
Right-Hand Rules
... direction of the charge's velocity, v, (recall conventional current). Point your middle finger in the direction of the magnetic field, B. Your thumb now points in the direction of the magnetic force, ...
... direction of the charge's velocity, v, (recall conventional current). Point your middle finger in the direction of the magnetic field, B. Your thumb now points in the direction of the magnetic force, ...
In this lecture Magnetic Field Magnetic Field Moving Charges in a B
... 3. A beam of electrons moves through a uniform magnetic field of 1T, directed alone the positive x-axis. The protons are travelling at an angle of 30o to the y-axis at with a velocity of 1 X 105 ms-1. What is the magnitude of the force and along which direction does the force act? 4. An electron bea ...
... 3. A beam of electrons moves through a uniform magnetic field of 1T, directed alone the positive x-axis. The protons are travelling at an angle of 30o to the y-axis at with a velocity of 1 X 105 ms-1. What is the magnitude of the force and along which direction does the force act? 4. An electron bea ...
PowerPoint Presentation - Lecture 1 Electric Charge
... It would also work if the polarity of the wire is reversed ...
... It would also work if the polarity of the wire is reversed ...
Homework No. 04 (2014 Fall) PHYS 320: Electricity and Magnetism I
... (c) Rewrite your results for the case when the solid slab is a perfect conductor? (Assume the same charge per unit area σ. Note that the charge is now only on the surface.) (d) Rewrite your results for the case of a uniformly charged hollow slab of infinite extent and thickness 2R with charge per un ...
... (c) Rewrite your results for the case when the solid slab is a perfect conductor? (Assume the same charge per unit area σ. Note that the charge is now only on the surface.) (d) Rewrite your results for the case of a uniformly charged hollow slab of infinite extent and thickness 2R with charge per un ...
images_magnetism
... L9.3 : Magnetic fields due to currents Use the Biot-Savart law to derive the magnetic field on the axis of a current loop: ...
... L9.3 : Magnetic fields due to currents Use the Biot-Savart law to derive the magnetic field on the axis of a current loop: ...
Document
... 4.2 3D simulation of a geomagnetic field •The longitudinal average of the 3D magnetic field (out to the surface) •Left – lines of force of the poloidal part of the field •Right – contours of the toroidal part of the field •Red (blue) contours – eastward (westward) directed toroidal field •Green (ye ...
... 4.2 3D simulation of a geomagnetic field •The longitudinal average of the 3D magnetic field (out to the surface) •Left – lines of force of the poloidal part of the field •Right – contours of the toroidal part of the field •Red (blue) contours – eastward (westward) directed toroidal field •Green (ye ...
Reflection of electrons in a structured shock front Prof. Michael Gedalin
... Shocks are known to be efficient particle accelerators, yet the process of the acceleration is not completely understood. Particle acceleration requires reflection off the shock front, that is, a particle, coming from upstream, should be able to return to upstream. For electrons this process is stro ...
... Shocks are known to be efficient particle accelerators, yet the process of the acceleration is not completely understood. Particle acceleration requires reflection off the shock front, that is, a particle, coming from upstream, should be able to return to upstream. For electrons this process is stro ...
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.