Electrostatic Zipping
Maxwell stress (electrostatic pressure) between electrode-covered areas exceeds the hydraulic restoring pressure of the fluid → electrodes zip together → fluid displaced toward unelectroded region → pouch contracts laterally.
Rectangular Pouch
Flat rectangular pouch; electrodes cover approximately half the length (L_e ≈ L_p/2). Unzipped region bulges into a circular segment. Kellaris (2019) analytic model: voltage → force/stroke.
Dielectric Fluid Advantage
Unlike solid DEAs, HASELs use liquid dielectric oil. Pinhole breakdowns self-heal as oil fills the gap. Key advantage for longevity in underwater or harsh environments.
Capacitance Change Mechanism
Zipped area acts as a parallel-plate capacitor: C = ε₀ε_r·w·l_e / 2t. As more electrode area zips, capacitance increases. Unzipped region contributes negligible capacitance (Kellaris 2019). C_max/C_min ≈ 11.7× for commercial HASELs.
Inertial vs. Viscous
Per Rothemund (2020): τ_v/τ_i = μwL^½/Mg^½. Inertial regime → t_n ∝ L^½, independent of viscosity. Artimus commercial HASELs operate in the inertial regime — response determined by inertia of the oil, not its viscosity.
Artimus Robotics
Denver, CO. Commercial Peano-HASEL with thin-film unipolar design. 8-channel ARDI power supply used for Nebula v2. Self-sensing via AC impedance built into their newest multi-channel supplies.
HASEL Material Parameters
Euler-Bernoulli Beam
Small-deflection assumption. Variable bending stiffness EI(x) and mass per unit length m(x). Augmented with nonlinear terms (Aureli 2012, Ramananarivo 2013) for large-amplitude cases.
Lighthill + Nonlinear Damping
Lighthill (1971) elongated-body theory provides reactive (added mass) and resistive forces. Aureli (2012) nonlinear cubic damping term accounts for vortex shedding at moderate amplitudes and Keulegan-Carpenter numbers.
Linearized Potential Flow
Garrick (1936) / Theodorsen unsteady lift on an oscillating flat plate. Valid at low reduced frequencies. Validated against LDV data from an aluminum propulsor in UF water tunnel.
Galerkin Projection
PDE projected onto N vacuum mode shapes as basis functions. Reduces to N coupled ODEs. Root-finding handles frequency-dependent nonlinear eigenvalue. N = 20 basis functions used for Nebula simulations.
Complex Orthogonal Decomposition
Ti ∈ [0,1] quantifies the proportion of traveling vs. standing waves in the response waveform. Ti = 0 → pure standing wave; Ti = 1 → pure traveling wave. Method from Feeny (2008), used in Musgrave (2021) and Hess (2022).
MAC — Modal Assurance Criterion
MAC ∈ [0,1] measures correlation between a simulated mode shape and the corresponding experimentally measured mode shape. MAC = 1 → perfect agreement; MAC < 0.5 → poor agreement. Nebula Mode 1 MAC = 0.989.
Governing Equation Summary
F_fluid (quiescent) = m_f(x) Γ(ω) ∂²w/∂t² + m_f(x) Δ(β,ε) ∂²w/∂t² [Aureli 2012]
M_HASEL = ∂²/∂x² [ θ(x) χ_p(x) V(t) ] [linearized HASEL constitutive relation]