The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
The search session has expired. Please query the service again.
Si analizza la formulazione spazio-temporale delle equazioni generalizzate di campo elettromagnetico, ottenute in [1] secondo il formalismo dell'algebra di Clifford. Da tali equazioni si risale alla formulazione variazionale e alla descrizione in termini di un tensore sforzi-energia, senza che l'estensione del formalismo classico implichi, prescindendo da dati sperimentali, una riduzione del campo generalizzato al campo classico.
Si considera una possibile generalizzazione delle equazioni di Maxwell, nell'ambito del formalismo dell'algebra di Clifford per lo spazio euclideo. Si indaga se tale generalizzazione conservi le proprietà formali della descrizione classica, e si conclude che solo il dato sperimentale della conservazione della carica elettrica e della non esistenza della carica magnetica impone la riduzione al caso classico.
Download Results (CSV)