View source for Engineering:Nuclear densometer

A '''nuclear densometer''' is a field instrument used in [[Engineering:Geotechnical engineering|geotechnical engineering]] to determine the density of a compacted material. Also known as a ''soil density gauge'', the device uses the interaction of gamma radiation with matter to measure density, either through direct transmission or the "backscatter" method.  The device determines the density of material by counting the number of photons emitted by a radioactive source (cesium-137) that are read by the detector tubes in the gauge base.  A 60-second time interval is typically used for the counting period.

A nuclear densometer is used on a compacted base to establish its percentage of compaction. Before field tests are performed, the technician performs a calibration on the gauge which records the 'standard count' of the machine. Standard counts are the amount of radiation released by the two nuclear sources inside the machine, with no loss or leakage. This allows the machine to compare the amount of radiation released to the amount of radiation received. With the use of a 3/4" diameter rod a hole is created in the compacted base by hammering the rod into the base to produce a hole that the densometer's probe can be inserted into. The densometer is placed on top of the hole, and then the probe is inserted into the hole by unlocking the handle at the top of the probe. One source produces radiation that interacts with the atoms in the soil, and is then compared to the standard count, to calculate the density. The other source interacts with [[Chemistry:Hydrogen|hydrogen]] atoms to calculate the percentage of water in the soil. 

In direct transmission mode, the source extends through the base of the gauge into a predrilled hole, positioning the source at the desired depth.  The testing procedure is analogous to burying a known quantity of radioactive material at a specific depth, and then using a [[Organization:Geiger counter|Geiger counter]] at the ground surface to measure how effectively the soil's density  blocks the penetration of gamma radiation through the soil.  As the soil's density increases, less radiation can pass through it, owing to dispersion from collisions with electrons in the soil being tested.

Since the soil's moisture level is partly responsible for its in-place density, the gauge also contains a [[Physics:Neutron moisture gauge|neutron moisture gauge]] consisting of an [[Chemistry:Americium|americium]]/[[Chemistry:Beryllium|beryllium]] high-energy [[Physics:Neutron source|neutron source]] and a thermal neutron detector.  The high-energy neutrons are slowed when they collide with hydrogen atoms, and the detector then counts the "slowed" neutrons.  This count is proportional to the soil's water content, since the hydrogen in this water ('''H'''<sub>2</sub>O) is responsible for almost all the hydrogen found in most soils.  The gauge calculates the moisture content, subtracts it from the soil's in-place (wet) density, and reports the soil's dry density.

== References ==
* {{citation |title=ASTM D2922-05 Standard Test Methods for Density of Soil and Soil-Aggregate in Place by Nuclear Methods (Shallow Depth) |doi=10.1520/D2922-05}} (Standard withdrawn 2007)
* {{citation |title=ASTM D6938 - 08a Standard Test Method for In-Place Density and Water Content of Soil and Soil-Aggregate by Nuclear Methods (Shallow Depth) |doi=10.1520/D6938-08A}}

== See also ==
* [[Physics:Nuclear power|Nuclear power]]

[[Category:Geotechnical engineering]]



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