
A computer aided education tool for electromagnetic scattering
... graphical, the accuracy of the solution is actually not very important. We have already presented such computer aided education (CAE) tools [2]. Depending on the objective which is sought, they are based either on an analytical solution or on a finite element (FE) solution. In this paper, a new appl ...
... graphical, the accuracy of the solution is actually not very important. We have already presented such computer aided education (CAE) tools [2]. Depending on the objective which is sought, they are based either on an analytical solution or on a finite element (FE) solution. In this paper, a new appl ...
Chapter 30 Maxwell`s Equations and Electromagnetic Waves
... Remarks: The solution presented here is valid only if the displacement of the bob during the absorption of the pulse is negligible. (Otherwise, the horizontal component of the momentum of the pulse-bob system is not conserved during the collision.) We can show that the displacement during the pulse- ...
... Remarks: The solution presented here is valid only if the displacement of the bob during the absorption of the pulse is negligible. (Otherwise, the horizontal component of the momentum of the pulse-bob system is not conserved during the collision.) We can show that the displacement during the pulse- ...
Chapter 29 Clicker Questions
... A29.4 A flexible loop of wire lies in a uniform magnetic field of magnitude B directed into the plane of the picture. The loop is pulled as shown, reducing its area. The induced current A. flows downward through resistor R and is proportional to B. B. flows upward through resistor R and is proporti ...
... A29.4 A flexible loop of wire lies in a uniform magnetic field of magnitude B directed into the plane of the picture. The loop is pulled as shown, reducing its area. The induced current A. flows downward through resistor R and is proportional to B. B. flows upward through resistor R and is proporti ...
Lecture 4
... for E fields generated by charges at rest (electrostatics) since this would correspond to the potential difference between a point and itself. Consequently, there can be no "potential function" corresponding to these induced E fields. ...
... for E fields generated by charges at rest (electrostatics) since this would correspond to the potential difference between a point and itself. Consequently, there can be no "potential function" corresponding to these induced E fields. ...
PhysicsNotes v1.pdf
... 2 Kinematics in One Dimension....................................................................................................................... 10 2.1 Motion of an object in space - Define velocity & acceleration .............................................................. 10 2.2 Motion of on ...
... 2 Kinematics in One Dimension....................................................................................................................... 10 2.1 Motion of an object in space - Define velocity & acceleration .............................................................. 10 2.2 Motion of on ...
Electric Potential
... Thus we can define an electric potential energy, U, in terms of the work done by the electric field, We, when a system changes its configuration from some initial configuration to some final configuration Change in electric potential energy = -Work done by electric field ...
... Thus we can define an electric potential energy, U, in terms of the work done by the electric field, We, when a system changes its configuration from some initial configuration to some final configuration Change in electric potential energy = -Work done by electric field ...
Applications of Gauss Law
... Now consider a configuration of electric charges which has planar symmetry but not the upside-down z → −z symmetry (46), for example an asymmetric ‘sandwich’ of several charged slabs with different thicknesses and charge densities. The electric field of such a configuration has direction along the z ...
... Now consider a configuration of electric charges which has planar symmetry but not the upside-down z → −z symmetry (46), for example an asymmetric ‘sandwich’ of several charged slabs with different thicknesses and charge densities. The electric field of such a configuration has direction along the z ...
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.