Evaluation of the deformation shape of a balloon-type dielectric elastomer actuator prestretched with water pressure

Abstract

In this study, we evaluated the deformation shape of a balloon-type dielectric elastomer actuator (DEA) that has been prestretched with water pressure. We fabricated the DEA with poly(dimethylsiloxane) (PDMS) as the elastomeric material and carbon grease as the electrode. We derived analytical solutions for the deformation of the DEA based on structural mechanical models. Additionally, we compared the deformation shapes obtained by theoretical analysis and experimental results. Our model can partially predict the deformation shape of the DEA with good accuracy. In addition, we discuss the applicable range of the theoretical model and error relative to the experimental results.

Introduction

Recently, soft actuators have attracted considerable attention because they have the potential to realize biomimetic soft mechanisms [1, 2] or to be used in various new applications, such as human machine cooperation [3] or low-invasive medical robots [4]. Various types of soft actuators have been proposed that are driven by pneumatic [5, 6], electrical [7,8,9], thermal [10, 11], or optical [12, 13] inputs. Among these types of soft actuators, electrically-driven soft actuators generally have advantages of fast response, small size, low weight, and large deformation. Dielectric elastomer actuators (DEAs) are one type of electrically driven soft actuator. They are driven by high voltage ($\approx$ kV), consist of commercially available soft polymer materials, and are easily fabricated due to their simple structures [14,15,16]. Since DEAs can be utilized in dry environments, they are potential candidates for practical applications in soft actuators.

Generally, DEAs are composed of thin planar dielectric elastomer materials sandwiched by flexible electrodes on both sides of the elastomer. When we apply a high electric voltage ($\approx$ kV) between the electrodes, the dielectric elastomer becomes thinner but extends in the planar direction because of Maxwell stress between the electrodes. Thus, DEAs are normally actuated in the in-plane direction of the sheet of DEA and are installed in mechanical structures to generate bending motion for practical applications, such as artificial muscles [17,18,19] or fish robots [20,21,22]. Here, we note that one important drive condition of a DEA is prestretching of the dielectric elastomer materials. To generate large deformations, dielectric elastomers should be stretched prior to actuation. Most DEAs are stretched in the in-plane direction by using mechanical jigs, which restricts the motions of DEAs in the in-plane direction. Another way to prestretch DEAs is to use air pressure [23] or water pressure [24]. When air or water pressure is applied to a DEA, the shape of the DEA is deformed like a balloon. Thus, the directions of actuation of these types of DEAs are intrinsically out-of-plane and can be applied to loud speakers [25], fluid pumps [26], or tactile presentation devices [27].

For detailed studies on prestretched DEAs with air or water pressure, there are several studies on the drive characteristics of balloon-type DEAs [25, 28,29,30]. These studies have experimentally evaluated static behaviors [30] or dynamic behaviors [25], or have numerically simulated dynamic characteristics of balloon-type DEAs [28, 29]. However, numerical simulations cannot predict the deformation shape of balloon-type DEAs according to various design values, such as diameter, thickness, and pressure [31, 32]. Thus, to design balloon-type DEAs with desired deformation shapes, a predictive analytical model of DEAs with various design parameters must be developed.

In this paper, we perform theoretical and experimental analyses of balloon-type DEA deformations. First, we theoretically and experimentally evaluate static characteristics of DEAs with uniaxial load and compare the results. Second, we derive analytical solutions of the deformations of a balloon-type DEA with water pressure and electric voltage under two assumptions; (i) employing a flexural model of a circular plate and spherical shell in structural mechanics for the analysis, (ii) employing linear constitutive law (Hooke’s law) to derive analytical solutions. Then, we compare the analytical results with the experimental results of various sizes of balloon-type DEAs prestretched with water pressure and discuss the validity and applicable range of the model.

Evaluations of DEA with uniaxial load

First, we evaluated DEAs with uniaxial load, which is a commonly used system to evaluate basic characteristics of DEAs. In this study, we used polydimethylsiloxane (PDMS) (Silpot 184, Toray Dow Corning, Tokyo, Japan) for both DEA samples prestretched with a uniaxial load and with water pressure. PDMS is a transparent and heat-curable silicone elastomer and is known to have high formability and a high dielectric coefficient. Furthermore, PDMS is also known to have relatively linear mechanical characteristics over a small deformation region of up to $\approx$ 50% [33, 34]. This DEA with a uniaxial load was evaluated to confirm the linearity of PDMS as a DEA material. For the theoretical analysis of the deformation shape of the DEA in the next section, we assumed that PDMS has linear characteristics.

Fabrication of DEA

For fabrication of a thin membrane of PDMS, we use a spin coating method commonly used in microfabrication. Liquid PDMS is applied to a polystyrene sheet substrate and spin coated at 1500 rpm for 30 s. Afterwards, liquid PDMS on the substrate were baked at 80 °C for 2 h in a constant-temperature oven. Then, we obtained a PDMS membrane with a thickness of approximately 100 $\upmu$m. Finally, the surface of the DEA was coated with carbon grease (MG846-80G, MG Chemicals, Burlington, Canada) as the electrode. We fabricated DEAs at thicknesses of 80, 100, 120 $\upmu$m by changing the preparation conditions. For each thickness, three samples were fabricated and evaluated.

Experimental system for uniaxial load

A fabricated PDMS membrane was fixed with fixing jigs as shown in Fig. 1a, b. This fixing jigs are made of acrylic plate and sandwiches fabricated PDMS membrane. Furthermore, we put thin PDMS sheets on the fixing jigs to increase friction forces between the jigs and PDMS membrane and firmly fix the PDMS membrane. Additionally, copper tapes were attached to both sides of the PDMS and used for connection to a power supply. This DEA was attached to an aluminum frame and a weight was hanged to the bottom fixing jig to apply uniaxial load. For electric voltage application, we used a function generator (AFG3022C, Tektronix) to generate the input signal. The input signal was connected to a high-voltage amplifier [HOPP-5P(A), Matsusada precision, Shiga, Japan]. In this study, we varied the voltage from 0 to 3.0 kV. Actuator displacement was acquired using digital cameras (DC-TZ90, Panasonic, Osaka, Tokyo) and measured using visual analysis software Image J [35, 36].

Fig. 1

Experimental system of uniaxial load. a Schematic figure of the experimental system, b picture of the actual experimental system, c schematic figures of deformation of a DEA with uniaxial load

Theoretical model of DEA with uniaxial load

Under the assumption that PDMS obeys linear constitutive law (Hooke’s law), the relationship between strain of PDMS $s_t$ and voltage V can be written as follows with a simple capacitor model.

$$\begin{aligned} s_t = \frac{\varepsilon _r\varepsilon _0}{E}\frac{V^2}{t^2}. \end{aligned}$$

(1)

Here, $\varepsilon _0$ is permittivity of vacuum, E is the Young’s modulus of the material, V is an applied electric voltage, and t is a thickness of PDMS. $\varepsilon _r$ is relative permittivity, which is 2.72 for Silpot 184. We used this Eq. (1) to evaluate the drive characteristics of the DEA with a uniaxial load.

To determine strains $s_t$ of DEA in the experiments, we calculated $s_t$, as shown in Fig. 1c. The DEA has three phases: first phase without a load (Fig. 1c-1), “off” phase with a load (Fig. 1c-2) and “on” phase with a load and electric voltage (Fig. 1c-3). Here, $l_1$, $l_2$, $l_{1_{off}}$, $l_{2_{off}}$, $l_{1_{on}}$ and $l_{2_{on}}$ are the electrode widths of every phase, and $t_0$, $t_{off}$ and $t_{on}$ are the thickness of the elastomer. When we assume that the elastomer is non-compressible, the elastomer volume $v=l_1l_2t_0$ is constant for every phase. Then, we can calculate elastomer thickness at the on phase $t_{on}$ by measuring widths and heights of the electrode $l_{1_{off}},l_{2_{off}},l_{1_{on}},l_{1_{on}}$. As a result, we can experimentally calculate thickness strain of the elastomer $s_t$ with the following equations.

$$\begin{aligned} t_{off} = \frac{v}{l_{1_{off}}l_{2_{off}}},&\qquad t_{on} = \frac{v}{l_{1_{on}}l_{2_{on}}}\nonumber \\ s_t =&\frac{t_{off}-t_{on}}{t_{off}} \end{aligned}$$

(2)

Results

Figure 2 shows the experimental results of the actuation of DEA with uniaxial load. To evaluate the strain characteristics of PDMS, we set $V^2/t^2$ as the horizontal axis and $s_t$ on the vertical axis in Fig. 2. By setting this horizontal axis, this plot should be linear, according to Eq. (1), if the Young’s modulus E is constant. In this case, we can estimate the Young’s modulus E from the slope of the line.

Fig. 2

Results of experimental and theoretical analyses of DEAs with a uniaxial load

In Fig. 2, experimental results of DEA with 80 $\upmu$m, 100 $\upmu$m, and 120 $\upmu$m are shown in green, blue, and red cross points, respectively. Also, we plotted the approximate line linearized by a least-squares method, which is shown as a solid line for each color. From this approximation, the slopes were 1.98, 2.60, and 1.78 $\times \, 10^{-17}$ for DEA with thicknesses of 80 $\upmu$m, 100 $\upmu$m, and 120 $\upmu$m, respectively. From these results, the Young’s modulus of the fabricated PDMS varied from 0.825 to 1.21 MPa. These values are thought to vary due to the curing conditions or fabrication error of the thickness. For theoretical analysis in the next section, we use 0.80 MPa as the value of the Young’s modulus of PDMS.

Evaluations of DEA only with water pressure

Second, we evaluated the deformation of DEA with water pressure, which is the main target of this study. The systems were previously reported by Godaba et al. [37] to realize large deformation in the out-of-plane direction of a DEA. In this study, we fabricated balloon shaped DEAs made of PDMS and evaluated the deformation shape.

Fabrication of DEA

For the fabrication of thin membranes of PDMS, we used a spin coating method similar to the DEA with uniaxial load in the previous section. In this case, we fabricated DEAs with thicknesses of 100 $\upmu$m, and three samples were fabricated and evaluated at each condition.

Experimental system for water pressure

For prestretching with water pressure, we used an experimental system to apply water pressure by connecting a water reservoir and a circular pipe with a hose, as shown in Fig. 3a, b. The fabricated PDMS membrane was affixed to an acrylic pipe. After that, the surface of the DEA was coated with carbon grease. In this study, we used acrylic pipes with diameters of 18.0, 24.0, and 32.0 mm.

Fig. 3

Experimental system of DEA actuation with water pressure. a Schematic of the experimental system. b Photograph of the experimental system, c DEA without electric voltage, d DEA with electric voltage

In using this system, water pressure for prestretching can be changed by the height of water in the reservoir. Water pressure p applied to DEA is determined as follows.

$$\begin{aligned} p = \rho g (h_1-h_2) \end{aligned}$$

(3)

Here, $\rho$ is density of water, g is acceleration of gravity, $h_1$ and $h_2$ are heights of water in the reservoir and the pipe, as shown in Fig. 3a. Additionally, water was also used as an electrode to apply electric voltage to the DEA. We connected the grand electrode of the high voltage amplifier to the water reservoir.

Analytical solution of the deformation of DEAs only with water pressure

To theoretically analyze deformations of DEAs with water pressure, we employed following two assumptions; (i) PDMS membrane is analyzed by using a flexural model of a circular plate. (ii) PDMS membrane has linear constitutive law (Hooke’s law). We assume PDMS has linear elastic properties in our model because PDMS is known to have linear characteristics until $\approx$ 50% deformation [33, 34], as we confirmed in the previous section. To analyze deformations of DEA, we consider that there are three phases of DEA actuation in our system, as shown in Fig. 4a. First, before applying water pressure to the membrane, the membrane had a circular disk shape, as shown in Fig. 4a, b. Second, when we applied water pressure to the membrane, the membrane expanded as a curved surface, and the displacement was determined as $\delta _1 (r)$, as shown in Fig.4a, c. Here, r is the radial coordinate of the circular plate. Third, when we applied electric voltage to the membrane, it expanded further according to the electrostatic voltage, and we determined this displacement as $\delta _2 (r)$, as shown in Fig.4a, d. Therefore, total displacement of the DEA $\delta (r)$ is written as follows and it is a function of r.

$$\begin{aligned} \delta (r) = \delta _1 (r)+\delta _2 (r) \end{aligned}$$

(4)

We analyzed the deformation of the DEA by using two models: (i) circumferentially supported disk model with distributed load for water pressure: $\delta _1 (r)$ (Fig.4c) and (ii) the curvature shell model with distributed load for an electric voltage: $\delta _2 (r)$ (Fig.4d) [33].

Fig. 4

Analysis model of DEA prestretched with water pressure. a Schematic of three phases of the DEA, structural mechanics model for: b pre-water pressure application, c post-water pressure application, d post-water pressure and electric voltage application

We assume that the membrane is a disk supported at its circumference, and the distributed load is applied to the disk to express prestretching with water pressure, as shown in Fig. 4c. Normally, deflection $\delta _1 (r)$ can be calculated by solving infinitesimal deformation models of the disk. However, when the out-of-plane deformation of the disk is larger than the thickness of the disk, the infinitesimal deformation model is not valid and this large deflection can be solved by using the energy method [38]. Thus, we employed the energy method for the analysis of our system. Considering conservation of energy, deflection energy of the disk U is a sum of bending energy $U_1$ and expanding energy $U_2$ and these can be written as follows.

$$\begin{aligned} U_1&= \frac{1}{2}\int _0^{2\pi } \int _0^a \left( M_r\frac{1}{R_1}+{M_\theta }\frac{1}{R_2}r \right) d{\theta }dr \end{aligned}$$

(5)

$$\begin{aligned} U_2&= \frac{1}{2} \int _0^{2\pi } \int _0^a \left( N_r {\varepsilon }_r + N_{\theta } {\varepsilon }_{\theta } r \right) d{\theta }dr \end{aligned}$$

(6)

Here, $M_r$ and $M_{\theta }$ are bending moments, $R_1$ and $R_2$ are curvature radii in r and $\theta$ directions, respectively. Also, $N_r$, $N_{\theta }$ are stresses and ${\varepsilon }_r$, ${\varepsilon }_{\theta }$ are strains of the middle surface in the r and $\theta$ directions, respectively. By using a relationship of bending moments $M_r$, $M_\theta$, curvature radii $R_1$, $R_2$, and bending rigidity $D = Et^3/12(1-\nu ^2)$, $U_1$ can be written as follows.

$$\begin{aligned} U_1 = -\frac{D}{2}\int _0^{2\pi } \int _0^a \Biggl [ \left( \frac{1}{R_1} +\frac{\nu }{R_2} \right) \frac{1}{R_1} \nonumber \\ +\left( \frac{1}{R_1} + \frac{\nu }{R_2} \right) \frac{1}{R_1} \Biggr ] rd{\theta }dr \end{aligned}$$

(7)

Here, $\nu$ is the Poisson’s ratio of the material. Furthermore, curvatures $R_1$ and $R_2$ can be rewritten by derivatives of deflection ${\delta }_1$ by using geometric relationships as follows.

$$\begin{aligned} U_1 = {\pi }D\int _0^a \Biggl [ \left( \frac{d^2 \delta _1}{dr^2} \right) ^2 + \frac{1}{r^2} \left( \frac{d{\delta }_1}{dr} \right) ^2 \nonumber \\ +2\nu \frac{1}{r} \frac{d{\delta }_1}{dr} \frac{d^2{\delta }_1}{dr^2} \Biggr ] rdr. \end{aligned}$$

(8)

Next, $U_2$ can be written as follows by using a relationship between stress $N_r$, $N_\theta$, and strain $\varepsilon _r$, $\varepsilon _\theta$.

$$\begin{aligned} U_2 = \frac{{\pi }tE}{(1-{\nu }^2)} \int _0^a \left[ (\varepsilon _r+\varepsilon _\theta )^2-2(1-\nu ) {\varepsilon }_r {\varepsilon }_\theta \right] rdr \end{aligned}$$

(9)

When we set a displacement in the radial direction as u(r), $\varepsilon _\theta$ and $\varepsilon _r$ can be written by using u(r) as follows.

$$\begin{aligned} {\varepsilon }_{\theta }&= \frac{2{\pi }(r+u)-2{\pi }r}{2{\pi }r}=\frac{u}{r}, \end{aligned}$$

(10)

$$\begin{aligned} {\varepsilon }_r&= \frac{du}{dr}+\frac{1}{2} \left( \frac{d{\omega }}{dr} \right) ^2 \end{aligned}$$

(11)

Thus, $U_2$ can be rewritten as the following equation by using Eqs. (9), (10) and (11), as follows.

$$\begin{aligned} U_2 =&\frac{{\pi }Et}{1-{\nu }^2}\int _0^a\Biggl [ \left( \frac{du}{dr}\right) ^2 +\frac{1}{4} \left( \frac{d{\delta }_1(r)}{dr}\right) ^4 \nonumber \\&+\frac{du}{dr} \biggl (\frac{d{\delta }_1(r)}{dr}\biggr )^2 +\frac{u^2}{r^2} \nonumber \\&+2{\nu } \frac{u}{r} \left\{ \frac{du}{dr}+\frac{1}{2} \left( \frac{d{\delta }_1 (r)}{dr}\right) ^2 \right\} \Biggr ]rdr. \end{aligned}$$

(12)

Here, we assume that the deflection of the disk $\delta _1 (r)$ can be written as follows, which is written in analogously to the infinitesimal deformation model.

$$\begin{aligned} {\delta }_1 (r) = {\delta }_1 (0) \left( 1-\frac{r^2}{a^2} \right) ^2 \left( 1-\frac{5+\nu }{1+\nu } \frac{r^2}{a^2}\right) \end{aligned}$$

(13)

In our model, a circumferential supported disk with distributed load should not deform at the center and circumference in the radial direction. Thus, radial displacement u(r) can be written under these boundary conditions as follows.

$$\begin{aligned} u&= r(a-r)(c_0+c_1 r+c_2 r^2+\cdots ) \nonumber \\&= c_0 a r + (ac_1 - c_0) r^2 + \cdots \end{aligned}$$

(14)

Here, $c_0$, $c_1$, $c_2\cdots$ are undetermined constants, and we used the second-order term of this equation in this study. $c_0$ and $c_1$ can be determined as the strain energy U, which become the minimum turning points as follows.

$$\begin{aligned} \frac{dU}{dc_0} = 0,{\qquad } \frac{dU}{dc_1} = 0. \end{aligned}$$

(15)

Then, we acquire following values for $c_0$ and $c_1$ by calculating integral of Eq. (12).

$$\begin{aligned} c_0 = 0.799 \frac{\delta _1(0)^2}{a^3}, \quad c_1 = -0.148 \frac{\delta _1(0)^2}{a^4} \end{aligned}$$

(16)

Here, we used the value of $\nu = 0.5$. By using these values of $c_0$ and $c_1$ , we can calculate $U_1$ and $U_2$ as follows.

$$\begin{aligned} U_1&= 0.441 \pi \frac{Et^3}{a^2}\delta _1(0)^2 \end{aligned}$$

(17)

$$\begin{aligned} U_2&= 0.402 \pi \frac{Et}{a^2} \delta _1(0)^4 \end{aligned}$$

(18)

Virtual work W by external force p can be calculated as:

$$\begin{aligned} W = \int _0^{2{\pi }}\int _0^a p{\delta _1(r)}rd{\theta }dr = \frac{5}{11} \pi a^2 p \delta _1 (0). \end{aligned}$$

(19)

By using Eqs. (17)–(19), the minimum deflection energy $U_{min}$ can be derived by the following equation.

$$\begin{aligned} \frac{d(U_{min}-W)}{d{\delta }_1 (0)} = 0 \end{aligned}$$

(20)

From this condition, we acquire the following equation.

$$\begin{aligned} 0.882\frac{E}{a^2}t^3 \delta _1(0) + 1.61\frac{E}{a^2}t \delta _1(0)^3 =\frac{5}{11}a^2 p \end{aligned}$$

(21)

In the case of the deflection $\delta _1 (0)$ is much larger than the thickness of the disk t, the first term is negligible. This approximation is equivalent to ignore the bending energy $U_1$. Then, we acquire the maximum deflection ${\delta }_1(0)$ by solving Eq. (21) and it can be written as follows.

$$\begin{aligned} \delta _1 (0) = 0.657a \left( \frac{pa}{Et} \right) ^{\frac{1}{3}}. \end{aligned}$$

(22)

From Eqs. (13) and (22), $\delta _1(r)$ can be written as follows.

$$\begin{aligned} \delta _1(r) = 0.657a \left( \frac{pa}{Et}\right) ^{1/3} \left( 1-\frac{r^2}{a^2} \right) ^2 \left( 1-\frac{11}{3}\frac{r^2}{a^2}\right) \end{aligned}$$

(23)

Results

Then, we experimentally and theoretically evaluated the deformation of DEA with prestretching by water pressure. Figure 5a, b are typical examples of ${\delta }_1 (r)$ acquired by experimental and theoretical calculations. These results were acquired with conditions of $p=1.37$ (kPa), $a=16.0$ (mm), $\nu = 0.5$, and $E=0.80$ (MPa). The experimental picture from the side and the perspective view of theoretical results seem to be in a good agreement with these shapes. Additionally, the maximum displacements at the top of the DEA $\delta _1 (0)$ are 7.84 mm in experiments and 7.71 mm in analysis, and these values agree well.

Fig. 5

Evaluation of DEA with water pressure. a Experimental picture of DEA with a water pressure of 1.37 kPa. b 3D plot of the analytical solution of Eq. 23. c Comparison of theoretical and experimental data with changing diameter a. d Comparison of theoretical and experimental data with changing pressure p

Next, we compared the experimental results and theoretical results with various diameters of acrylic pipes and water pressures. Figure 5c, d show the cross-sectional view of the $\delta _1 (r)$ at the center of the DEA. In the results in Fig. 5c, water pressures of 1.37 kPa were applied to DEA with diameters of acrylic pipe $a =$ 9, 13, 16 mm. Additionally, In Fig. 5d, water pressures of 1.17 kPa, 1.27 kPa, and 1.37 kPa are applied to DEA with an acrylic pipe radius of 16 mm. These results, especially the results of $a =$ 9 and 13 mm in Fig. 5c, theoretical and experimental are quantitatively in good agreement.

Evaluation of DEA with water pressure and electric voltage

Analytical solution of deformation of DEA with water pressure and electric voltage

To evaluate the deflection $\delta _2$ of the membrane with water pressure and electric voltage, we again employed following two assumptions similar to the previous section; (i) PDMS membrane is analyzed by using a flexural model of a spherical shell. (ii) PDMS membrane has linear constitutive law (Hooke’s law). We treat the electrostatic force generated by applying electric voltage as a distributed load on the membrane. First, we assumed the equilibrium of the force of infinitesimal area, as shown in Fig. 4d-2. The area is subjected to forces in the circumferential $N_\theta$ and meridional directions $N_\phi$, and electrostatic force is applied in the normal direction of the area Z. These forces are written as follows.

$$\begin{aligned} N_\theta = \frac{r_2}{2}Z,{\qquad }N_\phi = -\frac{3}{2}r_1Z \end{aligned}$$

(24)

Here, $r_1$, $r_2$ are curvature radii in each direction. These forces cause strain $\varepsilon _\theta$, $\varepsilon _\phi$ in each direction and these are written as follows.

$$\begin{aligned} \varepsilon _ \theta = \frac{\nu }{r_2} \cot \phi -\frac{{\delta }_2 (\phi )}{r_2 },{\quad } \varepsilon _ \phi = \frac{1}{r_1} \frac{dv}{d\phi }-\frac{\delta _2 (\phi )}{r_2} \end{aligned}$$

(25)

where v is displacement in the tangential direction of the meridian and $\delta _2$ is the displacement of the normal direction of the middle surface. By using Hooke’s low, these equations can be written as follows.

$$\begin{aligned} \varepsilon _ \theta = \frac{1}{Et}(N_{\phi }-{\nu }_{\theta }),{\quad } \varepsilon _ \phi = \frac{1}{Et}(N_\theta - \nu N_{\phi } ) \end{aligned}$$

(26)

Here, t is the thickness of the membrane. Then, deflection of the shell $\delta _2 (\phi )$ is derived by Eqs. (24), (25) and (26), as follows.

$$\begin{aligned}\delta _2(\phi ) & = \frac{r^2 \cos ^2\phi }{1-r^2 \cos ^2\phi }\frac{1}{Et} \nonumber \\ & \quad \times \left[ r_1 (N_\phi -\nu N_\theta ) -\frac{r_2}{\cos ^2\phi (N_\theta -\nu N_\phi )}\right] \end{aligned}$$

(27)

Finally, we acquired the equation of deflection of the DEA $\delta (r)$ as a function of water pressure p and electrostatic force Z is written as follows.

$$\begin{aligned} \delta (r) & = \delta _{1(r)} + \delta _{2(r)} = \delta _{1(r)}+\delta _{2} (\phi ) \cos \phi \\ & = 0.657a \left( \frac{pa}{Et}\right)^{{\frac{1}{3}}} \left( 1-\frac{r^2}{a^2} \right) ^2 \left( 1-\frac{11}{3}\frac{r^2}{a^2}\right) \\ & \quad + \frac{r^2 \cos ^3 \phi }{1-r^2\cos ^2\phi } \frac{1}{Et} \\ & \quad \times \left[ \frac{r_1}{2} (r_2+1.5r_1)Z-\frac{2r_2}{\cos ^2\phi (r_2+1.5)Z} \right] ,\\ Z & = \varepsilon _r \varepsilon _0 \frac{V^2}{t^2} \end{aligned}$$

(28)

Here, $\varepsilon _r$ and $\varepsilon _0$ are dielectric permittivity of PDMS and vacuum, respectively.

Results

Then, we also experimentally and theoretically evaluate the deformation of DEA with water pressure and electric voltage. Figure 6a, b are typical examples of $\delta (r)=\delta _1(r) + \delta _2 (r)$ that are acquired by experiments and theoretical calculations, respectively. These results were acquired with conditions of $p = 1.37$ (kPa), $a = 16$ (mm), $\nu = 0.50$, $E = 0.80$ (MPa) and $V = 3.0$ (kV). The experimental picture and theoretical results seem to be in good agreement with these shapes. Additionally, the maximum displacement at the top of the DEA $\delta (0)$ was 8.99 mm in the experiments and 8.84 mm in analysis. The values of deformation $\delta (0)$ acquired with experiments and theoretical calculations are slightly different.

Fig. 6

Evaluation of DEA with water pressure and electric voltage. a Experimental picture of DEA with a pressure of 1.37 kPa and electric voltage 3.0 kV. b Theoretical data with the same conditions as the experiments in a. c Comparison of experimental and theoretical data with changing voltage

Next, we compared experimental results and theoretical results with various electric voltages. Figure 6c shows the cross-sectional view of the $\delta (r)$ at the center of the DEA. In the results in Fig. 6c, water pressure $p=$ 1.37 (kPa), and electric voltage V is varied as 1.0, 2.0, and 3.0 kV. These experimental and theoretical results are qualitatively in agreement but the values are a little different. This difference is thought to be caused because of assumptions of our model. We assume that the actuator has shapes of a part of spherical shell and uniform thickness, as shown in Fig. 4d. However, actual actuators might have different shapes and non-uniform thicknesses.

We also evaluated the maximum deflections at the center of the DEA $\delta (0)$, by applying electric voltage from 0 to 3.0 kV, as shown in Fig. 7. From Fig. 7, the maximum differences of theoretical values from experimental values are $+0.40/-0.15$ mm and these values are $+5.15/-1.64$% of $\delta (0)$. Thus, our model is suitable for predicting the values of the maximum deformation $\delta (0)$ of the DEA in our system.

Fig. 7

Maximum deflection $\delta$(0) acquired by experiments and theoretical calculations with varies electric voltage 0 kV to 3.0 kV

Discussion

Here, we note the actual values of strains of PDMS and discuss the applicable range of our model. Basically, we analyzed the deformation of DEA by assuming that PDMS has linear mechanical characteristics. References [33, 34] shows that PDMS has almost linear mechanical characteristics up to 50% strain. Thus, we derived the deformation of DEA with water pressure and electric voltage with a constant Young’s modulus. By using this model, we acquired quantitatively good results in $a =$ 9 and 13 mm conditions in Fig. 5c. However, the results in $a =$ 16 mm and the theoretical results are a little different from experimental values. It is thought to be because of the large deformation of the PDMS.

Thickness strains of PDMS in conditions of $a =$ 9 and 13 mm in Fig. 5c are 53.7% and 56.4%, respectively. These values exceed the value 50%. However, the results of deformation in these conditions are quantitatively in good agreement with experiments. On the other hand, thickness strain of PDMS in condition of $a =$ 16 mm in Fig. 5c is 57.1% and theoretical results in this condition are quantitatively in not good agreement with experiments. Thus, the thickness strain $\approx$ 55% is thought to be a border of the applicable range of our model assuming linear mechanical characteristics of PDMS. Under this value of thickness strain, our model is thought to be applicable to quantitatively predict deformation shapes of the balloon-type DEA made of PDMS. These limitation can be resolved by introducing nonlinear characteristics of the material as studied in Ref. [39] However, for larger strain as shown in Figs. 6 and 7, the deformation shapes of the theoretical results are qualitatively in agreement with the experimental value and maximum deformation $\delta (0)$ can be acquired within the error of $+5.15/-1.64$%.

Conclusions

In this study, we analyzed deformation shape of balloon-type DEA prestretched with water pressure. We derived the analytical solution of the deformation shape based on structural mechanics. We evaluated deformation of the balloon-type DEA with theoretical calculations and experiments and compared them. Theoretical results of our model are quantitatively in good agreement with experimental results up to $\approx$ 55% of thickness strains. Thus, the model can be used to design the balloon-type DEA with desired deformation.