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Ampere law

The Gauss and Ampere laws of magnetism are obtained mathematically, and somewhat artificially, from the fact that using a Cartesian basis gives Eq. (143) (the Gauss law) and from the fact that there is no current and no B, so we have... [Pg.113]

The Ampere law is next used with a covariant definition of the curl operator V flx = Vx+i A x (351)... [Pg.149]

The origin of radiation is electromagnetic and is based on three phenomenological facts The Ampere law, the Faraday law, and the Lorentt force (Eg. 8.1) which are usually covered in a physics course. However, the usual form of Ampere s law, which gives... [Pg.396]

The Lorentz force coupled with the Ampere law and the Faraday law leads to the balance of electromagnetic momentum2 which involves the (divergence of) electromagnetic (Maxwell) stress. The isotropic limit of this stress is the electromagnetic pressure... [Pg.398]

Taking into account the continuity equation in the frequency domain V J —j ujp = 0, we may express the Maxwell-Ampere law and the Gauss electric field law as... [Pg.2]

Next, we consider the integral form of the Maxwell equations, i.e., for Faraday s induction law and Maxwell-Ampere law we integrate the differential equations on an open surface and apply the Stokes theorem, while for Gauss electric and magnetic field laws we integrate the differential equations on a bounded domain and use the Gauss theorem. [Pg.198]

Comparing the expression of the Ampere law (5.1.11) with the expression for a field created by an infinite conductor (5.1.19), one can imagine that current 7j (Figure 5.4) is creating the magnetic field which in turn acts on a neighboring conductor with current 4 then /jj = Accordingly,/ji = Bj/j. If the conductor is not rectihnear, we should... [Pg.320]

Figure 5.13 shows the arrangement of the vectors describing the field B, the conductor elanent cU and force acting on the conductor dF. Since the differential expression (5.1.24) is obtained starting fiom the Ampere law (5.1.11) the force dF is accordingly referred to as Ampere force. [Pg.320]

Figure 5.13 Vector disposition according an Ampere law in the differential form. Figure 5.13 Vector disposition according an Ampere law in the differential form.
In order to calculate the inductance of a long solenoid, we can use an expression for the total magnetic flux (Ampere law) P = L/ and P = = nIBS (where n is the number... [Pg.331]

The Ampere law from which the nonpotential character of the magnetic field follows is the next Maxwell equation. It follows from this law that the source of the magnetic field is the electric current and that it is of a nonpotential character ... [Pg.351]


See other pages where Ampere law is mentioned: [Pg.113]    [Pg.605]    [Pg.10]    [Pg.151]    [Pg.397]    [Pg.1040]    [Pg.1055]    [Pg.142]    [Pg.267]    [Pg.1]    [Pg.2]    [Pg.2]    [Pg.199]    [Pg.318]    [Pg.318]   
See also in sourсe #XX -- [ Pg.29 ]




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