Radiography in Modern Industry - Kodak

More documents

Recommendations

Info

Figure 96: With a very small focal spot, an enlarged image can be obtained. The degree ofenlargement depends on the ratio of the source-film and source-specimen distances.Neutron RadiographyNeutron radiography makes use of the differential absorption of neutrons--uncharged nuclearparticles having about the mass of the nucleus of a hydrogen atom (proton)--rather than ofelectromagnetic radiation. Neutrons, in particular those traveling at very low velocities (thermalneutrons), are absorbed in matter according to laws that are very different from those that governthe absorption of x-rays and gamma rays. The absorption of x-rays and gamma rays increases asthe atomic number of the absorber increases, but this is not the case with thermal neutrons.Elements having adjacent atomic numbers can have widely different absorptions, and some lowatomic number elements attenuate a beam of thermal neutrons more strongly than some highatomic number elements. For example, hydrogen has a much higher neutron attenuation thandoes lead. Thus, the height of the water in a lead standpipe can be determined by neutronradiography--which is impossible with x-ray or gamma-ray radiography.Neutrons, being uncharged particles, interact with matter to only a very slight degree. As a result,photographic materials are very insensitive to the direct action of neutrons and, if neutrons are tobe used for imaging, some method must be used to convert their energy into a form more readilydetectable photographically.Radiography in Modern Industry 156
Figure 97: Two methods of neutron radiography. Top: Direct Method. Bottom: Transfermethod.Two general classes of techniques are used in neutron radiography, both involving what areknown as "converter foils". In the first--the "direct exposure" technique (See Figure 97, top)--thefilm is exposed between two layers of foil of a material that becomes radioactive when exposed toneutrons. The exposure to the film is caused by the beta or gamma radiation emitted by theconverter foils. Foils of gadolinium, rhodium, indium, and cadmium have been used. Screens ofgadolinium (0.00025-inch front, 0.002-inch back) or a front screen of 0.010-inch rhodium and aback screen of 0.002-inch gadolinium give satisfactory image quality and are among the fastestcombinations.In the second--the "transfer exposure" method (See Figure 97, bottom)--the converter foil alone isexposed to the neutron radiation transmitted by the specimen, and is thus rendered radioactive.After the exposure is terminated, the converter foil is placed in intimate contact with the film, andthe pattern of radioactivity on the converter foil produces an imaging exposure on the film.Converter foils of gold, indium, and dysprosium have been used in this technique. A dysprosiumfoil about 0.010 inch thick appears to give the highest speed, and a gold foil about 0.003 inchthick appears to give the best image quality. For efficiency, both of time and of use of theradioactivity in the foil, foil and film are kept in intimate contact for three to four half-lives of the foilactivity.Conventional industrial x-ray films are ideal for neutron radiography because the photographicmaterial is exposed to the gamma or beta radiation from the converter foil. The relative speedvalues for moderately hard x-radiation are satisfactory approximations for neutron radiography.The most satisfactory neutron source for neutron radiography is a nuclear reactor that hasprovisions for bringing a beam of thermal neutrons to the face of the reactor shield. Neutronintensities are high enough to permit realistically short exposure times. However, unless specialarrangements are made, the beams are limited to a few inches in diameter. Thus, a large objectmust be radiographed in sections. A few electronic and isotopic sources of thermal neutrons areavailable, but these suffer from the disadvantages of low neutron intensity, large effective sourcesize, or both.Radiography in Modern Industry 157
Page 1 and 2:
RadiographyinModernIndustry
Page 3 and 4:
RadiographyinModernIndustryFOURTH E
Page 5 and 6:
ContentsIntroduction...............
Page 7 and 8:
Chapter 1: The Radiographic Process
Page 9 and 10:
Intensifying ScreensX-ray and other
Page 11 and 12:
makes it a very suitable material f
Page 13 and 14:
Figure 6: Typical voltage waveforms
Page 15 and 16:
Table I - Typical X-ray Machines an
Page 17 and 18:
The wavelengths (or energies of rad
Page 19 and 20:
Table III - Industrial Gamma-Ray So
Page 21 and 22:
1. The source of light should be sm
Page 23 and 24:
B and H in the Figure 13 show the e
Page 25 and 26:
Figure 14: Geometric construction f
Page 27 and 28:
Figure 17: Pinhole pictures of the
Page 29 and 30:
The kilovoltage applied to the x-ra
Page 31 and 32:
Figure 21: Schematic diagram of som
Page 33 and 34:
kind of material radiographed, the
Page 35 and 36:
instance, the kilovoltage may be fi
Page 37 and 38:
The technique need not be limited t
Page 39 and 40:
Chapter 5: Radiographic ScreensWhen
Page 41 and 42:
Contact between the film and the le
Page 43 and 44:
Figure 29: The number of electrons
Page 45 and 46:
lead foil screens ran be retained w
Page 47 and 48:
Figure 33: The sharpness of the rad
Page 49 and 50:
Figure 34: Low density (right) is a
Page 51 and 52:
such as a wall or floor, on the fil
Page 53 and 54:
from this source. Since scatter als
Page 55 and 56:
A filter reduces excessive subject
Page 57 and 58:
Definite rules as to filter thickne
Page 59 and 60:
0.010-inch front screen of value be
Page 61 and 62:
Example: Suppose that with a given
Page 63 and 64:
If the milliamperage remains consta
Page 65 and 66:
espectively. In other words, a cons
Page 67 and 68:
Any given exposure chart applies to
Page 69 and 70:
Figure 46: Typical gamma-ray exposu
Page 71 and 72:
where the slope of the characterist
Page 73 and 74:
Figure 49: Characteristic curves of
Page 75 and 76:
Figure 51: Characteristic curve of
Page 77 and 78:
Nomogram MethodsIn Figure 54, the s
Page 79 and 80:
Figure 56: Transparent overlay posi
Page 81 and 82:
Figure 58: Overlay positioned so as
Page 83 and 84:
The problem of radiographing a part
Page 85 and 86:
Figure 62: System of lines drawn on
Page 87 and 88:
Chapter 8: Radiographic Image Quali
Page 89 and 90:
Film contrast refers to the slope (
Page 91 and 92:
Hole Type PenetrametersThe common p
Page 93 and 94:
of the same thickness as the specim
Page 95 and 96:
Chapter 9: Industrial X-ray FilmsMo
Page 97 and 98:
Figure 70 indicates the direction t
Page 99 and 100:
the lead letters on a radiation-abs
Page 101 and 102:
Therefore, protection requirements
Page 103 and 104:
5. Avoid pressure damage caused by
Page 105 and 106: Paddles or plunger-type agitators a
Page 107 and 108: slow, and the development time reco
Page 109 and 110: ubbles make their way to the surfac
Page 111 and 112: When development is complete, the f
Page 113 and 114: soften considerably with prolonged
Page 115 and 116: Figure 77: The roller transport sys
Page 117 and 118: Rapid Access to Processed Radiograp
Page 119 and 120: Figure 78: Film-feeding procedures
Page 121 and 122: Chapter 11: Process ControlUsers of
Page 123 and 124: 3. Age of the developer replenisher
Page 125 and 126: Figure 80: Control chart below for
Page 127 and 128: DiscussionDensitometric data and pr
Page 129 and 130: Figure 82: Plan of a manual x-ray p
Page 131 and 132: Figure 83: A schematic diagram of a
Page 133 and 134: loading-bench activities are carrie
Page 135 and 136: KODAK Quinone-Thiosulfate Intensifi
Page 137 and 138: Methylene-Blue MethodTwo variations
Page 139 and 140: KODAK Hypo Test Solution HT-2Avoird
Page 141 and 142: In summary, use of the test papers
Page 143 and 144: narrow angle would be very thick, e
Page 145 and 146: When radiation passes through a spe
Page 147 and 148: Figure 89: Demonstration of the eff
Page 149 and 150: Figure 90: The amount of gamma radi
Page 151 and 152: The radiograph exposed in the right
Page 153 and 154: To illustrate, let us assume that t
Page 155: Figure 95: High-speed x-ray picture
Page 159 and 160: Duplicating RadiographsSimultaneous
Page 161 and 162: Sometimes, as when sets of referenc
Page 163 and 164: PhotofluorographyIn photofluorograp
Page 165 and 166: discontinuities or of segregation i
Page 167 and 168: from the camera or by reaching down
Page 169 and 170: Figure 106: Schematic diagram of th
Page 171 and 172: valuable technique, for instance, i
Page 173 and 174: The position of the spots is determ
Page 175 and 176: Powder Diffraction File, Internatio
Page 177 and 178: Processing TechniquesRadiographs on
Page 179 and 180: Since this formula applies only to
Page 181 and 182: such that it does not distort the i
Page 183 and 184: Figure 113: A: Representation of a
Page 185 and 186: Figure 115: Characteristic curve of
Page 187 and 188: film fairly well. If high densities
Page 189 and 190: Density = 1.5 Density = 2.5Film Rel
Page 191 and 192: In most industrial radiography, the
Page 193 and 194: e noted here. Although the average
Page 195 and 196: Chapter 17: Film Graininess; Signal
Page 197 and 198: The ratio of signal to noise has a
Page 199 and 200: Chapter 18: The Photographic Latent
Page 201 and 202: Thus, the change that makes an expo
Page 203 and 204: Figure 130: Stages in the developme
Page 205 and 206: electrons by successive Compton int
Page 207 and 208:
Development is essentially a chemic
Page 209 and 210:
Chapter 19: ProtectionOne of the mo
Page 211 and 212:
duct is brought into the x-ray room
show all

Radiography in Modern Industry - Kodak

Create successful ePaper yourself

Delete template?

Save as template?