Electromagnetic Waves from TNT Explosions
... charges. Signals peaked 80 - 160 μs after detonation. In Cook’s book: The Science of High Explosives [3] published in 1958, he devoted all of Chapter 7 to the subjects of ionization, electrical, magnetic and electromagnetic phenomena accompanying detonations. In 1990 Boronin et al. published a revie ...
... charges. Signals peaked 80 - 160 μs after detonation. In Cook’s book: The Science of High Explosives [3] published in 1958, he devoted all of Chapter 7 to the subjects of ionization, electrical, magnetic and electromagnetic phenomena accompanying detonations. In 1990 Boronin et al. published a revie ...
Modeling Domain Wall Dynamics in Thin Magnetic Strips With
... ness of the strip are sufficiently small, so that the stable domain wall structure is the so called transverse wall [9]–[11]. For an example of its micromagnetic structure, see the top panel of Fig. 1. For wider and/or thicker strips (not considered here), a domain wall with vortex topology would ha ...
... ness of the strip are sufficiently small, so that the stable domain wall structure is the so called transverse wall [9]–[11]. For an example of its micromagnetic structure, see the top panel of Fig. 1. For wider and/or thicker strips (not considered here), a domain wall with vortex topology would ha ...
3D Inversion of magnetic total gradient data in the presence of
... of total magnetization is unknown and can be significantly different from that of the current inducing field. Thus, a vital piece of a priori information is missing and the forward modeling required in interpretation can no longer be reliably carried out. Although this problem has existed since the ...
... of total magnetization is unknown and can be significantly different from that of the current inducing field. Thus, a vital piece of a priori information is missing and the forward modeling required in interpretation can no longer be reliably carried out. Although this problem has existed since the ...
Plasma Process 6 dyn..
... At this point, we need to deal with some of the bulk motions that occur in plasmas. These are not single particle motions but rather collective motion of all/most of the charge species in the plasma. The first, and most important is the electrostatic plasma oscillation, giving rise to the plasma fre ...
... At this point, we need to deal with some of the bulk motions that occur in plasmas. These are not single particle motions but rather collective motion of all/most of the charge species in the plasma. The first, and most important is the electrostatic plasma oscillation, giving rise to the plasma fre ...
Magnetoelectric coupling in the multiferroic compound LiCu O * Chen Fang,
... To summarize our work up to this point, we have derived all the possible forms of magnetoelectric coupling that are invariant under 共1兲 time reversal, 共2兲 space inversion, and 共3兲 the lattice symmetry operations that conserve the magnetic propagation vector by using the symmetry adapted variables. I ...
... To summarize our work up to this point, we have derived all the possible forms of magnetoelectric coupling that are invariant under 共1兲 time reversal, 共2兲 space inversion, and 共3兲 the lattice symmetry operations that conserve the magnetic propagation vector by using the symmetry adapted variables. I ...
... A permanent magnet attached to a swimming elasmobranch, if not moving relative to the electrosensory system, will not create any induced electric field and should not interfere with an induction-based mechanism for magnetoreception. However experiments have shown [12] that placement of a permanent m ...
Unit 5: Day 8 – Mutual & Self Inductance
... • The inductance, L, is dependent on the geometry and the presence of a core made out of ferro-magnetic material • The symbol for inductance is: • Every electronic component, such as a resistor, or a wire, has some amount of inductance called “parasitic inductance”, which is usually unwanted. ...
... • The inductance, L, is dependent on the geometry and the presence of a core made out of ferro-magnetic material • The symbol for inductance is: • Every electronic component, such as a resistor, or a wire, has some amount of inductance called “parasitic inductance”, which is usually unwanted. ...
Carolyn Tewksbury
... that are based on Delaney and Pollard’s 1981 model, and these models were used to determine the depth of connection between the dikes and the orientation of the dike segments with respect to the main dike. However, the four initial models produced anomalies that are both larger and wider than the an ...
... that are based on Delaney and Pollard’s 1981 model, and these models were used to determine the depth of connection between the dikes and the orientation of the dike segments with respect to the main dike. However, the four initial models produced anomalies that are both larger and wider than the an ...
83887 - Radboud Repository
... The magnetic moment of Pr clusters, as seen in Fig. 3, behaves quite differently than that of the Tb clusters. An odd-even oscillation is present for many of the cluster sizes, indicative of an antiferromagnetic ordering. There is also a large peak at Pr13, something which can be attributed to a HCP ...
... The magnetic moment of Pr clusters, as seen in Fig. 3, behaves quite differently than that of the Tb clusters. An odd-even oscillation is present for many of the cluster sizes, indicative of an antiferromagnetic ordering. There is also a large peak at Pr13, something which can be attributed to a HCP ...
Particle Accelerators for High Energy Physics A Short History
... As noted above the transverse emittance is a measure of the area in x, x0 (or y, y 0 ) phase space occupied by an ensemble of particles. The definition used in Equation 8 is the area that encloses 15% of a Gaussian beam. For present-day hadron synchrotrons, synchrotron radiation does not play a role ...
... As noted above the transverse emittance is a measure of the area in x, x0 (or y, y 0 ) phase space occupied by an ensemble of particles. The definition used in Equation 8 is the area that encloses 15% of a Gaussian beam. For present-day hadron synchrotrons, synchrotron radiation does not play a role ...
Electromagnet
An electromagnet is a type of magnet in which the magnetic field is produced by an electric current. The magnetic field disappears when the current is turned off. Electromagnets usually consist of a large number of closely spaced turns of wire that create the magnetic field. The wire turns are often wound around a magnetic core made from a ferromagnetic or ferrimagnetic material such as iron; the magnetic core concentrates the magnetic flux and makes a more powerful magnet.The main advantage of an electromagnet over a permanent magnet is that the magnetic field can be quickly changed by controlling the amount of electric current in the winding. However, unlike a permanent magnet that needs no power, an electromagnet requires a continuous supply of current to maintain the magnetic field.Electromagnets are widely used as components of other electrical devices, such as motors, generators, relays, loudspeakers, hard disks, MRI machines, scientific instruments, and magnetic separation equipment. Electromagnets are also employed in industry for picking up and moving heavy iron objects such as scrap iron and steel.