LEADER 04001nam  22006735  450 
001 9911007349503321
005 20250526130233.0
010   $a9783031679407$b(electronic bk.)
010   $z9783031679391
024 7 $a10.1007/978-3-031-67940-7
035   $a(MiAaPQ)EBC32131005
035   $a(Au-PeEL)EBL32131005
035   $a(CKB)38929095100041
035   $a(DE-He213)978-3-031-67940-7
035   $a(OCoLC)1521494981
035   $a(EXLCZ)9938929095100041
100   $a20250526d2025      u|         0
101 0 $aeng
135   $aurcnu||||||||
181   $ctxt$2rdacontent
182   $cc$2rdamedia
183   $acr$2rdacarrier
200 10$aExercises in Electricity and Magnetism $e100 Examples and 400 Exercises /$fby Teruo Matsushita
205   $a1st ed. 2025.
210  1$aCham :$cSpringer Nature Switzerland :$cImprint: Springer,$d2025.
215   $a1 online resource (569 pages)
311 08$aPrint version: Matsushita, Teruo Exercises in Electricity and Magnetism Cham : Springer,c2025 9783031679391 
327   $aElectrostatic Field -- Conductors -- Conductor System in Vacuum -- Dielectric Materials -- Steady Current -- Current and Magnetic Flux Density -- Superconductors -- Current Systems -- Magnetic Materials -- Electromagnetic Induction -- Displacement Current and Maxwell?s Equations -- Electromagnetic Wave.
330   $aThis book covers a great variety of problems on electricity and magnetism described in the textbook, "Electricity and Magnetism", in which superconductors are classified as one kind of magnetic materials. These problems will be helpful for a deeper understanding of the E-B analogy through a comparison between static electric and magnetic phenomena. Additionally, the usefulness of the vector potential is widely introduced. For example, the vector potential is directly used to determine the induced electromotive force. The author provides various exercises that are not covered in the textbook. The Poynting vector is useful for understanding the energy flow into capacitors or transmission lines during a charging process or into resistors during a dissipation process. A comparison between normal conducting and superconducting transmission lines shows a clear difference in the energy flow, although the final stored magnetic energy is the same. The electromagnetic potential of electromagnetic transverse electric (TE) and transverse magnetic (TM) waves in a waveguide also presents an interesting difference: The electric potential is zero in one case and non-zero in the other case. The reason for such a difference is explored. The relationship between the electric charge and electric current induced on the conductor surface is investigated for an electromagnetic wave in a waveguide or for that reflected on a conductor surface. This exercise book can be used together with the textbook 'Electricity and Magnetism' by the same author.
606   $aElectrodynamics
606   $aSuperconductivity
606   $aSuperconductors
606   $aCondensed matter
606   $aMathematical physics
606   $aElectrical engineering
606   $aClassical Electrodynamics
606   $aSuperconductivity
606   $aCondensed Matter
606   $aMathematical Methods in Physics
606   $aElectrical and Electronic Engineering
615  0$aElectrodynamics.
615  0$aSuperconductivity.
615  0$aSuperconductors.
615  0$aCondensed matter.
615  0$aMathematical physics.
615  0$aElectrical engineering.
615 14$aClassical Electrodynamics.
615 24$aSuperconductivity.
615 24$aCondensed Matter.
615 24$aMathematical Methods in Physics.
615 24$aElectrical and Electronic Engineering.
676   $a537.6
700   $aMatsushita$b Teruo$0792013
801  0$bMiAaPQ
801  1$bMiAaPQ
801  2$bMiAaPQ
912   $a9911007349503321
996   $aExercises in Electricity and Magnetism$94389683
997   $aUNINA