a special U-shaped aluminum sampler. The aluminum sampler was 60 cm long with an inside width of 6 cm. Two samplers were used to sample the soil profile from 0 to 100 cm depths. These samples were carried to a laboratory where a dual-energy gamma system was used to determine water content and bulk density simultaneously. Distributions of 0 and p with soil depth are shown in Figure 13. Bulk densities as high as 1.4 g/cm" were observed in the top 30 cm of soil as compared to densities of approximately 1.0 g/cm3 between soil depths of 60-100 cm. Assuming a soil particle density of 2.65 g/cm3, the bulk densities of 1.4 and 1.0 g/cm3 represent soil porosities of 47 and 62%, respectively. The higher densities and lower porosities in the surface soil were due primarily to the compacting effect of heavy agricultural equip- ment. VII. An Uncollimated Radiation Attenuation Method for In Situ Determination of Soil Water Content A. Description of the Method Uncollimated gamma radiation has not been used for in situ deter- mination of absolute water content but it has been used to determine relative differences in soil water content (54, 79). The uncollimated radiation method indicates relative changes in water rather precisely, but measurements of the absolute water content may be subject to large errors (72). When the gamma attenuation method is to be used for measurements in situ, many difficulties may be encountered, such as temperature effects in the detector and in the instruments, lack of colli- mation, low activity sources, standardization, alignment of access tubes for source and detector, and accurate values for mass attenuation coeffi- cients. Despite these problems, this method has been useful for field studies of drainage and evapotranspiration. Basically, this method consists of placing two access tubes into the soil at 20 to 30 cm distance apart, one for the gamma radiation source and another for the detector. When the source and detector are placed at the same soil depth, the attenuated fraction of the gamma beam is measured, and, by the Lambert-Beer law, changes in water content can be determined. If two measurements of radiation intensity (1) of the attenuated beam II and 12 are taken at two different times tl and t2, the difference between 11 and 12, can be attributed to water content variation at this soil depth. The change in water content from 01 to 02 can be expressed according to the equation 02 01 In3 [17] 34