Figure 6.33.
Calculated normalized average SAR as a function of the electric dipole location for E polarization
in a prolate spheroidal model of an average man.
Figure 6.32.
Calculated average SAR (by long-wavelength approximation) as a function of the electric dipole location for K polarization at 27.12 MHz in a prolate spheroidal model of an average man.
Figure 6.33.
Calculated average SAR (by long-wavelength approximation) as a function of the electric dipole location for H polarization at 27.12 MHz in a prolate spheroidal model of an average man.
Figure 6.34.
Calculated average SAR (by long-wavelength approximation) as a function of the electric dipole location
for E polarization at 100 MHz in a prolate spheroidal model of a medium rat.
Figure 6.35.
Calculated average SAR (by long-wavelength
approximation) as a function of the electric dipole location
for K polarization at 100 MHz in a prolate spheroidal model
of a medium rat.
Figure 6.36.
Calculated average SAR (by long-wavelength
approximation) as a function of the electric dipole location
for H polarization at 100 MHz in a prolate spheroidal model
of a medium rat.
Figure 6.37. Calculated normalized E-field of a short
electric dipole, as a function of y/at z = 30 cm.
Figure 6.38. Calculated normalized H-field of a short
electric dipole, as a function of y/ at z = 30 cm.
Figure 6.39. Calculated variation of as a function of
y/
, at z = 30 cm, for a short electric dipole.
Figure 6.40. Calculated normalized field impedance of a
short electric dipole, as a function of y/ at z = 30
cm.
Figure 6.41. Calculated average SAR in a prolate spheroidal model of an average man irradiated by the near fields of a short electric dipole, as a function of the dipole to body spacing, d.
Figure 6.43.
The block model of man used by Chatterjee et al. (1980a, 1980b, 1980c) in the planewave spectrum
analysis.
Figure 6.44.
Incident-field Ez from a 27.12-MHz RF sealer, used by Chatterjee et al. (1980a, 1980b, 1980c) in the planewave angular-spectrum analysis.
Figure 6.45.
Average whole- and part-body SAR in the block model of man placed in front of a half-cycle cosine field, Ez; frequency = 27.12 MHz, Ez|max = 1 V/m. Calculated by Chatterjee et al. (1980a, 1980b, 1980c).
Figure 6.46.
Average whole- and part-body SAR in the block model of man placed in front of a half-cycle cosine
field, Ez ; frequency = 77 MHz, Ez | max = 1 V/m. Calculated by Chatterjee et
al. (1980a, 1980b, 1980c).
Figure 6.47.
Whole- and part-body SAR at 77 MHz in the
block model of man as a function of an assumed linear
antisymmetric phase variation in the incident
Ez; Ez|max = 1 V/m. Calculated by Chatterjee et al.
(1980a, 1980b, 1980c).
Figure 6.48.
Whole- and part-body SAR at 77 MHz in the
block model of man as a function of an assumed linear
symmetric phase variation in the incident
Ez; Ez|max = 1 V/m. Calculated by Chatterjee
et al. (1980a, 1980b, 1980c).
Figure 6.49. Whole- and part-body SAR at 350 MHz in the block model of man as a function of an assumed linear antisymmetric phase variation in the incident Ez; Ez |max = 1 V/m. Calculated by Chatterjee et al. (1980a, 1980 b , 1980c).
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Last modified: June 14, 1997
© October 1986, USAF School of Aerospace Medicine, Aerospace Medical Division (AFSC), Brooks Air Force Base, TX 78235-5301