Residual Stress Instrument(RSI) is to measure residual stress distribution in metal or composite materials. When collimated monochromatic neutron beam impinges on specimen, diffraction peals of neutrons scattered by the sample appear according to Bragg's law. If interlayer distance do of material is changed by internal residual stress, the position of diffraction peak shifts. Using a position-sensitive detector one can measure the small shift of position of diffraction peak i.e., strain. One can calculate stree if Poison ratio and Young's modulus of material are known.
RSI was installed at ST2 sharing neutrons ith HRPD in early 2000. It will be reinstalled at ST1 in late 2003.


Fig 1. Schematic diagram of residual stress measurement by neutron diffraction


Fig. 2. A complete view of HANARO RSI


Design Characteristics
 
 

¡Û Monochromator : Focusing mosaic Ge (331)       -ST2
                           : bent perfect silicon crystal Si(220)  -ST1
¡Û Take off angle   : 10 - 65  (variable)
¡Û Wavelength       : 1.0 - 1.9  (variable)
¡Û Collimator         : one-slit open collimator
¡Û Detector            : One-dimensional position-sensitive detector
                             (100mm(w) 200mm(h), 2mm resolution)
¡Û Distance btw monochromator-specimen : 2.0m - 3.5m
¡Û Distance btw specimen-detector : 1.0m - 1.5m
¡Û Neutron flux at specimen position : 5 106
¡Û X-Y-Z translator table : stroke - 20cm, accuracy - 0.025mm
¡Û Measurable specimen : 5cm thickness, 1m length, 50kg weight
    Automatic measurement with individual time for each point


Instrument Description
 
 

By the end of 2003 the RSI will be installed at ST1 and will start operating  with optimized bent perfect crystal Si(220) monochromator. The Si(220) monochromator increased intensity about 2.5 times in comparison with vertical focusing mosaic Ge(331) monochromator.
Position-sensitive detector with 200mm high active window specially designed for RSI instrument decreased measurement time about 8 times in comparison with commercial position-sensitive detector.
The gauge volume is defined by fine cadmium slits fixed on snouts attatched to the slit boxes.
A computer controlled X-Y-Z translator table allowing to move the sample with accuracy 0.025mm is mounted on the diffractometer table to provide scanning of strain distribution.   
A software was developed, which allows to set individual measurement time for each point and thus save scanning time.  
In late 2004 a tensile jig will be installed to study charateristics of material and origin of residual stress.


Applications
 
 

Measurement of residual stress in welded components and composite


Major components
 

 




Representative publications
 
 

1. Residual Stress Mapping in Welded Stainless Steel Tubes, Submitted to
   KSME International Journal (2003).
2. Residual stress instrument at th HANARO, Appl. Phys A74[Suppl.] S1437-S1439(2002).
3. A High-Luminosity Position Sensitive Neutron Detector for Residual Stress
   Measurements, IEEE Transctions on nuclear science, Vol. 49, No. 5 (2002) pp. 2411-2414.
4. Development of 1-D Position Sensitive Neutron Detectors for Residual
   Stress Measurements, J. Phys. Soc. Jpn. 70(2001) Suppl. A pp.474-476.
5. Residual Stress Measurements at HANARO Reactor, Proceedings of the KSME 2000
   Fall Annual Meeting A, pp. 298-303.
6. Present Status and Perspective of Residual Stress Measurements at HANARO Reactor,
   Çѱ¹ºñÆÄ±«°Ë»çÇÐȸ 2001 Ãá°èÇмú¹ßǥȸ³í¹®Áý 3-18.