In this paper we make a comparison between the boundary conditions (BCs) derived by Tiersten and the so-called O(h) BCs for elastic surface waves guided by thin films. By a thin layer we here mean a layer for which the thickness is much smaller than the wavelengths involved. The advantage of the O(h) model is that it starts with the general three-dimensional equation of motion and derives the boundary conditions in a rational manner keeping all terms linear in the layer thickness. The Tiersten model is obtained from the approximate equations for low frequency and flexure of thin plates by neglecting the flexural stiffness. We consider straight-crested surface waves under plane-strain conditions, so-called Rayleigh-type waves (P-SV), and Love waves (SH). It is shown that for the Rayleigh type waves the O(h) BCs gives a much better approximation of the exact case than the Tiersten BCs. Even for the Tiersten model including flexural stiffness, the O(h) BCs yields more accurate results. Concerning Love waves both the Tiersten model and O(h) model reduces to the same dispersion relation which quite well approximates the exact solution.

1.
Achenbach
J. D.
, and
Keshava
S. P.
,
1967
, “
Free Waves in a Plate Supported by a Semi-Infinite Continuum
,”
ASME JOURNAL OF APPLIED MECHANICS
, Vol.
34
, pp.
397
404
.
2.
Bostro¨m
A.
,
Bo¨vik
P.
, and
Olsson
P.
,
1992
, “
A Comparison of Exact First Order and Spring Boundary Conditions for Scattering by Thin Layers
,”
Journal of Nondestructive Evaluation
, Vol.
11
, No.
3-4
, pp.
175
184
.
3.
Bromwich
T. J. I.
,
1899
, “
On the Influence of Gravity on Elastic Waves and, in Particular, on the Vibrations on an Elastic Globe
,”
Proceedings of the London Mathematical Society
, Vol.
30
, pp.
98
120
.
4.
Bo¨vik
P.
,
1994
, “
On the Modelling of Thin Interface Layers in Elastic and Acoustic Scattering Problems
,”
Quarterly Journal of Mechanics and Applied Mathematics
, Vol.
47
, No.
1
, pp.
16
42
.
5.
Bo¨vik, P., and Olsson, P., 1991, “Diffraction of Horizontally Polarised Shear Waves by a Crack Extending From a Thin Anisotropic Layer,” Division of Mechanics, Report CTH 1991:11, Chalmers University of Technology, S-412 96 Go¨teborg, Sweden.
6.
Bo¨vik
P.
, and
Olsson
P.
,
1992
, “
Effective Boundary Conditions for the Scattering of Two-Dimensional SH Waves From a Curved Thin Elastic Layer
,”
Proceedings of the Royal Society of London
, Vol.
A439
, pp.
257
269
.
7.
Love, A. E. H., 1911, Some Problems of Geodynamics, Cambridge University Press, Cambridge, U.K.
8.
Olsson
P.
,
Datta
S. K.
, and
Bostro¨m
A.
,
1990
, “
Elastodynamic Scattering From Inclusions Surrounded by Thin Interface Layers
,”
ASME JOURNAL OF APPLIED MECHANICS
, Vol.
57
, pp.
672
676
.
9.
Parker, D. F., and Maugin, G. A., eds., 1988, Recent Developments in Surface Acoustic Waves: Proceedings of the European Mechanics Colloquium 226, University of Nottingham, U.K., Sept. 2-5. Springer-Verlag, New York.
10.
Sezawa
K.
, and
Kanai
K.
,
1935
, “
The M2 Seismic Waves
,”
Bullentin of the Earthquake Institute of Tokyo
, Vol.
13
, pp.
740
749
.
11.
Tiersten
H. F.
,
1969
, “
Elastic Surface Waves Guided by Thin Films
,”
Journal of Applied Physics
, Vol.
40
, No.
2
, pp.
770
789
.
12.
Wickham
G.
,
1992
, “
A Polarization Theory for the Scattering of Sound at Imperfect Interfaces
,”
Journal of Nondestructive Evaluation
, Vol.
11
, No.
3-4
, pp.
199
210
.
13.
Wickham
G.
, and
Bostro¨m
A.
,
1991
, “
On the Boundary Conditions for Ultrasonic Transmission by Partially Closed Cracks
,”
Journal of Nondestructive Evaluation
, Vol.
10
, No.
4
, pp.
139
149
.
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