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Varian Linatron High-Energy X-ray Applications 2007

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The total unsharpness is reduced to include only inherent<br />

and geometrical unsharpness because they contribute much<br />

more than spot size to unsharpness. This reduces the<br />

expression the expression above to the following.<br />

UTOT = (U 2<br />

F + UG2 ) 1/2<br />

Example<br />

Let energy equal 2 MeV and focal spot equal 2 mm. If we<br />

use double emulsion film and automatic development,<br />

with U F = 0.3 mm, and a radiography arrangement where<br />

6 inches of steel are exposed with a D/T = 12, U TOT is:<br />

U TOT = (0.3 2 + (2/12) 2 ) 1/2 = 0.34 mm<br />

From this example, it can be seen that with a film<br />

unsharpness of 0.3, the geometric value only has a slight<br />

effect on the total. Figure 4-7 shows total unsharpness<br />

plotted for the case where inherent unsharpness is 1 mm.<br />

The plots show the effect of various values of D/T on the<br />

total unsharpness.<br />

FIGURE 4-7. Total unsharpness as a function of source spotsize.<br />

page 24<br />

Sensitivity and Image Quality<br />

A standard requirement in most high-energy radiography<br />

applications with <strong>Linatron</strong> sources is that the inspection<br />

process demonstrates 2% sensitivity using penetrameter<br />

wires or holes. <strong>Linatron</strong> radiography regularly produces<br />

sensitivities better than 1% through a wide range of<br />

material thicknesses. Many factors determine image<br />

quality in all high-energy <strong>Linatron</strong> radiography<br />

applications. Thickness, wire penetrameter, plaque<br />

penetrameter, and radiographic sensitivity are four kinds of<br />

sensitivity commonly evaluated determine <strong>Linatron</strong><br />

capability.<br />

Thickness Sensitivity. Thickness sensitivity refers to the<br />

ability of the radiographic inspection to demonstrate a<br />

thickness step by seeing the density difference produced on<br />

the film. Under good viewing conditions a trained eye can<br />

reliably perceive 0.006 density units with a reasonably<br />

sharp step edge in the image. This minimum perceptible<br />

density difference varies with energy and object thickness<br />

depending on the energy of the source and the contrast<br />

achieved by the film and screens. All <strong>Linatron</strong> sources can<br />

provide approximately 1% thickness sensitivity from 1 inch<br />

(25.4 mm) of steel up to 10 HVL thicknesses using finegrained<br />

film, lead screens and good scatter control.<br />

Wire Penetrameter Sensitivity. Wire penetrameters are<br />

generally used in Europe, and in several special applications<br />

in the United States. The German D.I.N. wires come in<br />

16 sizes from 3.2 mm to 0.10 mm as follows: 3.2, 2.64,<br />

2.0, 1.6, 1.32, 1.0, 0.8, 0.66, 0.5, 0.4, 0.33, 0.25, 0.20,<br />

0.165, 0.15, and 0.10 mm.<br />

Data shows that all <strong>Linatron</strong> sources should demonstrate<br />

better than 1% sensitivity above 1 inch (24.5 mm) of steel,<br />

and should achieve better than 0.5% for steel thicknesses at<br />

about 6 inches (152.4 mm).<br />

<strong>Varian</strong> <strong>Linatron</strong> applications

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