
KEY - AP Physics– Electrostatics – FR 1 #1 (1975
... e. From conservation of momentum mIvI = mIIvII and since the masses are equal we have vI = vII. Conservation of energy gives U = K = 2(½ mv2) = 0.09 J giving v = 6 m/s ...
... e. From conservation of momentum mIvI = mIIvII and since the masses are equal we have vI = vII. Conservation of energy gives U = K = 2(½ mv2) = 0.09 J giving v = 6 m/s ...
Gravitational Relativity Proposed by David Penny The only intrinsic
... Magnetism is a dependent phenomenon, the vector cross product of electric charges moving in a gravo-electric field. There is no magnetic phenomenon without electric charges moving in gravo-electric wave-fields. 8. Mechanical properties of matter are electromagnetic phenomena, or more strictly electr ...
... Magnetism is a dependent phenomenon, the vector cross product of electric charges moving in a gravo-electric field. There is no magnetic phenomenon without electric charges moving in gravo-electric wave-fields. 8. Mechanical properties of matter are electromagnetic phenomena, or more strictly electr ...
Physics 2 Homework 17 2013 We started discussing
... He noticed that a compass needle is deflected near a current carrying wire. The experimental work of Oersted was developed by two famous physicists: Michael Faraday and Andre-Mari Ampere. ...
... He noticed that a compass needle is deflected near a current carrying wire. The experimental work of Oersted was developed by two famous physicists: Michael Faraday and Andre-Mari Ampere. ...
Activity Document
... electrostatic force would be on a positive charge if one were placed at the point. The magnitude of the electric field at a given point is the magnitude of the electrostatic force that would be present on a 1.0 C charge if it were placed at the point. However, there does not actually have to be a ch ...
... electrostatic force would be on a positive charge if one were placed at the point. The magnitude of the electric field at a given point is the magnitude of the electrostatic force that would be present on a 1.0 C charge if it were placed at the point. However, there does not actually have to be a ch ...
A dipole in an electric field
... section of radius r and central angle 120°; point P is the center of curvature of the rod. (b) The field components from symmetric elements from the rod. ...
... section of radius r and central angle 120°; point P is the center of curvature of the rod. (b) The field components from symmetric elements from the rod. ...
PHYS 241 Exam Review
... Use integration to get the particle’s velocity as a function of time, then integrate again to gets its position Kinematic equations (the result when method 1. is applied in the case of constant acceleration) ...
... Use integration to get the particle’s velocity as a function of time, then integrate again to gets its position Kinematic equations (the result when method 1. is applied in the case of constant acceleration) ...
pptx - LSU Physics
... A circular loop or a coil currying electrical current is a magnetic dipole, with magnetic dipole moment of magnitude =NiA. Since the coil curries a current, it produces a magnetic field, that can be calculated using Biot-Savart’s law: ...
... A circular loop or a coil currying electrical current is a magnetic dipole, with magnetic dipole moment of magnitude =NiA. Since the coil curries a current, it produces a magnetic field, that can be calculated using Biot-Savart’s law: ...
Magnetism PowerPoint
... When the material is unmagnetized, the domains are randomly oriented. They can be partially or fully aligned by placing the material in an external magnetic field. ...
... When the material is unmagnetized, the domains are randomly oriented. They can be partially or fully aligned by placing the material in an external magnetic field. ...
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.