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FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

FIFTH CANADIAN CONFERENCE ON NONDESTRUCTIVE ... - IAEA

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containing the tube radius (X^) and the hoop direction (X3). At the place in<br />

the coupon where the (0002) plane spacing in the hoop direction shows residual<br />

tensile strain, the *(2ffO) plane spacing in the radial direction shows a<br />

compressive strain. The third major direction X2 (axial, corresponding to<br />

(1010)) shows a small residual tensile strain- Analysis of 19 interplanar<br />

spacings in three orthogonal planes X1X2, X2X3 and X3X1 gives the complete<br />

strain tensor including sizeable shear terms.<br />

To make this approximate one-to-one correspondence between plane normals and<br />

direction in the sample, we have made use of the marked texture of a production<br />

pressure tube. The vast majority of grains have their [01Î02 axes along the<br />

tube axis, the [0002] axes along a hoop direction and the [2110] axes along a<br />

radial direction. This is the first time such a detailed mapping of the strain<br />

has been carried out and it should lead to a realistic model of the distortion<br />

caused by overrolling.<br />

3.2 Residual stresses in Incoloy-800 steam generator tubes<br />

The steam generator tubes in CANDU nuclear generating stations are formed into<br />

hairpins. Residual stresses in a given tube after it has been bent to its<br />

design shape are undesirable because they make the tube prone to stresscorrosion<br />

cracking when a concentration of salts in areas of localized dryout<br />

coincides with high tensile stress.<br />

The spacings of the {ill} and {200} planes in the longitudinal direction of the<br />

tube were measured as a function of position around the circumference. The<br />

"relaxed" value of plane spacing was measured on a piece of straight tubing.<br />

The strains derived from {220}, {200} and {ill} planes in the radial and hoop<br />

directions were also measured as a function of circumferential position.<br />

Figure 4 shows a schematic view of the experimental arrangement in which the<br />

neutron beam beam passes first through the near wall of the tube but the<br />

incident and scattered beams only intersect in the far wall which in this case<br />

is oriented so that its axial direction lies along the scattering vector. The<br />

neutron counter is shielded so that it cannot see the scattering from the near<br />

wall. This kind of arrangement is very useful for studying tubes nondestructively.<br />

The results are shown in Fig. 5. The longitudinal (or axial)<br />

lattice strain shows a maximum just above the neutral plane of the bent tube<br />

and a minimum just below it. The maximum longitudinal strain derived from<br />

{200} planes is almost twice that derived from {ill} planes. The magnitude of<br />

the strains within the wall came as a surprise, since conventional X-ray<br />

methods [4] had indicated lower strains. The fact that the strain in the<br />

longitudinal direction could be different in differently aligned grains of a<br />

cubic material was also a surprise. Model calculations for a thin walled tube<br />

with elastic/plastic bending [5], following by elastic unloading, confirm the<br />

shape of the residual strain curve. They suggest, moreover, that the anisotropy<br />

of Young's modulus in Incoloy accounts for the difference between the {ill}<br />

and {200} strains. The Incoloy tubing is textured such that there are 5 times<br />

more {ill} planes oriented along the tube axis than {002} planes. The {ill}<br />

behaviour, showing a balanced bending moment, is more representative of the<br />

tube. However, the texture is not so strong that we can determine the complete<br />

strain tensor. The variation of lattice strain in both the hoop and radial

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