A neutron radiography facility(NRF) for non-destructive testing was installed at the NR port, one of the eight tangential beam ports of HANARO, a 30MW high flux research reactor on 1997. It was developed in compliancewith the nuclear fuel development program in KAERI for one of the post-irradiated fuel test methods. In variety of inspections in hot-cell laboratory, the fuel soundness and dimensional assessment of fuel elements and tubes were tested. As for non-nuclear applications, many diverse tests and trials on explosives, detonators, metallic molds and corrosions detection, archeological objects, were conducted etc. together with regular students education.
As industry in Korea is requiring more advanced technologies to be developed, neutron radiography techniques were applied and expanded for general industry in addition to nuclear field. Among the recent results in this trend include measurements of boron distribution and the analysis of it's quantitative content in alloy steels, defect finding in turbine blades, some tests from defense industry, and test of lithium-ion density of the cellular phone batteries, archeological objects and fuel cell.
As part of quality assurance in these of inspections, KAERI's neutron radiography laboratory has prepared not only  for accrediating in KOLAS, but also the development of tomography and dynamic radiogrpahy since 2000.
 There are two exposure units along the beam- line. The size of the first exposure unit is 120(w)185(l)190(h) cm and that of the second exposure unit is 120(w)185(l)190(h) cm. There is a beam window of 3040 cm between units through which the beam passes. The exposure time is controlled by the main beam shutter of 90 cm thickness located just behind the collimator exit. Currently, it takes about 15 seconds to open or close the main beam shutter. A quick beam shutter that spends less than 2 seconds is installed. The first exposure unit located behind the main beam shutter was designed to test the highly radioactive specimen of nuclear fuel pins using transfer method with a Dy screen converter. There is a hole of 30cm diameter, with a depth of 200cm below the floor and A cask will be moved through the ceiling so that a nuclear fuel pin up to 330cm can be scanned. The second exposure unit was designed to test the low activity or general specimens by the direct method using the combination of a 25m thick Gd converter screen and SRX-ray film. When we utilize the direct method, a typical irradiation time of 5 minutes is required to get a darkness film density of 2.5 to Kodak SR X-ray film by using a 25 mm gadolinium screen at 17 to 24MW reactor power. Gd converter is manufactured. Flaw in turbine blades, the fill-in of explosives from defense industry, the lithium-ion density of the cellular phone batteries and archeological objects are being tested
In addition, an image processing system has been installed to obtain real-time images in the second exposure unit. A commercial NE426(6LiF-ZnS(Ag)) scintillator screen and a high sensitivity SIT(silicon intensifier target) camera are being temporarily used. A digital image of 5124808bits is collected at a rate of 30 frames/sec through a commercial frame grabber. The input image frames are processed by using software we developed to perform dynamic studies.

The experiments in autoradiography require a somewhat high neutron intensity of ~ 1013 n/cm2 in order to make the clear tracks on a solid state nuclear track detectors(SSNTD) like Kodak CN-85 and LR 115. Since the neutron flux of NR beam port is not enough to reach this fluence in a reasonable time condition, a autoradiography system was set up at the vertical hole of HANARO. In principle, when 10B nuclei captures a thermal neutron, it emits alpha and recoils 7Li. These two particles make the tracks on the surface of  the SSNTD detector. Total intensity needed to make a clear image on a commercial SSNTD depend upon boron distribution in a sample. In the case of the HANARO autoradiography system, thermal neutron flux at the autoradiography beam port at the vertical hole of NAA1, NAA2, NAA3 with a diameter of 60mm is 2.671013 n/cm2/sec. An exposure time of less than 10 seconds is required for a metallic alloy having a boron content greater than 30 ppm when Kodak CN-85 is used.[4] Autoradiography of boron distribution of 130 ppm in carbon steel
The development of tomography and dynamic radiography is also in progress.
Since the HANARO NRF system has been set up, some NDT for industries and institutes has successfully been performed using film method. In addition, an image processing system has been set up for the study of dynamic observations.  Development of tomography 3D usinf cooled CCD camera is on the commissions. Along with these techniques, the HANARO neutron radiography program can be used in a wide range of user applications coming from industries and others.