Presentation of the General Solution of Three-Dimensional Dynamic Equations of a Transversely Isotropic Thermoelastic Medium. / Annin, B. D.; Ostrosablin, N. I.
In: Journal of Applied Mechanics and Technical Physics, Vol. 60, No. 2, 01.03.2019, p. 224-233.Research output: Contribution to journal › Article › peer-review
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TY - JOUR
T1 - Presentation of the General Solution of Three-Dimensional Dynamic Equations of a Transversely Isotropic Thermoelastic Medium
AU - Annin, B. D.
AU - Ostrosablin, N. I.
N1 - Publisher Copyright: © 2019, Pleiades Publishing, Ltd.
PY - 2019/3/1
Y1 - 2019/3/1
N2 - A presentation of the general solution of the equations of dynamics of a transversely isotropic thermoelastic medium is obtained in the case where the Carrier–Gassmann condition is satisfied with due allowance for the additional expression relating the temperature stress coefficients to the elasticity moduli. The displacements are expressed via three resolving potentials satisfying three inhomogeneous quasi-wave equations. The potentials are related by the heat conduction equation. A presentation of the solution with the use of the stress and displacement functions is provided. Two displacement functions are determined by solving the system of two homogeneous equations, which do not involve the temperature. After these displacement functions are determined, the temperature can be found from the third equation. The resultant presentation of the solution also yields the solution of the static equations of thermoelasticity.
AB - A presentation of the general solution of the equations of dynamics of a transversely isotropic thermoelastic medium is obtained in the case where the Carrier–Gassmann condition is satisfied with due allowance for the additional expression relating the temperature stress coefficients to the elasticity moduli. The displacements are expressed via three resolving potentials satisfying three inhomogeneous quasi-wave equations. The potentials are related by the heat conduction equation. A presentation of the solution with the use of the stress and displacement functions is provided. Two displacement functions are determined by solving the system of two homogeneous equations, which do not involve the temperature. After these displacement functions are determined, the temperature can be found from the third equation. The resultant presentation of the solution also yields the solution of the static equations of thermoelasticity.
KW - Carrier–Gassmann condition
KW - general solutions
KW - plane waves
KW - thermal conductivity
KW - thermoelasticity
KW - transverse isotropy
UR - http://www.scopus.com/inward/record.url?scp=85066477996&partnerID=8YFLogxK
U2 - 10.1134/S0021894419020044
DO - 10.1134/S0021894419020044
M3 - Article
AN - SCOPUS:85066477996
VL - 60
SP - 224
EP - 233
JO - Journal of Applied Mechanics and Technical Physics
JF - Journal of Applied Mechanics and Technical Physics
SN - 0021-8944
IS - 2
ER -
ID: 20347218