Illustrations of the magnetic field vectors would be virtually identical to these except all the vectors would be rotated 90 degrees about the axis of propagation so that they were perpendicular to both the direction of propagation and the electric field vector.
42.
Depending on the sign of the projection of the dipole moment onto the local electric field vector, a state may have energy that increases or decreases with field strength ( low-field and high-field seeking states respectively ).
43.
A linear retarder has a slow axis and a fast axis, and the two axes are orthogonal to each other . Polarized light travels at higher speed when its electric field vector is aligned with the fast axis of a retarder.
44.
The direction of the magnetic field vector " "'B " "'is by definition from the south to the north pole of a magnet inside the magnet; outside the field lines go from north to south.
45.
Since a wave's path through the ionosphere and the earth's magnetic field vector along such a path are rather unpredictable, a wave transmitted with vertical ( or horizontal ) polarization will generally have a resulting polarization in an arbitrary orientation at the receiver.
46.
In addition to hydrodynamical forces such as pressure and gravity, an element of magnetized fluid also feels the Lorentz force \ boldsymbol J \ times \ boldsymbol B \, where \ boldsymbol J is the current density and \ boldsymbol B is the magnetic field vector.
47.
The energy associated with an electric quadrupole moment in an electric field depends not on the field strength, but on the electric field gradient, confusingly labelled \ scriptstyle { \ underline { \ underline { q } } }, another rank-2 tensor given by the outer product of the del operator with the electric field vector:
48.
When it came to deriving the electromagnetic wave equation from displacement current in his 1865 paper A Dynamical Theory of the Electromagnetic Field, he got around the problem of the non-zero divergence associated with Gauss's law and dielectric displacement by eliminating the Gauss term and deriving the wave equation exclusively for the solenoidal magnetic field vector.
49.
Substituting equations ( 2.1 ) into ( 1.1 ) and ( 1.2 ) yields the spectral domain Greens function relating the radiated electric field to its source currents ( Scott [ 1989 ] ), where we now consider only those components of the field vectors lying in the plane of the FSS, the x-y plane:
50.
If one considers the flux of the electric field vector, "'E "', for a tube near a point charge in the field the charge but not containing it with sides formed by lines tangent to the field, the flux for the sides is zero and there is an equal and opposite flux at both ends of the tube.
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