P. Cawley et al., THE CHARACTERIZATION OF OXIDE LAYERS IN ADHESIVE JOINTS USING ULTRASONIC REFLECTION MEASUREMENTS, Proceedings - Royal Society. Mathematical, physical and engineering sciences, 452(1951), 1996, pp. 1903-1926
The use of ultrasonic reflection coefficient measurements at both norm
al and oblique incidence for the detection and characterization of oxi
de layers at the adhesive-adherend interface in adhesive joints has be
en investigated. Tests have been carried out on aluminium alloy-oxide-
epoxy specimens with a minimal (< 0.1 mu m) thickness oxide layer, 43
and 15 mu m thick sulphuric acid anodized oxide oxide layers and an in
dustry standard, 3.5 mu m thick chromic acid anodized oxide layer. A s
uperpure aluminium-90 mu m thick oxalic acid anodized layer-water syst
em has also been investigated. The results indicate that the cell wall
density of the sulphuric acid anodized oxide layer is only 1990 kg m(
-3), compared to 2850 kg m(-3) for the oxalic acid anodized layer. The
cell wall density and Young's modulus are obtained from normal incide
nce measurements. Predictions of the oblique incidence reflection coef
ficients using the effective elastic constants of the oxide layer obta
ined from a standard porosity model assuming these cell wall propertie
s and the porosity measured from TEM images showed good agreement with
the measurements made on both the sulphuric acid anodized and oxalic
acid anodized specimens, only small adjustments to the properties bein
g required to obtain a very good fit. The frequency range over which i
t is necessary to take measurements increases as the thickness of the
oxide layer decreases. Maximum frequencies of 15 MHz for the oblique i
ncidence measurements and 70 MHz for the normal incidence measurement
were adequate to obtain values of rho, C-11 and C-33 for a 43 mu m thi
ck sulphuric acid anodized layer to an estimated accuracy of +/- 10% a
nd to set a lower bound on C-55. In order for a 3.5 mu m thick oxide l
ayer with similar properties to be detectable at normal incidence, the
frequency would have to be increased to over 200 MHz, while the frequ
ency of the oblique incidence measurements would have to be raised to
about 25 MHz if a 5% change could reliably be detected, or 50 MHz if a
10% change is necessary in order to ensure detection.