Alfvén wings at Earth`s magnetosphere under strong interplanetary
... duced. Magnetic field lines are shown, indicating that the magnetic field bends sharply as it enters the Alfvén wing, and bends back as it leaves the wing. These are the outstanding characteristics of the Alfvén wing. For Mach numbers greater than 1, the Alfvén wing angle would be shallower. At E ...
... duced. Magnetic field lines are shown, indicating that the magnetic field bends sharply as it enters the Alfvén wing, and bends back as it leaves the wing. These are the outstanding characteristics of the Alfvén wing. For Mach numbers greater than 1, the Alfvén wing angle would be shallower. At E ...
Course Description COVERPAG
... 2.E.2.1: The student is able to determine the structure of isolines of electric potential by constructing them in a given electric field. [SP 6.4, 7.2] 2.E.2.2: The student is able to predict the structure of isolines of electric potential by constructing them in a given electric field and make conn ...
... 2.E.2.1: The student is able to determine the structure of isolines of electric potential by constructing them in a given electric field. [SP 6.4, 7.2] 2.E.2.2: The student is able to predict the structure of isolines of electric potential by constructing them in a given electric field and make conn ...
Unit Systems for Electrical and Magnetic Quantities
... Systems of units for electrical and magnetic quantities have passed through a complicated and somewhat conflicting history on account of changes in our knowledge of electrical and magnetic phenomena. Historically, electrical and magnetic phenomena were researched independently up to 1820, when Oerst ...
... Systems of units for electrical and magnetic quantities have passed through a complicated and somewhat conflicting history on account of changes in our knowledge of electrical and magnetic phenomena. Historically, electrical and magnetic phenomena were researched independently up to 1820, when Oerst ...
Electromagnetic Induction
... • The magnetic flux F through a planar surface in a magnetic field B is ...
... • The magnetic flux F through a planar surface in a magnetic field B is ...
IB Misirlioglu HN Cologlu M Yildiz Under Review at JAP
... Figure 2 displays the domain structures that form in films of various thicknesses that have a fixed volumetric depletion charge density corresponding to 2x1026 ionized impurties/m3. Upon finding that low densities of depletion charge yield only a unidirectional Pf in thin films, we focus on the den ...
... Figure 2 displays the domain structures that form in films of various thicknesses that have a fixed volumetric depletion charge density corresponding to 2x1026 ionized impurties/m3. Upon finding that low densities of depletion charge yield only a unidirectional Pf in thin films, we focus on the den ...
Physics
... 1.1. Defining the systems under study (by specifying their boundaries and making explicit models of the systems) provides tools for understanding and testing ideas that are applicable throughout physics. 1.2. Objects can be treated as having no internal structure or an internal structure that can be ...
... 1.1. Defining the systems under study (by specifying their boundaries and making explicit models of the systems) provides tools for understanding and testing ideas that are applicable throughout physics. 1.2. Objects can be treated as having no internal structure or an internal structure that can be ...
Notes on (algebra based) Physics
... The list of overtones (frequencies of vibrations) of a drum is completely determined by the shape of the drumhead. Is the converse true? That is, what physical quantities regarding the shape of a drum can one infer, if the complete list of overtones is given. This is popularly stated as ‘Can one hea ...
... The list of overtones (frequencies of vibrations) of a drum is completely determined by the shape of the drumhead. Is the converse true? That is, what physical quantities regarding the shape of a drum can one infer, if the complete list of overtones is given. This is popularly stated as ‘Can one hea ...
Dynamic Line Integral Convolution for Visualizing Streamline Evolution Andreas Sundquist
... the introduction of the Line Integral Convolution (LIC) technique [3], it has been possible to depict static vector fields at an extraordinarily high spatial resolution. Traditionally, such fields had been depicted at relatively low spatial resolution using icons on a coarse grid or by using a few s ...
... the introduction of the Line Integral Convolution (LIC) technique [3], it has been possible to depict static vector fields at an extraordinarily high spatial resolution. Traditionally, such fields had been depicted at relatively low spatial resolution using icons on a coarse grid or by using a few s ...
The spin Hall effect
... [ki , k j ] 0, [ xi , k j ] i ij , [ xi , x j ] iFij Eq. of motion ...
... [ki , k j ] 0, [ xi , k j ] i ij , [ xi , x j ] iFij Eq. of motion ...
Electrostatics
Electrostatics is a branch of physics that deals with the phenomena and properties of stationary or slow-moving electric charges with no acceleration.Since classical physics, it has been known that some materials such as amber attract lightweight particles after rubbing. The Greek word for amber, ήλεκτρον electron, was the source of the word 'electricity'. Electrostatic phenomena arise from the forces that electric charges exert on each other. Such forces are described by Coulomb's law.Even though electrostatically induced forces seem to be rather weak, the electrostatic force between e.g. an electron and a proton, that together make up a hydrogen atom, is about 36 orders of magnitude stronger than the gravitational force acting between them.There are many examples of electrostatic phenomena, from those as simple as the attraction of the plastic wrap to your hand after you remove it from a package, and the attraction of paper to a charged scale, to the apparently spontaneous explosion of grain silos, the damage of electronic components during manufacturing, and the operation of photocopiers. Electrostatics involves the buildup of charge on the surface of objects due to contact with other surfaces. Although charge exchange happens whenever any two surfaces contact and separate, the effects of charge exchange are usually only noticed when at least one of the surfaces has a high resistance to electrical flow. This is because the charges that transfer to or from the highly resistive surface are more or less trapped there for a long enough time for their effects to be observed. These charges then remain on the object until they either bleed off to ground or are quickly neutralized by a discharge: e.g., the familiar phenomenon of a static 'shock' is caused by the neutralization of charge built up in the body from contact with insulated surfaces.