
Modeling Of The Active`s Layer Thickness Effect OnTransfer
... considering a current transport mechanism across the grain boundary. We formulate it by using the thermionic emission current. Indeed, being modeled as a nearly amorphous semiconductor, with energy band gap of 1.5-1.6eV [4], the grain boundary potential barrier turns out to be ≈ egb/2= 0.750.80eV an ...
... considering a current transport mechanism across the grain boundary. We formulate it by using the thermionic emission current. Indeed, being modeled as a nearly amorphous semiconductor, with energy band gap of 1.5-1.6eV [4], the grain boundary potential barrier turns out to be ≈ egb/2= 0.750.80eV an ...
Electric Charge
... sphere is opposite to that on the van de Graaff sphere. By Coulomb’s law, the two objects now attract one another, and the small sphere feels a force attracting it toward the van de Graaff. To repeat the motion of the small sphere in the animation, we have that charge “bounce off” of a square fixed ...
... sphere is opposite to that on the van de Graaff sphere. By Coulomb’s law, the two objects now attract one another, and the small sphere feels a force attracting it toward the van de Graaff. To repeat the motion of the small sphere in the animation, we have that charge “bounce off” of a square fixed ...
Example CF2: Export the field solution to a uniform grid
... Note: The surface in all the above calculator commands should lie in free space or should coincide with the surface of an object surrounded by free space (vacuum, air). It should also be noted that the above calculations hold true in general for any instance where a volume distribution of force dens ...
... Note: The surface in all the above calculator commands should lie in free space or should coincide with the surface of an object surrounded by free space (vacuum, air). It should also be noted that the above calculations hold true in general for any instance where a volume distribution of force dens ...
Chapter 5 Electric Fields in Material Space
... • For a good conductor the relaxation time is so short that most of the charge will vanish from the interior point and appear at the surface within a short time. • For a good dielectric the relaxation time is very long that the introduced charge remains wherever placed for times up to days. ...
... • For a good conductor the relaxation time is so short that most of the charge will vanish from the interior point and appear at the surface within a short time. • For a good dielectric the relaxation time is very long that the introduced charge remains wherever placed for times up to days. ...
SC related electric and magnetic field phenomena observed by the... satellite inside the plasmasphere
... The initial excursion of the electric field during SCs tends to be directed westward. The amplitude does not show a dependence on magnetic local time that has been observed outside the plasmasphere. The magnitude of the electric field variations tends to be proportional with the power of 0.6 to the ...
... The initial excursion of the electric field during SCs tends to be directed westward. The amplitude does not show a dependence on magnetic local time that has been observed outside the plasmasphere. The magnitude of the electric field variations tends to be proportional with the power of 0.6 to the ...
Physics A - Animated Science
... What do we mean by gravitational potential? How do we calculate the gravitational potential difference between two points? Where would an object have to be placed for its gravitational potential energy to be zero? ...
... What do we mean by gravitational potential? How do we calculate the gravitational potential difference between two points? Where would an object have to be placed for its gravitational potential energy to be zero? ...
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.