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Phys 12 - hrsbstaff.ednet.ns.ca
Phys 12 - hrsbstaff.ednet.ns.ca

... 3. Explain how the data in an experiment to verify Coulomb’s law can be analyzed to produce a straightline graph. 4. (a) List two ways in which electric, gravitational, and magnetic forces are similar. (b) List one way in which each force is different from the other two. 5. The gravitational field i ...
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... We now use the Biot-Savart law to deal with problems in magnetostatics: this is the situation of steady currents leading to constant magnetic fields. ...
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E-field and Electric Potential Practice Problems

... 3. Which of the following statements about conductors under electrostatic conditions is true? (A) Positive work is required to move a positive charge over the surface of a conductor. (B) Charge that is placed on the surface of a conductor always spreads evenly over the surface. (C) The electric pote ...
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Kerr effect at high electric field in the isotropic

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... Thus, whatever initiates the current (i.e. a voltage source like a battery) must do work against the backward component of the magnetic force. The total horizontal force on the top segment is given by . In a time dt, the charges move a horizontal ...
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... negligibly small [14]. In these calculations the inner conductor was capped with 20 cm long end caps to reduce fringing fields. Because the calculation assumed axial symmetry, the effect of the holes in the end cap were simulated with ring-shaped apertures. As such, the calculation greatly overestim ...
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... • Will the changes below cause the capacitance of a parallelplate capacitor to increase, decrease, or stay the same. • Increase the area of each plate:  C INCREASES • Double the charge on each plate:  C stays the same • Increase the potential difference across the capacitor:  C stays the same • I ...
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REVIEW: • ELECTRIC FORCE, ELECTRIC FIELD, • ELECTRIC

... • E vector at a point in space is tangent to the EFL through that point • “Density” of EFL is proportional to E (magnitude) in that region o Larger E → closer packing of lines • EFL start on positive charges and end on negative charges • Number of EFL starting/ending on charge is proportional to its ...
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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.
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