetic field
direction of magnetic field

... • Describe the magnetic field created by a current carrying wire • Use the Right Hand Slap Rule to predict the direction of the magnetic force ion a current carrying wire inside a magnetic field. • Use F = BIL and F = BILsin(θ) to calculate the size of the magnetic force on a current carrying wire i ...
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Lecture_8_Magnets and Magnetism print

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L`ACADEMIE POLONAISE DES SCIENCES

... h* (0, T) — N [&+(er erfc ] / T — 1)] > -&N. The solutions for the functions h, h* and
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Lecture 09 - Purdue Physics

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Electric Fields and Potentials

Homework Journal Problems 5
Homework Journal Problems 5

... and the precise nature of the assistance you received in completing this assignment. You DO NOT need to document use of the text, class handouts, or your own classroom instructor. Any published or unpublished material, or internet source, does not need to be documented unless the material specifical ...
SP212E.1121 JVanhoy Test 2 – Magnetic Fields 27 Mar 03 You may
SP212E.1121 JVanhoy Test 2 – Magnetic Fields 27 Mar 03 You may

... 6. An electron is launched with velocity v in a uniform magnetic field B. The angle between v and B is between 0 and 90o. As a result, the electron follows a helix, its velocity vector v returning to its initial value in a time interval of: A) 2m/eB B) 2mv/eB C) 2mv sin/eB D) 2mv cos/eB E) non ...
Electrostatics PP
Electrostatics PP

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charge to mass ratio of the electron motion of a charged particle
charge to mass ratio of the electron motion of a charged particle

... (b) The magnitude of the force varies as the sine of the angle, θ, between the direction of motion and the direction of the field. (c) The magnitude of the force is proportional to q, v, and B. Hence, F = qvB sinθ ...
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Ground Plane Ribbon Installation

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It is sometimes difficult to find the polarity of an
It is sometimes difficult to find the polarity of an

... The direction is away from the positive charge. A -20 mC charge would be pushed in the opposite direction of the field. F = qE F = (20 x 10-6)90000 F = 1.8 N ...
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Decay of 2S-states of the hydrogen atom in a magnetic field

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PHYS 1443 – Section 501 Lecture #1

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Chapters 16 17 Assig.. - hrsbstaff.ednet.ns.ca

... nearby electric field lines. At point B, the net force on a positive test charge would be up and to the right, parallel to the nearby electric field lines. At point C, the net force on a positive test charge would be 0. In order of decreasing field strength, the points would be ordered A, B, C. 19. ...
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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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