
Phys202_Final_Exam_Spr2006.doc
... 54. If a clock that flashes an alarm every 7 hours, on the object in the last problem moves at the same velocity, then at what interval will that flash be seen to the observer that sees it moving? a. 783 b. 238 c. 832 d. ~ 495 ...
... 54. If a clock that flashes an alarm every 7 hours, on the object in the last problem moves at the same velocity, then at what interval will that flash be seen to the observer that sees it moving? a. 783 b. 238 c. 832 d. ~ 495 ...
About that problem that we did in class
... The other approach is via the Electric Field concept where we remove the charge B entirely from the picture and calculate the effect that the other charges have on the space where B was located. After this, we return the charge to the point to calculate the force on it. The beauty of this approach i ...
... The other approach is via the Electric Field concept where we remove the charge B entirely from the picture and calculate the effect that the other charges have on the space where B was located. After this, we return the charge to the point to calculate the force on it. The beauty of this approach i ...
Ch 12: Electromagnetic Waves
... can behave as a particle, called a photon, whose energy depends on the frequency of the waves. ...
... can behave as a particle, called a photon, whose energy depends on the frequency of the waves. ...
Physics 322 Midterm 2 1 (15 pt) 2 (50 pt) 3 (20 pt) 4 (15 pt) total (100
... c) (10 pt) Suppose the toroidal coil described in part b) has a magnetic field ~B(s, φ , z) = f (s)φ̂ (where s is a cylindrical coordinate variable: e.g. the inner radius is described as s = a). In this magnetic field, suppose a pointlike magnetic dipole with ~m = mẑ is placed at rest at s = u ∈ (a ...
... c) (10 pt) Suppose the toroidal coil described in part b) has a magnetic field ~B(s, φ , z) = f (s)φ̂ (where s is a cylindrical coordinate variable: e.g. the inner radius is described as s = a). In this magnetic field, suppose a pointlike magnetic dipole with ~m = mẑ is placed at rest at s = u ∈ (a ...
Homework No. 03 (Spring 2014) PHYS 420: Electricity and Magnetism II
... If d is the transverse length of the conductor, and v is the average drift speed of the charge carriers, show that the voltage, in magnitude, is V = vBd. ...
... If d is the transverse length of the conductor, and v is the average drift speed of the charge carriers, show that the voltage, in magnitude, is V = vBd. ...
Tomsk state university, Tomsk, Russia.
... Tomsk state university, Tomsk, Russia, e-mail: [email protected] In this paper a calculation of state lifetimes of atoms in an alternating electric field was carried out. Of special interest is a study of lifetimes of rare gas atoms because these gases are widely used for plasma physics. In the given ...
... Tomsk state university, Tomsk, Russia, e-mail: [email protected] In this paper a calculation of state lifetimes of atoms in an alternating electric field was carried out. Of special interest is a study of lifetimes of rare gas atoms because these gases are widely used for plasma physics. In the given ...
Gravity - barransclass
... representing the net force on the satellite. Label all the force vectors F. b. At each position, draw a vector to represent the satellite’s velocity. Label each vector v. ...
... representing the net force on the satellite. Label all the force vectors F. b. At each position, draw a vector to represent the satellite’s velocity. Label each vector v. ...
Electric Fields - Xavier High School
... You are probing the field of a charge of unknown magnitude and sign. You first map the field with a 1.0 x 10-6 C test charge, then you repeat your work with a 2.0 x 10-6 C test charge. a) Would you measure the same forces with the two test ...
... You are probing the field of a charge of unknown magnitude and sign. You first map the field with a 1.0 x 10-6 C test charge, then you repeat your work with a 2.0 x 10-6 C test charge. a) Would you measure the same forces with the two test ...
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.