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Hidden nonlinearity

The standard Maxwell equations are the exact linearization by change of variables (not by truncation) of a set of nonlinear equations referring to the scalars <[), 0. The fact that this change is not completely invertible produces a hidden nonlinearity, thanks to which the linearity of the Maxwell equations is compatible with the existence of topological constants of motion that are nonlinear in A 1 and F[IV. [Pg.201]

In order to better understand the role of the hidden nonlinearity, let us examine two properties of the knots. [Pg.241]

See other pages where Hidden nonlinearity is mentioned: [Pg.197]    [Pg.198]    [Pg.199]    [Pg.201]    [Pg.203]    [Pg.205]    [Pg.207]    [Pg.209]    [Pg.211]    [Pg.213]    [Pg.215]    [Pg.217]    [Pg.219]    [Pg.221]    [Pg.223]    [Pg.225]    [Pg.227]    [Pg.229]    [Pg.231]    [Pg.233]    [Pg.235]    [Pg.236]    [Pg.237]    [Pg.239]    [Pg.240]    [Pg.241]    [Pg.241]    [Pg.243]    [Pg.245]    [Pg.247]    [Pg.249]    [Pg.251]    [Pg.253]   


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