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Three - University of Arkansas Physics Department

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The Portable Holographic Interferometer for residual stress<br />

measurement and nondestructive testing (NDT) <strong>of</strong> the pipelines<br />

Ywiy Onishchenko*, Anatoli Kniazkov, Jon Shulz, Gregory J. Salamo<br />

<strong>University</strong> <strong>of</strong> <strong>Arkansas</strong>, 226 <strong>Physics</strong> Bld., Fayetteville, AR 72703, USA<br />

ABSTRACT<br />

Introducing a small scratch (10-25p depth) on the surface <strong>of</strong> a part containing residual stresses produces a small<br />

change in displacements around <strong>of</strong> the scratch on the surface. When the displacements are measured as a function <strong>of</strong><br />

the depth <strong>of</strong> a scratch, a very small depth releases displacements <strong>of</strong> about U1O.The present paper shows that<br />

introduction <strong>of</strong> an additional faze shift permits determination <strong>of</strong> very small displacements and also presents the<br />

portable interferometer and the technique for measurement <strong>of</strong> residual stress in field conditions.<br />

Keywords: residual stress, portable interferometer, NDT, pipe lines.<br />

1. Introduction<br />

Holographic interferometry is an inspection technique that proved very useful in nondestructive testing. There is no<br />

physical contact with the test object. It can be applied to test objects <strong>of</strong> a wide variety <strong>of</strong> sizes and shapes, and to any<br />

type <strong>of</strong> solid materials, optical transparent or opaque. A high degree <strong>of</strong> sensitivity may be obtained, which makes<br />

possible the deteaion <strong>of</strong> low levels <strong>of</strong> displacements during inspection, resulting in interference patterns. Most<br />

procedures for measurement <strong>of</strong> residual stress near the surfsce involve removal <strong>of</strong> the material layer or drilling a<br />

hole. X-ray measurement is widely used but may be difficult to implement for certain geometric configurations and<br />

materials. The feasibility <strong>of</strong> employing interferometric techniques to measure the change in dioplacement occuning<br />

in the vicinity <strong>of</strong> the zone <strong>of</strong> the defoct or <strong>of</strong> the removal material (drilled hole, thin cut, etc.) has been recently<br />

investigated [1,2,3.4,9,10,11]. For good accuracy in counting the interference fringes (good accuracy <strong>of</strong> the<br />

determination <strong>of</strong> the residual stress) it is necessary to create a number <strong>of</strong> them. This number depends on depth <strong>of</strong> the<br />

zone <strong>of</strong> the removed material (0.5mm and more). In this case, we have to question the use <strong>of</strong> this technique for the<br />

investigation <strong>of</strong> the real structures. Ifthe depth <strong>of</strong> the zone <strong>of</strong> the removed material is very small (10-25p) one can<br />

get a number <strong>of</strong> interference less than 1/2. This depth is compared with the structural relief <strong>of</strong> the structure and can be<br />

very efasily removed from the structure if it is necessary. For determination <strong>of</strong> the number <strong>of</strong> interference less than '/1<br />

it is necessary <strong>of</strong> use the additional phase shift. This paper reports a technique for measuring residual stress using<br />

the portable holographic interferometer which has been mounted on the real construction to make measurement in<br />

field conditions.<br />

2. Background <strong>of</strong> the Complience Method (Optical Part)<br />

It is well known that holography is a linear process in the sense that two or more opt~cal waves can be recorded<br />

sequentially in time and later can be reconstructed simultaneously. Therefore the sum, difference, or even time<br />

average <strong>of</strong> a sequence <strong>of</strong> waves can be formed. In applications to interferometry, Ul(qy) represents the light<br />

scattered or transmitted to the hologram plane by some object, and U2(qy) represents light &om the same object<br />

after it has been slightly deformed or changed in some manner. Slight deformation or changes <strong>of</strong> the object<br />

primarily affect the phase <strong>of</strong> U1, so we write<br />

U ~ Y = 4hy)erp ) { -i+(&y) I,<br />

The irrad'iance <strong>of</strong> the rcconsrructed wave then becomes:<br />

U~(&Y) = a(%y)erp { -iIMx,y) + A$(&Y)I 1. (1)<br />

'~m-ce:<br />

Email: P&U@&&&&~B ; Telephone: 501 575 7978; Fax: 501 575 4580<br />

part <strong>of</strong> the SPIF Conference on Nondestructive Evaluation <strong>of</strong> Utilities and Pi~elines Ill<br />

Newoort Beach. California March 1999 SPlE Vol. 3588 0277-786X1991810.00

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