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Systematic and Random Errors in Dual Gamma Energy Soil Bulk Density and Water Content Measurements
Author(s) -
Gardner Walter H.,
Campbell Gaylon S.,
Calissendorff C.
Publication year - 1972
Publication title -
soil science society of america journal
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.836
H-Index - 168
eISSN - 1435-0661
pISSN - 0361-5995
DOI - 10.2136/sssaj1972.03615995003600030012x
Subject(s) - attenuation , photon , water content , content (measure theory) , gamma ray , physics , analytical chemistry (journal) , optics , chemistry , nuclear physics , mathematics , geology , geotechnical engineering , chromatography , mathematical analysis
Soil bulk density and water content may be obtained concurrently through measurement of the attenuation of gamma photons from two different gamma ray sources and simultaneous solution of the resulting attenuation equations. Errors in the soil bulk density and water content measurements result from random emission from the sources, random errors in attenuation coefficients and soil column thickness measurements, presence of a small, higher energy peak in the 241 Am spectrum, and counting equipment dead time. Using gamma photons from 241 Am at 0.060 Mev and from 137 Cs at 0.662 Mev, attenuated in 10‐cm soil columns, the standard deviation in both water content and bulk density measurements is primarily due to random emission and is about 0.007 g/cm 3 for 10 6 counts measured in air and about 0.005 g/cm 3 for 2.5 × 10 6 counts. However, as larger counts are used the precision of measurement of column thickness and soil and water attenuation coefficients becomes limiting. If, by obtaining large counts, the variance due to random emission is reduced to the same magnitude as that associated with measurement of column thickness or attenuation coefficients, precision limit would be about 0.0035 g/cm 3 at midrange values of water content and bulk density. At high count rates instrument dead time corrections are made to get accurate counts. Gamma rays scattered down from the small 0.103 Mev peak in the 241 Am spectrum result in attenuation dependent attenuation coefficients for which appropriate corrections must be made. For narrow collimating slits the spatial resolution is only a little greater than slit thickness. Collimater and shielding requirements are shown.