On the Scattered Reflection of Electromagnetic Waves
On the Scattered Reflection of Electromagnetic Waves
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i - Superscript or subscript character! ?ing the Incident wave, r - Superscript or subscript character! 7ing the total reflected wave.
p - Superscript or subscript characterizing the specularly reflected rave components, c, 8 - Superscript or subscript characterizing the scattered components of the total reflected wave for the (semi) cylindrical and (hemi) spherical cases re- spectively.
A, B, - Arbitrary constants (determined from proscribed initial conditions) that specify the polarization pa...rallel and perpendicular to the plane of incidence.
II', II" - Vector Hertz potentials of the electric and magnetic type respectively.
y^yw _ scalar components of the Hertz potentials, K = Kn = (27T/71 )n = (ou/cjfi" - Propagation vector (the symbol^ denotes the unit vector) .
o(, Q, - Angles of incidence, i, i, k - Unit rectangular coordinate vectors, R = r(cos 9 i + sin 8 j)+ zk - Position vector in cylindrical coordinates .
A 1, B* - Constants introduced for brevity.
a - Radius of the boss.
£ n - Neumann's factor: € n - 1 if n-0, £ n = 2ifn>0 J - Bessel functions, n B_ - Hankel functions of the first kind, Z n - Derivatives of the cylindrical functions with respect to their arguments.
What to read after On the Scattered Reflection of Electromagnetic Waves?
You can find similar books in the "Read Also" column, or choose other free books by Vic Twersky to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
i - Superscript or subscript character! ?ing the Incident wave, r - Superscript or subscript character! 7ing the total reflected wave.
p - Superscript or subscript characterizing the specularly reflected rave components, c, 8 - Superscript or subscript characterizing the scattered components of the total reflected wave for the (semi) cylindrical and (hemi) spherical cases re- spectively.
A, B, - Arbitrary constants (determined from proscribed initial conditions) that specify the polarization pa...rallel and perpendicular to the plane of incidence.
II', II" - Vector Hertz potentials of the electric and magnetic type respectively.
y^yw _ scalar components of the Hertz potentials, K = Kn = (27T/71 )n = (ou/cjfi" - Propagation vector (the symbol^ denotes the unit vector) .
o(, Q, - Angles of incidence, i, i, k - Unit rectangular coordinate vectors, R = r(cos 9 i + sin 8 j)+ zk - Position vector in cylindrical coordinates .
A 1, B* - Constants introduced for brevity.
a - Radius of the boss.
£ n - Neumann's factor: € n - 1 if n-0, £ n = 2ifn>0 J - Bessel functions, n B_ - Hankel functions of the first kind, Z n - Derivatives of the cylindrical functions with respect to their arguments.
What to read after On the Scattered Reflection of Electromagnetic Waves?
You can find similar books in the "Read Also" column, or choose other free books by Vic Twersky to read onlineMoreLess
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