Summary
Within the context of a nonlinear formulation of electrodynamics based on the constraintA 2Μ = ϱ2(A Μtimelike) for the electromagnetic potentialA Μtogether with the usual gauge-invariant electromagnetic-field Lagrangian, we study the propagation of weak discontinuities and shocks. Further the structure of the system of differential equations for the different fields is briefly examined.
Riassunto
Nellàmbito di una formulazione non lineare dell’elettrodinamica fondata sul vincolo A 2Μ , = ϱ2 A Μdi tipo tempo) per il potenziale elettromagneticoA Μ insieme all’usuale Lagrangiana invariante di gauge per il campo elettromagnetico, si studia la propagazione di discontinuità deboli e di urti. Si esamina inoltre brevemente la struttura del sistema di equazioni differenziali per i diversi campi.
РЕжУМЕ
В РАМкАх НЕлИНЕИНОИ Ф ОРМУлИРОВкИ ЁлЕктРОДИНАМИкИ, ОсН ОВАННОИ НА ОгРАНИЧЕНИИA 2μ =-ϱ2 (АΜ ь ВльЕтсь ВРЕМЕНИпОДО БНыМ) Дль ЁлЕктРОМАгНИтНОгО пОтЕНцИАлА АΜ, ВМЕстЕ с ОБыЧНыМ лАгРАНжИАН ОМ кАлИБРОВОЧНО ИНВАРИ АНтНОгО ЁлЕктРОМАгНИтНОгО п Оль, Мы ИсслЕДУЕМ РАсп РОстРАНЕНИЕ слАБых РАжРыВОВ И УДА РНых ВОлН. РАссМАтРИВАЕтс ь стРУктУРА сИстЕМы ДИФФЕРЕНцИАльНых УР АВНЕНИИ Дль РАжлИЧНы х пОлЕИ.
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Boillat, G., Venturi, G. Waves, shocks and symmetrization in a nonlinear theory of electrodynamics. Nuov Cim A 77, 358–367 (1983). https://doi.org/10.1007/BF02816661
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DOI: https://doi.org/10.1007/BF02816661