Theoretical and numerical models were developed to calculate the polariscopic integrated light intensity that forms a projection of the dynamic stress within an axisymmetric elastic object. Although the model is general, this paper addressed its application to measurements of stresses in model kidney stones from a burst wave lithotripter for stone fragmentation. The stress was calculated using linear elastic equations, and the light propagation was modeled in the instantaneous case by integrating over the volume of the stone. The numerical model was written in finite differences. The resulting images agreed well with measured images. The measured images corresponded to the maximum shear stress distribution, although other stresses were also plotted. Comparison of the modeled and observed polariscope images enabled refinement of the photoelastic constant by minimizing the error between the calculated and measured fields. These results enable quantification of the stress within the polariscope images, determination of material properties, and the modes and mechanisms of stress production within a kidney stone. Such a model may help in interpreting elastic waves in structures, such as stones, toward improving lithotripsy procedures.

1.
K.
Ramesh
,
Digital Photoelasticity: Advanced Techniques and Application
(
Springer
,
Berlin
,
2000
).
2.
A.
Kuske
, “
Photoelastic research on dynamic stresses
,”
Exp. Mech.
6
(
2
),
105
112
(
1966
).
3.
R. C.
Wyatt
, “
Visualization of pulsed ultrasound using stroboscopic photoelasticity
,”
Non-destructive Test.
5
(
6
),
354
358
(
1972
).
4.
H. U.
Li
and
K.
Negishi
, “
Visualization of Lamb mode patterns in a glass plate
,”
Ultrasonics
32
(
4
),
243
248
(
1994
).
5.
A.
Pawlak
and
A.
Galeski
, “
Photoelastic method of three-dimensional stress determination around axisymmetric inclusions
,”
Polymer Eng. Sci.
36
(
22
),
2736
2749
(
1996
).
6.
Y. H.
Nam
and
S. S.
Lee
, “
A quantitative evaluation of elastic wave in solid by stroboscopic photoelasticity
,”
J. Sound Vib.
259
(
5
),
1199
1207
(
2003
).
7.
T. T. P.
Nguyen
,
R.
Tanabe
, and
Y.
Ito
, “
Laser-induced shock process in under-liquid regime studied by time-resolved photoelasticity imaging technique
,”
Appl. Phys. Lett.
102
(
12
),
124103
(
2013
).
8.
X.
Xi
and
P.
Zhong
, “
Dynamic photoelastic study of the transient stress field in solids during shock wave lithotripsy
,”
J. Acoust. Soc. Am.
109
(
3
),
1226
1239
(
2001
).
9.
A. D.
Maxwell
,
B.
MacConaghy
,
M. R.
Bailey
, and
O. A.
Sapozhnikov
, “
An investigation of elastic waves producing stone fracture in burst wave lithotripsy
,”
J. Acoust. Soc. Am.
147
(
3
),
1607
1622
(
2020
).
10.
A. D.
Maxwell
,
B. W.
Cunitz
,
W.
Kreider
,
O. A.
Sapozhnikov
,
R. S.
Hsi
,
J. D.
Harper
,
M. R.
Bailey
, and
M. D.
Sorensen
, “
Fragmentation of renal calculi in vitro by burst wave lithotripsy
,”
J. Urology
193
(
1
),
338
344
(
2015
).
11.
H.
Aben
and
C.
Guillemet
,
Photoelasticity of Glass
(
Springer
,
Berlin
,
1993
).
12.
R. O.
Cleveland
and
O. A.
Sapozhnikov
, “
Modeling elastic wave propagation in kidney stones with application to shock wave lithotripsy
,”
J. Acoust. Soc. Am.
118
(
4
),
2667
2676
(
2005
).
13.
M. L. L.
Wijerathne
,
M.
Hori
, and
H.
Sakaguchi
, “
Simulation of dynamic crack growth in shockwave lithotripsy with PDS-FEM
,”
J. Appl. Mech.
13
,
253
262
(
2010
).
14.
O. A.
Sapozhnikov
,
A. D.
Maxwell
,
B.
MacConaghy
, and
M. R.
Bailey
, “
A mechanistic analysis of stone fracture in lithotripsy
,”
J. Acoust. Soc. Am.
112
(
2
),
1190
1202
(
2007
).
15.
G. B.
Malykin
, “
VL Ginzburg's helical elliptically polarized modes and their application
,”
Physics-Uspekhi
59
(12),
1245
1248
(
2016
).
16.
J.-M.
Ginoux
, “
Van der Pol's method: A simple and classic solution
,” In
History of Nonlinear Oscillations Theory in France
(1880–1940),
275
289
(Springer, Cham,
2017
).
17.
D. H.
Goldstein
,
Polarized Light
, 3rd ed. (
CRC Press
,
Boca Raton, FL
,
2011
).
18.
O.
Smolik
and
D. G.
Bellow
, “
On the mixing of photoelastic immersion liquids
,”
Exp. Mech.
14
(
10
),
400
402
(
1974
).
19.
O. A.
Sapozhnikov
, “
An exact solution to the Helmholtz equation for a quasi-Gaussian beam in the form of a superposition of two sources and sinks with complex coordinates
,”
Acoust. Phys.
58
(
1
),
41
47
(
2012
).
20.
A. B. J.
Clark
and
R. J.
Sanford
, “
A comparison of static and dynamic properties of photoelastic materials
,”
Exp. Mech.
3
(
6
),
148
151
(
1963
).
21.
D. F.
Marshall
, “
The dynamic stress-optic coefficient of Perspex
,”
Proc. Phys. Soc. (Sec. B)
70
(
11
),
1033
1039
(
1957
).
You do not currently have access to this content.