
Magnetosphere - UMass Lowell
... Some of the factors accounting for differences between the magnetospheres of the outer planets and that of earth include: • Properties of the solar wind change as we move outward, affecting the coupling of energy flux from the solar wind to the magnetospheres. • Magnetic fields of the outer planets ...
... Some of the factors accounting for differences between the magnetospheres of the outer planets and that of earth include: • Properties of the solar wind change as we move outward, affecting the coupling of energy flux from the solar wind to the magnetospheres. • Magnetic fields of the outer planets ...
Charges and Electric Fields - University of Colorado Boulder
... spread out smoothly over the volume of some object. What is the electric field at some point p due to this volume of charge? A very small (infinitesimal) volume of the the object has an infinitesimal charge dq. "dq" means a "little bit of charge" This little bit of charge dq creates an infinitesimal ...
... spread out smoothly over the volume of some object. What is the electric field at some point p due to this volume of charge? A very small (infinitesimal) volume of the the object has an infinitesimal charge dq. "dq" means a "little bit of charge" This little bit of charge dq creates an infinitesimal ...
Phase Transition and hysteresis loops in ferroelectric
... A dielectric material is any material that support charge without conducting it to a significant degree or any electrical insulator is also called a dielectric. In vacuum But the magnitude g of charge g per p unit area on either plate is called ‘electric displacement’ ...
... A dielectric material is any material that support charge without conducting it to a significant degree or any electrical insulator is also called a dielectric. In vacuum But the magnitude g of charge g per p unit area on either plate is called ‘electric displacement’ ...
physics - monikatubb
... 8. (III) Determine the magnitude and direction of the net force on the middle charge shown below. ...
... 8. (III) Determine the magnitude and direction of the net force on the middle charge shown below. ...
Unit packet Electrostatics II and Circuits Sketch the electric field
... greater field strength than ‘B’. What is true about the field lines at ‘A’ compared to B? b) Indicate all of the locations in the electric field above that are at the same field strength as ‘A’. c) Place a + (positive charge) in the field above and indicate the direction of the force it experiences ...
... greater field strength than ‘B’. What is true about the field lines at ‘A’ compared to B? b) Indicate all of the locations in the electric field above that are at the same field strength as ‘A’. c) Place a + (positive charge) in the field above and indicate the direction of the force it experiences ...
When a charged particle moves near a bar magnet, the magnetic
... When a charged particle moves near a bar magnet, the magnetic force on the particle at a certain point depends A. on the direction of the magnetic field at that point only. B. on the magnetic field and the charge of the particle only. C. on the magnetic field, the charge of the particle and the velo ...
... When a charged particle moves near a bar magnet, the magnetic force on the particle at a certain point depends A. on the direction of the magnetic field at that point only. B. on the magnetic field and the charge of the particle only. C. on the magnetic field, the charge of the particle and the velo ...
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.