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There is no quivalent ta these plots in P1][22] but b re is a good ag-nt betwlieen the UTD and moment mthod resub.
0.5 - TEz plane wave Figure 3.25: Magnitude of cmnt density distribution (J in Nm) on the surface of a square cylinder (radius-a) illuminated by a TEz plane wave at an angle of incidence oCS9.9 ' (ka=lO. a=lSY 15 b ). [- UTD. ow MM 1
Evafuation of the Uniforrn Théory
ABSTRACT Evaluation of the Uniform
ACKNOWLEDGEMENT I am grateful to E.
TABLE OF CONTENTS (continued) 3.5.4
Figur, 3.6: Magnihrde of cummt dsns
Figur, 3.28: Magnihide of cunient d
LIST OF TABLES ....................
60th TEz and TMz plane wave illumin
ISB 1 Figure 2.1 : UTD 2-D wdge dif
L=p for plane wave incidence or L-
the distance from each edge and the
2.2 CHOlCE B€IWEEN UT D RADIATION
Ffgun, 2.2: Radiation pattern (Norm
2.3 CWPARING UTD GENERAL FORMULATIO
and the final fomulation of equatio
If the lower limit of the integral
Sinœ we are dealing with the Tk ca
Figura 24: Magnitude of surface cun
2.4 CHOEE OF AN INDEPENDENT METHOD
where, fZ&) is the incident field o
where VM = &(&) (known excitation f
points, the boundary conditions wil
from equation (4.21) On any surface
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