
Chapter 27 Questions
... potential difference of 833 V, the ion enters a magnetic field of 0.92 T along a direction perpendicular to the direction of the field. Calculate the radius of the path of the ion in the field. 11. A cosmic-ray proton in interstellar space has an energy of 10 MeV and executes a circular orbit with a ...
... potential difference of 833 V, the ion enters a magnetic field of 0.92 T along a direction perpendicular to the direction of the field. Calculate the radius of the path of the ion in the field. 11. A cosmic-ray proton in interstellar space has an energy of 10 MeV and executes a circular orbit with a ...
On the Magnet - Colorado Mesa University
... Petrus Peregrinus defines magnetic poles and observes that they are never seen in isolation. ...
... Petrus Peregrinus defines magnetic poles and observes that they are never seen in isolation. ...
HUJI Syllabus
... 5. Poisson and Laplace equations - uniqueness and boundary conditions. 6. Conductivity - the image method. 7. Capacitance - placed in series or parallel, energy. 8. Electrostatic dipoles, the multipole expansion, forces, moment. 9. Dialectric materials and macroscopic polarization - the connection t ...
... 5. Poisson and Laplace equations - uniqueness and boundary conditions. 6. Conductivity - the image method. 7. Capacitance - placed in series or parallel, energy. 8. Electrostatic dipoles, the multipole expansion, forces, moment. 9. Dialectric materials and macroscopic polarization - the connection t ...
the big picture
... The number of magnetic field lines inside the wire loop changes when the loop is rotated. The faster this change occurs, the larger the induced voltage. ...
... The number of magnetic field lines inside the wire loop changes when the loop is rotated. The faster this change occurs, the larger the induced voltage. ...
Chapter 7 Sec 2
... Copyright © Glencoe/McGraw-Hill, a division of The McGraw-Hill Companies, Inc. ...
... Copyright © Glencoe/McGraw-Hill, a division of The McGraw-Hill Companies, Inc. ...
Multiferroics

Multiferroics have been formally defined as materials that exhibit more than one primary ferroic order parameter simultaneously (i.e. in a single phase), and many researchers in the field consider materials to be multiferroics only if they exhibit coupling between primary order parameters. However, the definition of multiferroics can be expanded to include non-primary order parameters, such as antiferromagnetism or ferrimagnetism.The four basic primary ferroic order parameters areferromagnetismferroelectricityferroelasticityferrotoroidicityThe last is a topic of some debate, as there was no evidence for switching ferrotoroidicity until recently.Many multiferroics are transition metal oxides with perovskite crystal structure, and include rare-earth manganites and -ferrites (e.g. TbMnO3, HoMn2O5, LuFe2O4 and recently, ""PZTFT"",). Other examples are the bismuth compounds BiFeO3 and BiMnO3, non-perovskite oxide LiCu2O2, and non-oxides such as BaNiF4 and spinel chalcogenides, e.g. ZnCr2Se4. These alloys show rich phase diagrams combining different ferroic orders in separate phases.Apart from single phase multiferroics, composites and heterostructures exhibiting more than one ferroic order parameter are studied extensively. Some examples include magnetic thin films on piezoelectric PMN-PT substrates and Metglass/PVDF/Metglass trilayer structures.Besides scientific interest in their physical properties, multiferroics have potential for applications as actuators, switches, magnetic field sensors or new types of electronic memory devices.