Abstract
This work lays out the two-potential framework for the constitutive modeling of dielectric elastomers. After its general presentation, where the constraints imposed by even electromechanical coupling, material frame indifference, material symmetry, and entropy imbalance are all spelled out, the framework is utilized to put forth a specific constitutive model for the prominent class of isotropic incompressible dielectric elastomers. The model accounts for the non-Gaussian elasticity and electrostriction typical of such materials, as well as for their deformation-enhanced shear thinning due to viscous dissipation and their time-dependent polarization due to electric dissipation. The key theoretical and practical features of the model are discussed, with special emphasis on its specialization in the limit of small deformations and moderate electric fields. The last part of this paper is devoted to the deployment of the model to fully describe the electromechanical behavior of a commercially significant dielectric elastomer, namely, the acrylate elastomer VHB 4910 from 3M.
Similar content being viewed by others
Notes
In this paper, for definiteness, we restrict attention to the Lagrangian electric field \({\mathbf{E}}\) as the independent electric variable.
Numerical experiments have shown that this scheme remains stable and accurate over very long times, while, at the same time, it also outperforms in terms of computational cost all of the various implicit methods that we have examined.
References
Amin AFMS, Lion A, Sekita S, Okui Y (2006) Nonlinear dependence of viscosity in modeling the rate-dependent response of natural and high damping rubbers in compression and shear: experimental identification and numerical verification. Int J Plast 22:1610–1657
Ask A, Menzel A, Ristinmaa M (2012) Electrostriction in electro-viscoelastic polymers. Mech Mater 50:9–21
Bauer S, Bauer-Gogonea S, Graz I, Kaltenbrunner M, Keplinger C, Schwödiauer R (2014) 25th anniversary article: a soft future: from robots and sensor skin to energy harvesters. Adv Mater 26:149–162
Böttcher CJF, Bordewijk P (1978) Theory of electric polarization, dielectrics in time-dependent fields, vol II. Elsevier, Amsterdam
Büschel A, Klinkel S, Wagner W (2013) Dielectric elastomers—numerical modelling of nonlinear visco-electroelasticity. Int J Numer Methods Eng 93:834–856
Carpi F, De Rossi D, Pelrine R, Sommer-Larsen P (2008) Dielectric elastomers as electromechanical transducers. Elsevier, Amsterdam
Cole KS, Cole RH (1941) Dispersion and absorption in dielectrics I. Alternating current characteristics. J Phys Chem 9:341–351
Debye P (1929) Polar molecules. The Chemical Catalog Company Inc, New York
Dorfmann A, Ogden RW (2005) Nonlinear electroelasticity. Acta Mech 174:167–183
Foo CC, Cai S, Koh SJA, Bauer S, Suo Z (2012) Model of dissipative dielectric elastomers. J Appl Phys 111:034102
Fosdick R, Tang H (2007) Electrodynamics and thermomechanics of material bodies. J Elast 88:255–297
Gent AN (1962) Relaxation processes in vulcanized rubber I: relation among stress relaxation, creep, recovery, and hysteresis. J Appl Polym Sci 6:433–441
Germain P, Nguyen QS, Suquet P (1983) Continuum thermodynamics. J Appl Mech 50:1010–1020
Gross B (1953) Mathematical structure of the theories of viscoelasticity. Hermann, Paris
Gupta U, Qin L, Wang Y, Godaba H, Zhu J (2019) Soft robots based on dielectric elastomer actuators: a review. Smart Mater Struct 28:103002
Halphen B, Nguyen QS (1975) Sur les matériaux standard généralisés. J Méc 14:39–63
Havriliak S, Negami S (1966) A complex plane analysis of \(\alpha \)-dispersions in some polymer systems. J Polym Sci C 14:99–117
Hong W (2011) Modeling viscoelastic dielectrics. J Mech Phys Solids 59:637–650
Hossain M, Vu DK, Steinmann P (2012) Experimental study and numerical modelling of VHB 4910 polymer. Comput Mater Sci 59:65–74
Hossain M, Vu DK, Steinmann P (2015) A comprehensive characterization of the electromechanically coupled properties of VHB 4910 polymer. Arch Appl Mech 85:523–537
Khan AS, Lopez-Pamies O (2002) Time and temperature dependent response and relaxation of a soft polymer. Int J Plast 18:1359–1372
Kofod G, Sommer-Larsen P, Kornbluh R, Pelrine R (2003) Actuation response of polyacrylate dielectric elastomers. J Intell Mater Syst Struct 14:787–793
Kremer F (2003) Schönhals A (2003) Broadband dielectric spectroscopy. Springer, Berlin
Kumar A, Lopez-Pamies O (2016) On the two-potential constitutive modelling of rubber viscoelastic materials. Comptes Rendus Mecanique 344:102–112
Lawson JD (1966) An order five Runge–Kutta process with extended region of stability. SIAM J Numer Anal 3:593–597
Lefèvre V, Lopez-Pamies O (2014) The overall elastic dielectric properties of a suspension of spherical particles in rubber: an exact explicit solution in the small-deformation limit. J Appl Phys 116:134106
Lefèvre V, Lopez-Pamies O (2017) Nonlinear electroelastic deformations of dielectric elastomer composites: I—ideal elastic dielectrics. J Mech Phys Solids 99:409–437
Lefèvre V, Lopez-Pamies O (2017) Nonlinear electroelastic deformations of dielectric elastomer composites: II—non-Gaussian elastic dielectrics. J Mech Phys Solids 99:438–470
Lefèvre V, Danas K, Lopez-Pamies O (2017) A general result for the magnetoelastic response of isotropic suspensions of iron and ferrofluid particles in rubber, with applications to spherical and cylindrical specimens. J Mech Phys Solids 107:343–364
Lefèvre V, Garnica A, Lopez-Pamies O (2019) A WENO finite-difference scheme for a new class of Hamilton–Jacobi equations in nonlinear solid mechanics. Comput Methods Appl Mech Eng 349:17–44
Lopez-Pamies O (2010) A new \(I_1\)-based hyperelastic model for rubber elastic materials. C R Méc 338:3–11
Lopez-Pamies O (2014) Elastic dielectric composites: theory and application to particle-filled ideal dielectrics. J Mech Phys Solids 64:61–82
Maugin GA, Muschik W (1994) Thermodynamics with internal variables. Part II. Applications. J Non-Equilibrium Thermodyn 19:250–289
McMeeking RM, Landis CM (2005) Electrostatic forces and stored energy for deformable dielectric materials. J Appl Mech 72:581–590
Pao YH (1978) Electromagnetic forces in deformable continua. Mech Today 4:209–305
Pei Q, Hu W, McCoul D, Biggs SJ, Stadler D, Carpi F (2016) Dielectric elastomers as EAPs: applications. Springer International Publishing, Berlin
Qiang J, Chen H, Li B (2012) Experimental study on the dielectric properties of polyacrylate dielectric elastomer. Smart Mater Struct 21:025006
Saxena P, Vu DK, Steinmann P (2014) On rate-dependent dissipation effects in electro-elasticity. Int J Non-Linear Mech 62:1–11
Sidoroff F (1974) Un modèle viscoélastique non linéaire avec configuration intermédiaire. J Méc 13:679–713
Schröder J, Keip M-A (2012) Two-scale homogenization of electromechanically coupled boundary value problems. Comput Mech 50:229–244
Spinelli SA, Lefèvre V, Lopez-Pamies O (2015) Dielectric elastomer composites: a general closed-form solution in the small-deformation limit. J Mech Phys Solids 83:263–284
Stratton JS (1941) Electromagnetic theory. McGraw-Hill, New York
Suo Z, Zhao X, Greene WH (2008) A nonlinear field theory of deformable dielectrics. J Mech Phys Solids 56:467–486
Tian L, Tevet-Deree L, deBotton G, Bhattacharya K (2012) Dielectric elastomer composites. J Mech Phys Solids 60:181–198
Toupin RA (1956) The elastic dielectric. J Ration Mech Anal 5:849–915
Vogel F, Göktepe S, Steinmann P, Kuhl E (2014) Modeling and simulation of viscous electro-active polymers. Eur J Mech A/Solids 48:112–128
Wang S, Decker M, Henann DL, Chester SA (2016) Modeling of dielectric viscoelastomers with application to electromechanical instabilities. J Mech Phys Solids 95:213–229
Wissler M, Mazza E (2007) Electromechanical coupling in dielectric elastomer actuators. Sens Actuators A Phys 138:384–393
Wu H, Huang Y, Xu F, Duan Y, Yin Z (2016) Energy harvesters for wearable and stretchable electronics: from flexibility to stretchability. Adv Mater 28:9881–9919
Zener CM (1948) Elasticity and anelasticity of metals. University of Chicago Press, Chicago
Zhao X, Koh SJA, Suo Z (2011) Nonequilibrium thermodynamics of dielectric elastomers. Int J Appl Mech 3:203–217
Zhou J, Jiang L, Cai S (2020) Predicting the electrical breakdown strength of elastomers. Extreme Mech Lett 34:100583
Ziegler H (1958) An attempt to generalize Onsager’s principle, and its significance for rheological problems. Z Angew Math Phys 9b:748–763
Ziegler H, Wehrli C (1987) The derivation of constitutive relations from the free energy and the dissipation function. Adv Appl Mech 25:183–238
Funding
This work was supported by the National Science Foundation through Grants CMMI–1661853 and DMREF–1922371.
Author information
Authors and Affiliations
Corresponding author
Ethics declarations
Conflict of interest
The authors declare that they have no conflict of interest.
Additional information
Publisher's Note
Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
Appendix. The reduced dissipation inequality
Appendix. The reduced dissipation inequality
Denote by \({\mathbf{v}}({\mathbf{x}},t)\) the velocity of the material point that occupies the location \({\mathbf{x}}\in {\Omega }(t)\) at time \(t\in [0,T]\) and assume that at any \({\mathbf{x}}\in {\Omega }(t)\) and time \(t\in [0,T]\) the following quantities exist and are sufficiently regular both in space and time: the mass density \(\rho ({\mathbf{x}},t)\), the mechanical Cauchy stress \({\mathbf{T}}^m({\mathbf{x}},t)\), the mechanical body force \({{\mathbf {f}}}^m({\mathbf{x}},t)\) (per unit volume), the electric force \({{\mathbf {f}}}^e({\mathbf{x}},t)\) (per unit volume), the electric couple \({\mathbf{g }}^e({\mathbf{x}},t)\) (per unit volume), the electric field \({\mathbf{e }}({\mathbf{x}},t)\), the electric displacement \({\mathbf{d }}({\mathbf{x}},t)\), the space charge \(q({\mathbf{x}},t)\) (per unit volume), the internal energy \(u({\mathbf{x}},t)\) (per unit mass), the heat source \(r({\mathbf{x}},t)\) (per unit mass), the heat flux \(\widetilde{{{\mathbf {q}}}}({\mathbf{x}},t)\), the entropy \(\eta ({\mathbf{x}},t)\) (per unit mass), and the absolute temperature \(\theta ({\mathbf{x}},t)\).
1.1 Conservation of mass
Conservation of mass is said to be satisfied provided that
1.2 Balance of linear and angular momenta
Absent inertia, the balance of linear and angular momenta are said to be satisfied provided that
and
where \(\widetilde{\varvec{\varepsilon }}\) stands for the permutation symbol.
In the context of electro-quasi-statics of interest here, the electric force and couple take the form (see, e.g., Eqs. (7.38) and (7.48) in [35])
where we recall that \({\mathbf{p }}={{\mathbf {d}}}-\varepsilon _0{{\mathbf {e}}}\) stands for the polarization.
Upon defining the electric stress
and invoking Gauss’s (A.6) and Faraday’s (A.7) laws introduced further below, the balance of linear (A.2) and angular (A.3) momenta can be recast as
and
in terms of the total Cauchy stress \({\mathbf{T}}={\mathbf{T}}^m+{\mathbf{T}}^e\). With help of the connections (6) and the definition \({{\mathbf {f}}}=J{{\mathbf {f}}}^m\), Eqs. (A.4)–(A.5) can be further recast as those summoned in the main body of the text, namely, (11).
1.3 Maxwell’s equations
In the context of electro-quasi-statics of interest here, Maxwell’s equations are said to be satisfied provided that
and
With help of the connections (6) and the definition \(Q=J q\), Eqs. (A.6)–(A.7) can be recast in the form (12) provided in the main body of the text.
1.4 Balance of energy
Granted the balance Eqs. (A.1), (A.2), (A.3), (A.6), (A.7), balance of energy is said to be satisfied provided that
where \({{\mathbf {\Gamma }}}=\partial {\mathbf{v}}({\mathbf{x}},t)/\partial {\mathbf{x}}\) stands for the Eulerian velocity gradient.
Throughout this appendix, a superposed “dot” denotes the material time derivative.
1.5 Entropy imbalance
Granted the balance Eq. (A.1), the entropy imbalance is said to be satisfied provided that
Upon defining the free energy (per unit mass)
and invoking the balance Eq. (A.8), the entropy imbalance (A.9) can be recast as the reduced dissipation inequality
which, in the context of isothermal processes of interest in this work, specializes to
With help of the definition
and the connections (6), the reduced dissipation inequality (A.10) can be further recast as
Writing now
and making use of the connections (3)–(5), the inequality (A.11) reduces finally to the form (10) provided in the main body of the text.
Rights and permissions
About this article
Cite this article
Ghosh, K., Lopez-Pamies, O. On the two-potential constitutive modeling of dielectric elastomers. Meccanica 56, 1505–1521 (2021). https://doi.org/10.1007/s11012-020-01179-1
Received:
Accepted:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s11012-020-01179-1