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... isotropy of the nematic elasticity. The increased total disclination length is over-compensated by the energy decrease due to the conversion of the high energy splay-bend deformation into the lower energy twist 关13–15兴. As far as we know, the deformation dynamics of an isolated disclination remains ...
... isotropy of the nematic elasticity. The increased total disclination length is over-compensated by the energy decrease due to the conversion of the high energy splay-bend deformation into the lower energy twist 关13–15兴. As far as we know, the deformation dynamics of an isolated disclination remains ...
Magnetism
... Determine the new current if the voltage of the power supply was ... a. ... increased by a factor of 2 and vthe resistance was held constant. b. ... increased by a factor of 3 and the resistance was held constant. c. ... decreased by a factor of 2 and the resistance was held constant. d. ... held co ...
... Determine the new current if the voltage of the power supply was ... a. ... increased by a factor of 2 and vthe resistance was held constant. b. ... increased by a factor of 3 and the resistance was held constant. c. ... decreased by a factor of 2 and the resistance was held constant. d. ... held co ...
ece3313notes7.
... According to Coulomb’s law, any distribution of stationary charge produces a static electric field (electrostatic field). The analogous equation to Coulomb’s law for electric fields is the Biot-Savart law for magnetic fields. The Biot-Savart law shows that when charge moves at a constant rate (direc ...
... According to Coulomb’s law, any distribution of stationary charge produces a static electric field (electrostatic field). The analogous equation to Coulomb’s law for electric fields is the Biot-Savart law for magnetic fields. The Biot-Savart law shows that when charge moves at a constant rate (direc ...
Wave analogy tutorial
... A hand steadily wiggles the left end of the string up and down. The figure below shows snapshots of the wave on the string at three instants in time (t1, t2, t3) as the wave travels to the right. The dot painted on the string is indicated at point 1. The pictures below show two possible physical sit ...
... A hand steadily wiggles the left end of the string up and down. The figure below shows snapshots of the wave on the string at three instants in time (t1, t2, t3) as the wave travels to the right. The dot painted on the string is indicated at point 1. The pictures below show two possible physical sit ...
Homework-Biot-Savart.. - University of Colorado Boulder
... atoms of 87 Rb (one of the rubidium isotopes). In one of their internal states (the F = 1 hyperfine state), such atoms have a magnetic dipole moment of m = mB /2 where mB = e h/2me is the Bohr magneton. Magnetic trapping is achieved under the condition that the atomic magnetic moment remains anti-a ...
... atoms of 87 Rb (one of the rubidium isotopes). In one of their internal states (the F = 1 hyperfine state), such atoms have a magnetic dipole moment of m = mB /2 where mB = e h/2me is the Bohr magneton. Magnetic trapping is achieved under the condition that the atomic magnetic moment remains anti-a ...
25_InstructorGuideWin
... arise from lack of sufficient opportunities for qualitative reasoning, with appropriate feedback, ...
... arise from lack of sufficient opportunities for qualitative reasoning, with appropriate feedback, ...
The force on a conductor in a magnetic field
... Factors affecting the force The experiments above lead to the conclusion that the force F on the conductor is proportional to the length of wire in the field, L, the current I and the ‘strength’ of the field, represented by the flux density B. (There is also an 'angle factor' to consider, but we wil ...
... Factors affecting the force The experiments above lead to the conclusion that the force F on the conductor is proportional to the length of wire in the field, L, the current I and the ‘strength’ of the field, represented by the flux density B. (There is also an 'angle factor' to consider, but we wil ...
Experiment 1: Equipotential Lines and Electric
... Thus far in class we have talked about fields, both gravitational and electric, and how we can use them to understand how objects can interact at a distance. A charge, for example, creates an electric field around it, which can then exert a force on a second charge which enters that field. In this l ...
... Thus far in class we have talked about fields, both gravitational and electric, and how we can use them to understand how objects can interact at a distance. A charge, for example, creates an electric field around it, which can then exert a force on a second charge which enters that field. In this l ...
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.