Abstract
In this work, a bond-based peridynamic de-icing model has been developed to simulate the thermo-mechanical ice removal process of frozen structures. In the proposed numerical method, the influence of the deformation on the thermal states is considered. In this work, the ice is treated as an elastic brittle material in the framework of bond-based peridynamics, which can capture ice cracking during temperature increase and other temperature-dependent features of ice. Moreover, the characteristics of thermal load induced crack patterns in an ice sheet are discussed. The developed simulation method is verified and validated in a de-icing system of an aluminum sheet covered with ice, which is done by comparing the results obtained from peridynamic simulation with that obtained from finite element method (FEM) simulation. The results show good consistency between the peridynamic simulation and the FEM simulation. On the other hand, we find that the peridynamic simulations can directly capture the ice crack initiation and the crack propagation during the entire ice removal process, which is difficult to obtain from the FEM simulations.
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Abbreviations
- \(\varvec{\xi }_{A B}\) :
-
The bond vector in reference configuration, see Eq. (1)
- \(\varvec{\eta }_{AB}\) :
-
The relative displacement vector in current configuration, see Eq. (2)
- \({{H}_{{{x}_{A}}}}\) :
-
The horizon of particle \({{\mathbf{x}}}_{A}\)
- \({\mathbf{f}}({\xi },{\eta },t)\) :
-
The body force density function, see Eq. (4)
- s :
-
The bond stretch, see Eq. (5)
- c :
-
The micro-modulus, see Eq. (9)
- \(\kappa \) :
-
Bulk modulus of the material
- \(G_0\) :
-
The energy release rate, see Eq. (11)
- \({\mathbf{h}}\) :
-
The heat flow density, see Eq. (14)
- \(f_{h}\) :
-
The heat flow density function, see Eq. (15)
- \(c_{\nu }\) :
-
The specific heat capacity
- \(\alpha \) :
-
The coefficient of thermal expansion
- \(\varTheta ({{\mathbf{x}}_{A}},t)\) :
-
The temperature at material point \({\mathbf{x}}_{A}\)
- e :
-
The extension between the two material points, see Eq. (18)
- \(\dot{e}\) :
-
The time rate of change of e,see Eq. (19)
- \(\rho {{s}_{b}}({{\mathbf{x}}_{A}},t)\) :
-
The heat source contributed to the heat generation
- \(\dot{\varvec{\eta }}\) :
-
The time rate of change of \(\varvec{\eta }\)
- \({\mathbf{b}}({{\mathbf{x}}_{{\text {A}}}},t)\) :
-
The vector of body force density
- \(\bar{\varTheta }\) :
-
The average value of the temperature change, see Eq. (21)
- \(T_A\) :
-
The temperature at the material point \({\mathbf{x}}_{A}\)
- \(T_B\) :
-
The temperature at the material point \({\mathbf{x}}_{B}\)
- \(T_0\) :
-
The reference temperature
- \(\varGamma \) :
-
The number of the transferred wave, which is a positive real number
- \(\varsigma \) :
-
The plural
- \(\varDelta t\) :
-
Thermal time step size, see Eq. (31)
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Acknowledgements
This work is performed at the University of California Berkeley. Ms. Y. Song and Mr. R. Liu gratefully acknowledge the financial support from the Chinese Scholar Council (CSC) (CSC Grant No. 201706680094).
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Song, Y., Liu, R., Li, S. et al. Peridynamic modeling and simulation of coupled thermomechanical removal of ice from frozen structures. Meccanica 55, 961–976 (2020). https://doi.org/10.1007/s11012-019-01106-z
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DOI: https://doi.org/10.1007/s11012-019-01106-z