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Morris, R.A.
Los Alamos National Lab., NM (United States). Funding organisation: USDOE, Washington, DC (United States)1997
Los Alamos National Lab., NM (United States). Funding organisation: USDOE, Washington, DC (United States)1997
AbstractAbstract
[en] The previous paper described the concept of using the net number of information bits transmitted in a radiographic image as a measure of the contrast parameter of image quality. The concept is particularly useful when the image contrast is limited by the statistics of the photon fluence incident on the detector (low doses). The Wolfram Research Mathematica program (described in Ref. 1) that was used to simulate a noisy image of an object with two thicknesses and to calculate the resulting IC (information content). The only noise source in the simulation was fluctuations in the photon fluence incident on the detector. The results from the simulation were compared to data obtained from actual radiographs of a copper step wedge radiographed with 10 and 50 pulses from a 150-p, V x-ray machine. Good agreement between the simulation and experiment was obtained when the photon fluence was considered a free, adjustable parameter. This report extends the simulation described in Ref. 1 and shows how IC varies as the following radiographic parameters change: object thickness; object Z number; x-ray energy; and incident x-ray fluence
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Oct 1997; 9 p; CONTRACT W-7405-ENG-36; Also available from OSTI as DE98001770; NTIS; US Govt. Printing Office Dep
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Morris, R.A.
Los Alamos Scientific Lab., N.Mex. (USA)1975
Los Alamos Scientific Lab., N.Mex. (USA)1975
AbstractAbstract
[en] The potential of pulsed eddy current testing for furnishing more information than conventional single-frequency eddy current methods has been known for some time. However, a fundamental problem has been analyzing the pulse shape with sufficient precision to produce accurate quantitative results. Accordingly, the primary goal of this investigation was to: demonstrate ways of digitizing the short pulses encountered in PEC testing, and to develop empirical analysis techniques that would predict some of the parameters (e.g., depth) of simple types of defect. This report describes a digitizing technique using a computer and either a conventional nuclear ADC or a fast transient analyzer; the computer software used to collect and analyze pulses; and some of the results obtained. (U.S.)
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1975; 20 p; 10. symposium on nondestructive evaluation; San Antonio, Texas, USA; 23 Apr 1975; CONF-750463--1
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Morris, R.A.
Los Alamos Scientific Lab., NM (USA)1980
Los Alamos Scientific Lab., NM (USA)1980
AbstractAbstract
[en] Nondestructive examination (NDE) can be defined as a technique or collection of techniques that permits one to determine some property of a material or object without damaging the object. There are a large number of such techniques and most of them use visual imaging in one form or another. They vary from holographic interferometry where displacements under stress are measured to the visual inspection of an objects surface to detect cracks after penetrant has been applied. The use of image processing techniques on the images produced by NDE is relatively new and can be divided into three general categories: classical image enhancement; mensuration techniques; and quantitative sensitometry. An example is discussed of how image processing techniques are used to nondestructively and destructively test the product throughout its life cycle. The product that will be followed is the microballoon target used in the laser fusion program. The laser target is a small (50 to 100 μm - dia) glass sphere with typical wall thickness of 0.5 to 6 μm. The sphere may be used as is or may be given a number of coatings of any number of materials. The beads are mass produced by the millions and the first nondestructive test is to separate the obviously bad beads (broken or incomplete) from the good ones. After this has been done, the good beads must be inspected for spherocity and wall thickness uniformity. The microradiography of the glass, uncoated bead is performed on a specially designed low-energy x-ray machine. The beads are mounted in a special jig and placed on a Kodak high resolution plate in a vacuum chamber that contains the x-ray source. The x-ray image is made with an energy less that 2 keV and the resulting images are then inspected at a magnification of 500 to 1000X. Some typical results are presented
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Source
1980; 11 p; SPIE meeting; North Hollywood, CA, USA; 4 - 7 Feb 1980; CONF-800207--2; Available from NTIS., PC A02/MF A01
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Morris, R.A.
Los Alamos National Lab., NM (United States). Funding organisation: USDOE, Washington, DC (United States)1997
Los Alamos National Lab., NM (United States). Funding organisation: USDOE, Washington, DC (United States)1997
AbstractAbstract
[en] Two measures (not independent) of radiographic image quality are contrast and spatial frequency response. At normal radiographic exposure levels, noise is not a significant factor in evaluating these parameters. However, when the photon fluence on the detector is less than 100 photons/pixel, the statistical noise in the image significantly degrades the image contrast. This paper presents a method of characterizing the image quality that utilizes both contrast and noise by calculating the net information content of the image (in bits) using the image entropy. An algorithm for calculating information content (IC) is developed and results are presented for simulated radiographs as various radiographic parameters are varied. This Mathematica code is listed in the Appendix. A copper step wedge is radiographed and the actual IC is measured for all the steps which are taken two at a time. This experimental data is compared to simulated results with good agreement. A companion report will show how varying such radiographic parameters as x-ray energy and total dose affect the IC of the image
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Jun 1997; 14 p; CONTRACT W-7405-ENG-36; ALSO AVAILABLE FROM OSTI AS DE98001875; NTIS; INIS; US GOVT. PRINTING OFFICE DEP
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Report
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Sachs, R.D.; Morris, R.A.
Los Alamos Scientific Lab., N.Mex. (USA)1976
Los Alamos Scientific Lab., N.Mex. (USA)1976
AbstractAbstract
[en] A fail-safe, reliable, easy-to-use neutron shutter was designed, built, and put into operation at the Omega West Reactor, Los Alamos Scientific Laboratory. The neutron shutter will be used primarily to perform thermal neutron radiography, but is also available for a highly collimated source of thermal neutrons [neutron flux = 3.876 x 106 (neutrons)/(cm2.s)]. Neutron collimator sizes of either 10.16 by 10.16 cm or 10.16 by 30.48 cm are available
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Nov 1976; 10 p; Available from NTIS. $3.50
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Morris, R.A.; Dalton, L.J.
Los Alamos Scientific Lab., N.Mex. (USA)1972
Los Alamos Scientific Lab., N.Mex. (USA)1972
AbstractAbstract
No abstract available
Source
Oct 1972; 33 p
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Morris, R.A.; Bryant, L.
Los Alamos Scientific Lab., NM (USA)1979
Los Alamos Scientific Lab., NM (USA)1979
AbstractAbstract
[en] Topics discussed include: high-pressure diamond cell work; x-ray fluorescence analysis; shroud of turin; laser fusion target inspection; and scanning electron microscope. Organization charts for the M-1 group are included
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Source
1979; 8 p; WANTO meeting; Oak Ridge, TN, USA; 9 - 11 Oct 1979; CONF-791098--1; Available from NTIS., PC A02/MF A01
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Kruger, R.P.; Morris, R.A.
Los Alamos Scientific Lab., NM (USA)1979
Los Alamos Scientific Lab., NM (USA)1979
AbstractAbstract
[en] The results of an on-going research project to assess the use of resonance-neutron computed-tomography for the assay of fissile materials will be discussed. A simulation study has indicated the potential value of this technique for the nondestructive inspection of a standard to be fabricated by the National Bureau of Standards
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1979; 7 p; Available from NTIS., PC A02/MF A01
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Kruger, R.P.; Morris, R.A.; Wecksung, G.W.
Los Alamos Scientific Lab., NM (USA)1980
Los Alamos Scientific Lab., NM (USA)1980
AbstractAbstract
[en] A research and development program was begun three years ago at the Los Alamos Scientific Laboratory (LASL) to study nonmedical applications of computed tomography. This program had several goals. The first goal was to develop the necessary reconstruction algorithms to accurately reconstruct cross sections of nonmedical industrial objects. The second goal was to be able to perform extensive tomographic simulations to determine the efficacy of tomographic reconstruction with a variety of hardware configurations. The final goal was to construct an inexpensive industrial prototype scanner with a high degree of design flexibility. The implementation of these program goals is described
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1980; 9 p; 1. European signal processing conference; Lausanne, Switzerland; 16 - 19 Sep 1980; CONF-800911--1; Available from NTIS., PC A02/MF A01
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Morris, R.A.; Kruger, R.P.; Wecksung, G.W.
Los Alamos Scientific Lab., NM (USA)1979
Los Alamos Scientific Lab., NM (USA)1979
AbstractAbstract
[en] A feasibility study was conducted to determine the possibility of detecting and sizing cracks in reactor cooling water tubes using tomographic techniques. Due to time and financial constraints, only one tomographic reconstruction using the best technique available was made. The results indicate that tomographic reconstructions can, in fact, detect cracks in the tubing and might possibly be capable of measuring the depth of the cracks. Limits of detectability and sensitivity have not been determined but should be investigated in any future work
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Jun 1979; 10 p; Available from NTIS., PC A02/MF A01
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