NBS Technical NoteU.S. Government Printing Office, 1981 |
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Page 7
... obtained . The Green's function is the solution of eq . ( 5 ) . By imposing the proper boundary condition for the parallel plate waveguide , i.e. ƏG ах = 0 at x = 0 and x = b , then one finds [ 10 ] where + ( 11 ) G ( x , z ; x ' , z ...
... obtained . The Green's function is the solution of eq . ( 5 ) . By imposing the proper boundary condition for the parallel plate waveguide , i.e. ƏG ах = 0 at x = 0 and x = b , then one finds [ 10 ] where + ( 11 ) G ( x , z ; x ' , z ...
Page 8
... obtain n Σ α i i = 1 { a , [ f , ( x , z ) + ƒ ̧‚f ; ( x ^ , z1 ) G ( x , z ; x ' , z ' ) ds ' ] = H1nc ( x , z ) . ( 15 ) i S ' i an Equation ( 15 ) is a single equation with n unknown To create at least n linear equations , a set of ...
... obtain n Σ α i i = 1 { a , [ f , ( x , z ) + ƒ ̧‚f ; ( x ^ , z1 ) G ( x , z ; x ' , z ' ) ds ' ] = H1nc ( x , z ) . ( 15 ) i S ' i an Equation ( 15 ) is a single equation with n unknown To create at least n linear equations , a set of ...
Page 11
... obtained is shown in figure 28 as the ratio of the cylinder height to the separation distance of the TEM cell . It is very interesting to note that the phase degradation at the center of the cylinder becomes predominant as the frequency ...
... obtained is shown in figure 28 as the ratio of the cylinder height to the separation distance of the TEM cell . It is very interesting to note that the phase degradation at the center of the cylinder becomes predominant as the frequency ...
Page 12
... obtain the degree of magnetic field distortion . given in the paper are for the magnetic field intensity on the surface of the cylinder . Other related quantities , such as the electric field intensity and the poynting vector can be ...
... obtain the degree of magnetic field distortion . given in the paper are for the magnetic field intensity on the surface of the cylinder . Other related quantities , such as the electric field intensity and the poynting vector can be ...
Page 4
... obtained by forming H - TS agrees quite well with the tabulated G down to 0.5 K but begins to differ from the tabulated G below 0.5 K and the two values actually have opposite signs at 0.2 K and below . Since the values of G are so ...
... obtained by forming H - TS agrees quite well with the tabulated G down to 0.5 K but begins to differ from the tabulated G below 0.5 K and the two values actually have opposite signs at 0.2 K and below . Since the values of G are so ...
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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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