NBS Technical NoteU.S. Government Printing Office, 1981 |
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Page 1
... equation for the magnetic field , or equivalently , the current density on the surface of a perfectly conducting cylinder in a parallel plate waveguide is solved by the method of moments to predict the degree of magnetic field ...
... equation for the magnetic field , or equivalently , the current density on the surface of a perfectly conducting cylinder in a parallel plate waveguide is solved by the method of moments to predict the degree of magnetic field ...
Page 2
... equation ; linear equation ; method of moments ; parallel plate waveguide ; quasi electrostatic ; TEM cell . I. INTRODUCTION The study of electromagnetic compatibility ( EMC ) , that is the electric and biological effects due to ...
... equation ; linear equation ; method of moments ; parallel plate waveguide ; quasi electrostatic ; TEM cell . I. INTRODUCTION The study of electromagnetic compatibility ( EMC ) , that is the electric and biological effects due to ...
Page 4
... equation for the magnetic field , or equivalently , the current density on the surface of a perfectly conducting ... equations . II . THEORY The problem of determining the electromagnetic field scattered by a perfectly conducting ...
... equation for the magnetic field , or equivalently , the current density on the surface of a perfectly conducting ... equations . II . THEORY The problem of determining the electromagnetic field scattered by a perfectly conducting ...
Page 5
... equation in Hy , i.e. , 2 2 H + k H Hy = jwε M My ? ( 3 ) where y2 = 22 2х2 22 az2 and k is the free space wave number . The boundary condition is that the normal field be zero on all of the reflecting conducting surfaces , i.e. ану = 0 ...
... equation in Hy , i.e. , 2 2 H + k H Hy = jwε M My ? ( 3 ) where y2 = 22 2х2 22 az2 and k is the free space wave number . The boundary condition is that the normal field be zero on all of the reflecting conducting surfaces , i.e. ану = 0 ...
Page 6
... Equation 7 then reduces to ӘН ( r ' ) У = 0 . an ( 8 ) -jwε G ( r , r ' ) Hy ( r ) = -Jwe { G ( r , r ' ) Myr ' ) dv ' - √se Hy ( r ' ) a Girir " ) ds ' , ( 9 ) where s Sc an indicates the surface of the rectangular cylinder . The ...
... Equation 7 then reduces to ӘН ( r ' ) У = 0 . an ( 8 ) -jwε G ( r , r ' ) Hy ( r ) = -Jwe { G ( r , r ' ) Myr ' ) dv ' - √se Hy ( r ' ) a Girir " ) ds ' , ( 9 ) where s Sc an indicates the surface of the rectangular cylinder . The ...
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antenna attenuation Backscatter response backscatter signal backscatter signature beam beam divergence Bureau of Standards C3Hg calculated calibration capture fractions components coupling loss dBV/m densimeter DEPARTMENT OF COMMERCE detector diameter diode dipole electric field electronic engineering equation experimental far-field fault signature Federal field distortion due field intensity field strength Figure frequency function graded-index fiber Haynes Hiza IEEE Trans index fibers input instrument isotropic Laboratory laser laser diode leaky modes lens logarithmic Magnetic field distortion measurement metering unit methane microbending MIXTURE mode filter mole fraction N₂ National Bureau near-field numerical aperture optical fiber OTDR output parameters peak percent perfectly conducting cylinder potentiometer pulse radiation angle radiation monitor range Rayleigh scattering Report Resistor scan Science sensor step-index fiber switch Table Tech technical Technology temperature transverse electromagnetic cell U.S. DEPARTMENT voltage waveguide wavelength ZERO
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