Everyone today is familiar with transmission mode X-ray radiography, in which X-rays are used to cast shadow images of teeth, bones, and luggage in airports. Less familiar is reflection mode tomography, in which X-rays or gamma rays are scattered back to a detector array for producing an image. Since the X-ray response to scattering differs from that of absorption and transmission, reflected images can reveal details that shadow images miss. In addition, reflection mode only requires access to one surface. This can have advantages where the high density bulk of an object obliterates all transmission shadows but a volume of interest is near one surface.
About a decade ago, we investigated some of the potential of closely related gamma ray backscattering inspection in a scanning mode for a range of applications including polymer composite materials, silica tiles, and metal welds, possibly even for microscopy. Related wide aperature configurations have used gamma ray backscatter radiometry (GRBR) to monitor surface coatings such as paint, enamel, and hardfacings. The new approach combined the scanning geometry of near field microscopy with carefully collimated photon sources and detectors. Such collimation only views a selected volume under a surface, potentially resolving microscopic features. For rough surfaces or inhomogeneous materials, a dual detector system can eliminate spurious responses to surface features. Energy resolution by sodium iodide spectrometry further refines system responses to changes in density in the sensitive volume.
Collimation and energy resolution together promise greater sensitivity
to delaminations, cracks, voids, and inclusions for GRBR in comparison
with related X-ray backscatter tomography. A computer code adapted
to model GRBR performance for realistic material configurations and collimator
designs made predictions verified in later bench-scale tests. The verified
code allowed selection of optimal gamma ray energies for various applications.
For inspecting through up to 2.5 inches of polymer type material, optimal
response energy was found to be below 0.200 MeV, which is conveniently
low for shielding and source handling.
The
distinguishing design feature of GRBR is the use of converging plate collimators,
constructed of tungsten foils. Scattered gamma rays are isolated
from the rest of the pulse height spectrum by selecting a specific energy
region of interest based on Compton's scattering formula. A primary
detector is collimated to view in depth, while a less finely collimated
reference detector eliminates response to surface features by accepting
scattered events from a must larger volume but with a concurrent surface
area of intersection.
Above, basic converging plate collimator
configuration using thin tunsten plates.
Left, arrangement of concurrent collimated
detectors and gamma ray source.
In several years of bench testing, digitized signals were counted individually
and compared to determine relative intensity from two detectors, but a
rapidly-scanning system could operate in "current mode" with readily available
electronic comparator circuitry. A (256 channel) multichannel analyzer
system was used to create the pulse height spectrum for discrete events
from each detector. Even simpler pulse height gating or capacitance-discharge
current mode would be suitable for a prototype hand-held instrument.
Experimental
mapping of a reference detector collimation made by moving a 30 microcurie
Co-57 source in front of the collimator slits.
Experimental
mapping of primary detector collimator with vanes that converge to touching,
i.e., a completely closed collimator. Nonvanishing acceptance is
due to transmission through corners at the front edge of each vane. Thus,
this is a measure of leakage and the limit of resolution.
Calculated counting rates for two-inch thick silica tile (Space Shuttle
protective covering).
Both computer predictions and laboratory tests confirmed feasibility of constructing a reliable scanning instrument based on GRBR for inspection of composite materials, welds, and various other applications. Effective designs all included a low-energy gamma radionuclide source (exact energy optimized for the different applications), sodium iodide detectors, single-channel analyzers, comparator circuitry, and small collimators weighing about one pound.
Pattern of scattering probabilities for energetic photons.
The computer code predicted sensitivity to hidden voids in polymer composites
to be optimized for a gamma ray energy range of 0.070 to 0.200 MeV.
With a 200 µCi Co-57 source, sufficient sensitivity was demonstrated
in bench tests to easily map delaminations smaller than 0.005 inches through
0.125 inches of simulated material. Larger sources and tighter collimation
can potentially increase sensitivity by an order of magnitude if desired.
Representative
backscatter spectrum. The two fluorescence peaks are excited by a combination
of the incident primary signal and high energy gamma contamination from
outside the system, including cosmic rays. The boxed area indicates the
kinematic region on which measurements were based.
Counting statistics, sufficient for one percent resolution in counting
rate, were achieved in 15 minutes of data collection for static configurations,
using source strengths which do not require special handling. Results
and theoretical estimates indicate that safety should not be a problem,
although a radioactive materials license will be required. Although
stronger sources will be required for a rapidly scanning instrument, this
should not create problems because the low energy gamma rays are easily
shielded and collimated. NRC approved containers and devices for
such sources are readily available for common medical and industrial radiography
applications.
Depth scan of two Lexan sheets, 3.2 mm thick separated by a 1.6 mm gap.
The curve represents the response of a solid piece of Lexan. Similar scans
easily resolved gaps as small as one micrometer.
Potential advantages of NDI and calculated performance estimates confirmed
by tests strongly warrant further bench testing and laboratory development
including detailed calibrations of actual defect densities and sizes.
We plan construction of a prototype instrument as a student project with
thorough testing, both in laboratory mock-ups and in field settings.
System modifications required for portable hand-held inspection should
also be carefully evaluated.
Scan of a 0.38 mm tantalum wire sandwiched between two 3.2 mm thick
aluminum plates.