SHAPE MEMORY POLYMER ACTUATORS

Abstract

Resistive heating elements are embedded in a shape memory polymer actuator. Sensing elements are associated with the resistive heating elements. The sensing elements sense changes in the resistive heating elements and correlate the changes with deformation of the shape memory polymer actuator.

Claims

1. An assembly comprising: resistive heating elements embedded in a shape memory polymer actuator, called an SMPA; and sensing elements associated with said resistive heating elements, said sensing elements configured to sense changes in said resistive heating elements and to correlate said changes with deformation of said SMPA.

2. The assembly according to claim 1, wherein said sensing elements comprise electrical resistance sensors configured to sense changes in electrical resistance of said resistive heating elements.

3. The assembly according to claim 1, wherein upon deformation of said SMPA, an amount of contact points at which said resistive heating elements contact each other changes.

4. The assembly according to claim 1, wherein said resistive heating elements comprise carbon fiber-based resistive heater elements, and upon deformation of said SMPA, a density of π electrons of said carbon fiber-based resistive heater elements changes.

5. The assembly according to claim 1, comprising a power supply controller coupled to said SMPA, and wherein electrical resistance output of said SMPA is coupled to said controller as a feedback to control a degree of deformation of said SMPA.

6. The assembly according to claim 1, wherein said SMPA is coated with a metallic layer that reflects radiative heat energy emitted by said SMPA back to said SMPA.

7. The assembly according to claim 1, wherein said SMPA is part of a low earth orbit space device.

Description

BRIEF DESCRIPTION OF THE DRAWINGS

[0011] The present invention will be understood and appreciated more fully from the following detailed description taken in conjunction with the drawings in which:

[0012] FIGS. 1A-1D are prior art illustrations of molecular structure of:

[0013] FIG. 1A: EPON 826 resin; FIG. 1B: JEFFAMINE D230 Polyetheramine crosslinker; FIG. 1C: N-Phenylaminopropyl AM0281 POSS cage; and FIG. 1D: schematics of a carbon fiber structure [19].

[0014] FIGS. 2A-2C are illustrations of (FIG. 2A) epoxy-carbon SMPA (including a resistive heater with a w-like architecture), (FIG. 2B) aluminum-coated epoxy-carbon SMPA, and (FIG. 2C) epoxy-reference and POSS-epoxy samples.

[0015] FIGS. 3A-3B are illustrations of (FIG. 3A) bending by INSTRON machine at 130° C., and (FIG. 3B) recovery parameters superimposed on an SMPA installed in a vacuum chamber.

[0016] FIGS. 4A-4D are illustrations of macroscopic SME by resistive heating at ambient pressure conditions: FIG. 4A: Beginning of test, SMPA in its temporary shape; FIGS. 4B and 4C: After 3 and 6 min, respectively, from the beginning of the resistive heating, and FIG. 4D: Full deployment to permanent shape.

[0017] FIGS. 5A-5D are illustrations of: FIG. 5A: 1.sup.st stage results, resistance versus temperature during oven heating of the SMPA; FIG. 5B: 2.sup.nd stage results, resistance versus deflection during bending of the preheated SMPA at 130° C.; FIG. 5C: 3.sup.rd-stage results, resistance versus temperature during cooling of the SMPA; FIG. 5D: 4.sup.th stage results, resistance versus deflection during recovery of the SMPA by resistive heating.

[0018] FIGS. 6A-6E are illustrations of: FIG. 6A: SMPA after bending and cooling; FIG. 6B: Buckling of the carbon fibers due to compression stress; FIG. 6C: The SMPA after recovery; FIGS. 6D-6E: Micro- and nano-meter scale HRSEM images of carbon fibers, respectively.

[0019] FIG. 7 is an illustration of a phenomenological model, which demonstrates the major parameters that influence the SMPA's electrical resistance during bending, on the micro- and macro-structure levels.

[0020] FIGS. 8A-8D are illustrations of recovery of the SMPAs at ambient and vacuum conditions, with and without aluminum (Al) coating, wherein FIG. 8A shows recovery angle change (Δθ) versus deployment time, FIG. 8B shows Δθ versus deployment power, FIG. 8C shows angular velocity versus deployment time, and FIG. 8D shows resistance versus Δθ.

[0021] FIGS. 9A-9D are illustrations of SME of 15 wt. % POSS-epoxy SMP sample in its (FIG. 9A) initial permanent shape, before SME; (FIG. 9B) temporary shape; and (FIG. 9C) final permanent shape, after SME; and FIG. 9D shows samples' mass loss versus LEO equivalent AO fluence.

[0022] FIGS. 10A-10E are illustrations of: SME of 15 wt. % POSS-epoxy SMP sample in its (FIG. 10A) initial permanent shape, before SME; (FIG. 10B) temporary shape; and (FIG. 10C) final permanent shape, after SME; and FIG. 10D shows samples' mass loss versus LEO equivalent AO fluence HRSEM images of (a, c) epoxy reference and POSS-epoxy SMPs, respectively, before exposure to AO, and (b, d) epoxy reference and POSS-epoxy SMPs, respectively, after exposure to LEO equivalent AO-fluence of 1×10.sup.20 O-atoms/cm.sup.2; and FIG. 10E shows a high-resolution image of the POSS-epoxy SMP after exposure to LEO equivalent AO.

DETAILED DESCRIPTION OF EMBODIMENTS

[0023] Adhesive for the SMPA was prepared from EPON 826 DGEBA resin (Momentive, Inc.) and JEFFAMINE D230 Poly(propylene Glycol)bis(2-Aminopropyl) Ether crosslinker agent (Huntsman Chemicals, Inc.). AM0281 N-Phenylaminopropyl POSS cage mixture additive (Hybrid Plastics, Inc.) was mixed with the amino-based crosslinker to create 15 wt. % POSS-epoxy actuator. The chemical structures of these materials are shown in FIGS. 1A-1D. In addition, 3k-70-p, type 2, grade 3, class 1 polyacrylonitrile (PAN)-based carbon fiber yarn (Hexcel Inc.) was used.

[0024] Four types of epoxy-based SMPAs were prepared using an aluminum mold, in which carbon fibers were immersed into the cavity, and epoxy adhesive was poured above. The materials used for the various SMPs and SMPAs prepared in this work are summarized in Table 1.

[0025] Epoxy resin was mixed with the crosslinker agent in a volume ratio of 2.52:1, respectively [in accordance with ref. 20]. Both materials were preheated to 50° C. and added to a vial. The vial was first shaken vigorously by hand, and then by Vortex shaker for 1 minute at 30 rpm. Next, the vial was placed in a vacuum oven, which was preheated to 50° C., for degassing at a pressure of less than 10 mmHg. After 13 minutes, the vial was taken out, and the adhesive was ready to be poured into the mold.

TABLE-US-00001 TABLE 1 Composition of the epoxy based SMPs and SMPAs. EPON AM0281 826 JEFFAMINE POSS Carbon Aluminum SMP/SMPA (wt. %) D230 (wt. %) (wt. %) fiber coating Epoxy- 75.5 24.5 — — — reference POSS-Epoxy 67.6 17.4 15.0 — — Epoxy-carbon 75.5 24.5 — ✓ — Aluminum- 75.5 24.55 — ✓ ✓ coated Epoxy- carbon

[0026] Before pouring the adhesive, the molds, having inner dimensions of 70×10×1 mm.sup.3, were coated with a WATERSHIELD release agent (Zyvax, Inc.). In the next stage, the carbon fibers were connected to electrical wires and were placed in the mold. Next, 0.8 mL of the adhesive was poured into each mold. The epoxy adhesive was thermally cured at 100° C. for 1.5 h, and post-cured at 130° C. for another 1 h [in accordance with ref. 20]. Upon completion of curing, the mold was cooled to room temperature (RT), and the epoxy-based SMPAs were demolded. FIG. 2a depicts the SMPA scheme, including the resistive heaters' w-like architecture. Some of the samples were coated with 100 nm thick aluminum coating, using electron beam physical vapor deposition (EBPVD) at 1 Å/s rate, 2×10.sup.−6 Torr, and RT conditions, as schematically illustrated in FIG. 2b. Additional samples of pristine epoxy and POSS-epoxy were prepared in the same manner, without carbon fibers and without aluminum coating, see FIG. 2c. The POSS additive was pre-mixed with the crosslinker at 50° C. A molar ratio of 1:1 was kept between the primary amine groups of the crosslinker and the amine groups from the POSS that replaced them, while the overall POSS content was set to 15 wt. %.

[0027] The SMP samples and SMPAs were deformed to a u-like shape using 3-point bending grips, mounted on an INSTRON 3365 universal machine, equipped with an environmental chamber and a 100 N load cell. The bending was performed by using a 22.8 mm radius “upper nose”, see FIG. 3a. This setup was used for fixing the SMPAs in their temporary shape, at a temperature of 130° C., using the environmental chamber, and then cooling to RT while keeping the SMPAs under load. The SMPAs were deflected to a maximum strain of 2.4% at 0.4 mm/min crosshead speed and 42 mm support span. 2.4% strain is equivalent to 9.5 mm deflection, according to Equation 1 [in accordance with ref. 21].

[00001]$\begin{array}{cc}\mathrm{.Math.}=\frac{6\mathrm{Dd}}{L^2}\times 100& \left(1\right)\end{array}$

[0028] where ε (%) is strain, D (mm) is the deflection, d (mm) is the thickness of the sample, and L (mm) is the support span.

[0029] The SME of the SMPAs was measured either at ambient pressure or in vacuum (5.5×10.sup.−4 Torr) using resistive heating. The recovery effect was recorded by a video camera, and was quantified by the following values: recovery angle (Δθ) and deflection (D), see FIG. 3b, where at t=0, Δθ=0° and D=D.sub.max.

[0030] The surfaces of the SMP samples were characterized by a high-resolution scanning electron microscope (HRSEM) equipped with a secondary electrons detector (model Sigma 300 VP from Zeiss). Images of the epoxy reference and POSS-epoxy samples were collected in a variable pressure mode. This enabled measurements of the insulating samples without the application of a conductive coating [compare ref. 22].

[0031] The durability of the reference and POSS-containing epoxy SMP samples to AO attack was measured by a ground-based AO simulation facility that is based on a radio frequency (RF) plasma source (Litmas RPS). The source operates at a maximum power of 3 kW, a frequency of 1.7-3.0 MHz, and an O.sub.2 feed. During the experiment, the samples were held in the RF plasma source vacuum chamber for a total exposure time of 260 h; they were removed periodically from the vacuum chamber for measurement of their mass loss. The mass loss is used to calculate the material's LEO equivalent AO-fluence. The experiment parameters were: pressure of 6×10.sup.−2 Torr, power of 810 W, and O.sub.2 flow rate of 12 sccm. Under these conditions, a current of 20 μA was measured between the sample holder and the ground, using a picoammeter (model 485 from Keithley). This current was used to monitor the RF plasma performance.

[0032] The LEO equivalent AO-fluence was calculated by measuring the mass loss of a Kapton sample, which was simultaneously exposed to the AO beam, assuming an erosion yield of 3×10.sup.−24 cm.sup.3/O-atoms [23], see Equation 2 [in accordance with ref. 17].

[00002]$\begin{array}{cc}F=\frac{\Delta m}{\rho \mathrm{AE}}& \left(2\right)\end{array}$

[0033] where Δm is the mass loss (g), A is the material's exposed area (cm.sup.2), ρ is the material's density (g/cm.sup.3), F is the equivalent AO fluence (O-atoms/cm.sup.2), and E is the erosion yield (cm.sup.3/O-atom).

[0034] FIG. 4 depicts a visual description of the shape recovery of the SMPA. In this experiment, the SME was obtained by resistive heating under ambient pressure conditions. The current was increased gradually at a constant rate of 0.03 A/min to avoid uneven heat distribution and, as a result, uneven strains that can lead to local failures. Full recovery was accomplished after 7 min, using resistive heating current of 0.21 A, see FIG. 4d. The recovery effect started just after the actuator reached a temperature equal to the glass transition temperature of the epoxy.

SMPA Recovery Control Through Electrical Resistance Measurements

[0035] During bending and shape memory recovery cycles of the SMPA, changes between the electrical resistance at the permanent and the temporary shapes, as well as at different temperatures, were observed. Hence, it was decided to study the influence of bending and temperature on the electrical resistance of the actuators while separating these variables. This methodology was used to control the recovery angle, and may be used in future space deployable mechanisms to control a deployment process. In order to investigate the effect of temperature and bending on the actuators' electrical resistance, an experiment was performed in four stages: 1) heating, 2) bending, 3) cooling, and 4) recovery by resistive heating. The resistance was calculated using Ohm's and Pouillet's laws, see Equation 3 [in accordance with ref. 24, 25].

[00003]$\begin{array}{cc}R=\frac{V}{I}=\frac{\rho L}{A}& \left(3\right)\end{array}$

[0036] where R (Ω) is the resistance, V (V) is the voltage, I (A) is the current, ρ (Ω.Math.m) is the resistivity, L (m) is the length, and A (m.sup.2) is the cross-sectional area.

[0037] FIG. 5a shows the electrical resistance as a function of temperature at the 1.sup.st stage during oven heating of the SMPA in its permanent shape. During heating to a temperature of 130° C., its resistance increased by 77%, from 66 Ω to 117 Ω. This increase is composed of two phases. The first shows a relatively small increase in resistance, from 66 Ω to 72 Ω as the SMPA is heated from RT to 110° C. Above 110° C., an abrupt increase in resistance is observed, reaching 117 Ω at a temperature of 128° C. This phenomenon has been previously observed for epoxy resins filled with carbon fibers at various aspect ratios [refs. 26, 27]. While the first phase depicts the resistance change due to the change in the graphite fiber metallic conductivity, the second abrupt increase in resistance is associated with mechanical changes in the epoxy resin itself. The actuator's semicrystalline carbon fibers contain unordered plains of hexagonally arrayed sp.sup.2 carbon atoms sheets. Electrical current passes through the carbon fiber by π electrons, below and above these sheets (parallel to the basal xy plane). The mobility of the π electrons is similar to the behavior of electron gas in metals [ref. 28]. During the first phase, while heating the SMPA in the environmental chamber, electron scattering increases due to increased thermal vibrations of the atoms, i.e., collisions between the electrons and the phonons, and lattice irregularities, e.g., vacancies [refs. 24, 29], resulting in smaller electron mean free path (MFP) [ref. 28]. The abrupt increase in resistance during the second phase of the heating process is associated with mechanical changes in the epoxy resin itself. The reason for this positive temperature coefficient (PTC) effect is the breaking-off of inter-fiber contacts. The carbon fibers embedded in the epoxy are composed of micron-sized filaments, with a very small distance between them. When the polymer matrix shrinks during the curing and final cooling processes, residual compressive strain is stored in the polymer gap between the fibers, as the carbon fibers were pushed together. During heating, as the material becomes rubbery, the thermal expansion of the epoxy will compensate for the residual strain, and at a critical temperature will lead to the separation of the fibers, thus lowering the number of inter-fiber contacts. Consequently, the temperature at which the PCT effect occurs is highly dependent on the curing temperature. In this case, the epoxy was cured at 100° C. and 130° C.; therefore the PCT effect started at an intermediate temperature, and was observed above 110° C. Thus, during the 1.sup.st stage, the dominant mechanism that affects the SMPA's resistivity is electron scattering and reduction of inter-fiber contacts, which increases the resistivity during the heating [ref. 25].

[0038] According to Equation 3, the resistance may also be affected by dimensional changes in the carbon fiber's length and cross-section area. In order to evaluate the influence of the temperature on these parameters, the linear expansion was calculated according to Equation 4 [in accordance with ref. 30]:

[00004]$\begin{array}{cc}\Delta L=L_0\mathrm{\alpha \Delta }T& \left(4\right)\end{array}$

[0039] where ΔL is the dimensional change, L.sub.0 is the initial dimension, α is the coefficient of thermal expansion, and ΔT is the temperature change.

[0040] The carbon fiber's coefficient of thermal expansion in its z direction is extremely low and negative, −4.1×10.sup.−7° C..sup.−1 [31]; it is about 2×10.sup.−5° C..sup.−1 in its x or y directions [in accordance with ref. 28]. The length of the carbon fiber is 26 cm per SMPA, whereas the typical cross-sectional area of a single fiber filament is 38.5 μm.sup.2 [in accordance with ref. 31]. Therefore, the fiber's longitudinal thermal dimensional change is 13.7 μm, merely 5×10.sup.−3% change. The thermal expansion of the fiber's cross-sectional area was also very small, only 0.2%. Thus, through the 4 stages of the SMPA recovery control experiment, L was set constant, and in stage 1 the cross-sectional area was considered constant too.

[0041] FIG. 5b shows the 2nd-stage results of resistance versus deflection measurements during bending of the SMPA to its temporary u-like shape. An increase in the resistance by 9.1%, from 117 Ω to 128 Ω, was measured. This increase may be due to two possible reasons. First, a sufficient number of fractured carbon monofilaments, or disconnection of nearby filaments at certain points, due to the bending, may lead to lower cross-sectional area for electron current, if those filaments became electrically disconnected [in accordance with ref. 32]. Second, the carbon fiber buckling deformation, which occurred during the bending test [in accordance with refs. 33, 34], as shown in FIG. 6a and b. In the z-direction (normal to the graphitic basal planes), the spacing between the graphite sheets presumably becomes larger due to buckling. Hence, the density-of-state of the π electrons decreased, and higher resistance was measured as the electrons were forced to move a larger distance from one graphite sheet to the other [ref. 29]. FIG. 6d presents HRSEM images of the carbon fibers, demonstrating the inter-fiber contact points between nearby filaments. FIG. 6e presents the HRSEM image of a single filament composed of interconnected fibrils having diameters of 20-50 nm.

[0042] FIG. 5c depicts the electrical resistance as a function of temperature in the 3.sup.rd stage during cooling of the SMPA to RT in its temporary shape. During cooling, the resistance of the bended SMPA decreased by 32%, from 128 Ω to 87 Ω. During cooling, one parameter may lead to an opposite effect that may increase the actuator resistivity and, hence, its resistance. This parameter concerns the residual stresses that may increase between the matrix and the fibers during cooling due to the shrinkage of the thermoset matrix around the fibers [ref. 35], thus increasing the buckling effect. However, the actual decrease in the resistance during cooling indicates that another, more dominant, parameter exists. It is assumed that this parameter is the reduction in electron-scattering events. At lower temperatures, fewer electron-scattering events occur and, hence, the resistivity and resistance decrease [refs. 24, 25, 28].

[0043] FIG. 5d depicts 4.sup.th-stage results of resistance versus deflection measurements during recovery of the actuator to its permanent shape by gradual resistive heating. The resistive heating itself is a result of retarding forces and collisions involving charge carriers, usually electrons [ref. 24]. A drastic decrease in the resistance by 23%, from 70 Ω to 54 Ω, after deployment of less than 1 mm was observed. This drastic decrease may be attributed to two factors. First, when the SMPA reached the glass-transition temperature, the residual stresses and the buckling deformation were released immediately as SME started, leading to closer graphite aligned sheets, higher density of π electrons and, thus, lower resistivity. Second, instant alternative connecting points are formed between the carbon fibers during the deployment of the SMPA in the initial deployment stage, which leads to higher cross-sectional area for electron current and, hence, the electrical resistivity and resistance decrease. FIG. 6c demonstrates the disappearance of the carbon fibers' buckling at the end of the SME. The phenomenon of instant decrease in electrical resistance during the SMPA's deployment may be used for indication and control of the SMPA deployment process while in space.

[0044] FIG. 7 presents a phenomenological model, which demonstrates the major parameters that influence the SMPA's resistance during bending, on the micro- and macro-structure levels. This model demonstrates the structure-property dependency, which leads to the resistance decrease during deployment, by using three hierarchies: actuator level, carbon fiber macrostructure level, and graphite sheets molecular level. The actuator level depicts the permanent and the temporary shapes of the actuator, and the associated buckling effect. The carbon fiber macrostructure level shows the fibers in the aligned and buckled position. The circles around the monofilaments depict the monofilament-to-monofilament electrical contact points, and the rectangles show monofilaments fractured due to bending. In the permanent shape, a larger number of contact points exist between the monofilaments. During bending, the monofilaments are far apart, and some of them are fractured. The molecular level depicts the plains of graphite sheets in the carbon monofilament and the π electrons below and above these sheets. The distance between the sheets becomes larger (L.sub.temporary>L.sub.permanent) during bending, hence the density-of-state of the π electrons presumably decreased.

[0045] Although heating per se increases the carbon fibers' resistivity, during recovery by resistive heating, resistivity decreases sharply. The dominant parameters during recovery, which lead to this decrease in the resistance, are the increase in the number of the inter-fiber contacts and the density of the it electrons.

The Kinetics of SMPAs in Space-Simulated Conditions

[0046] The dominant heat transfer mechanisms are different under ambient and under vacuum conditions. At ambient pressure, the dominant mechanisms of heat transfer to the surrounding atmosphere are convection and conduction, while in vacuum the main mechanism is radiation [ref. 36]. The influence of the vacuum effect on the SMPAs' deployment kinetics was tested in order to simulate the UHV conditions in LEO. In addition, in order to improve the energetic efficiency of the SMPAs' deployment, a novel approach was developed, which is based on an internal reflectance heating mechanism. Implementation of this mechanism was done by coating the SMPAs with a 100 nm aluminum coating. Aluminum offers high reflectivity in the near-IR and, hence, can be used as solar reflector of the IR photons, which are emitted during the resistive heating process.

[0047] The SMPAs were recovered in both ambient and vacuum conditions, while aluminum-coated SMPAs were recovered only in vacuum conditions. FIG. 8 presents the recovery kinetic parameters of the SMPAs under both ambient and vacuum conditions, with and without aluminum coating. Each curve is the average of three experiments. FIG. 8a depicts the SMPAs' deployment kinetics in terms of recovery angle change (Δθ) versus time. The maximum bending angle was defined as Δθ=0°. FIG. 8b shows the SMPAs' deployment kinetics in terms of Δθ versus the actuator's power consumption. FIG. 8c presents the angular velocity (dθ/dt) versus deployment time, while FIG. 8d presents the SMPAs' electrical resistance versus Δθ. FIG. 8a-c show a general trend in all 3 cases of almost instantaneous deployment that occurred after a certain dwell time. The highest values of 310 s dwell time, 97 s recovery duration, and 2.46 W recovery power were observed at ambient pressure for the epoxy-carbon SMPA. Performing the epoxy-carbon SMPA deployment experiment under vacuum conditions resulted in moderate values of 224 s dwell time, 72 s recovery duration, and 1.53 W recovery power. The lowest values of 171 s dwell time, 71 s recovery duration, and 1.17 W recovery power were observed under vacuum conditions by the aluminum-coated epoxy-carbon SMPA. These results prove the benefit of coating the SMPAs with aluminum, as deployment power consumption (under vacuum conditions) dropped by 25% as a result of this process.

[0048] During the recovery stage, electrical current passes through the carbon fibers and produces resistive heating. In this test, the current was set to produce a temperature of around 130° C., above the glass transition temperature of the SMPA. According to Wein's law [37], at this temperature the emitted heat from the actuator has a typical wavelength of 7.2 μm. At ambient pressure, the SMPA loses heat through convection to the surrounding air and, hence, longer time and higher power are needed to heat it. Under vacuum conditions, the aluminum-coated SMPA preserved its temperature by internal radiative heating process. In this process, the emitted photons were reflected back to the bulk polymer by the solar reflective aluminum coating. In this manner, the aluminum coating preserved the temperature as a solar-reflective element and reduced the electric power consumption, as shown in FIG. 8b.

[0049] The results presented in FIG. 8c show that at ambient pressure, the epoxy-carbon had the longest dwell time, lowest angular velocity, and wider velocity distribution. In vacuum, the maximum velocity was higher, and the distribution of the angular velocity was symmetric and narrow. These results indicate that the deployment in vacuum occurred at a short and specific period of time when reaching the glass transition temperature. The deployment was even shorter for the aluminum-coated epoxy-carbon SMPA. The values of the angular velocity were 2.75°/s for the epoxy-carbon SMPA at ambient pressure, 3.5°/s for the epoxy-carbon SMPA in vacuum, and 6°/s for the aluminum-coated epoxy-carbon SMPA in vacuum.

[0050] FIG. 8d shows the electrical resistance versus recovery angle change of the SMPAs at ambient and vacuum conditions, with or without aluminum coating. A sharp decrease in the resistance at the beginning of the deployment, and a lower decrease during the rest of the deployment, are evident. Furthermore, the highest resistance was obtained under vacuum conditions for the aluminum-coated epoxy-carbon SMPA. The lowest resistance was measured under ambient conditions for the epoxy-carbon SMPA. The decrease in the actuator's resistance was due to the release of the buckling deformation and the residual stresses, as analyzed previously in Section 3.2. The higher the temperature of the SMPA, the higher its resistance, as shown in FIG. 5a. The aluminum-coated epoxy-carbon SMPA operated under vacuum conditions reached the highest temperature due to internal IR reflections, and therefore showed the highest measured resistance. The epoxy-carbon SMPA operated in ambient conditions reached the lowest temperature, due to heat losses through convection and conduction to the surrounding atmosphere, and therefore showed the lowest measured resistance.

[0051] To briefly summarize this part, the main heat transfer mechanisms for the SMPA in ambient condition are convection and conduction to the surrounding air. In vacuum condition, the main heat transfer mechanism is radiation; hence, heat losses are much smaller. As a result, the energy consumption in vacuum conditions is also much smaller. Coating the epoxy-carbon SMPA with aluminum further decreases its energy consumption by internal radiation, which further decreases heat losses. Hence, internal aluminum coating can save power during the deployment process in space.

POSS-Epoxy SME and Durability to AO

[0052] Incorporation of POSS monomers into the epoxy adhesive by copolymerization may improve its durability to AO attack by formation of SiO.sub.2 passivation layer. The AO oxidizes the SiO.sub.1.5 POSS into SiO.sub.2 [16]. Hence, reference and POSS-containing epoxy SMP samples were exposed to oxygen RF-plasma, which simulates AO irradiation. The SMP samples were removed periodically from the system for a short period of time in order to measure their mass loss. Prior to the AO exposure, the SME of the POSS-epoxy sample was verified. The POSS-epoxy SMP sample was exposed to an elevated temperature of 100° C. in a hot bath, bended to a u-like temporary shape, fixed in its temporary shape in a cold bath, and exposed again to an elevated temperature until SME occurred and the sample returned to its permanent shape, see FIG. 9a-c. As shown, the POSS-epoxy sample fully recovered to its original permanent shape, exemplifying the potential of this nano-composite material system as an SMP.

[0053] FIG. 9d depicts the mass loss (Δm) of epoxy-reference and POSS-epoxy SMPs during ground-based AO-irradiation, as a function of the LEO equivalent AO fluence. The epoxy reference mass loss under a LEO equivalent AO fluence of 2.6×10.sup.20 O-atom/cm.sup.2 was 3.95 mg/cm.sup.2. In comparison, the POSS-epoxy SMP mass loss under the same LEO equivalent AO fluence was only 1.17 mg/cm.sup.2, a reduction of 70% compared to the epoxy-reference SMP. Furthermore, while the mass loss of the epoxy-reference versus the LEO equivalent AO fluence was linear, the mass loss of the POSS-epoxy decreased gradually as the LEO equivalent AO fluence increased. This implies a gradual formation of a SiO.sub.2 passivation layer during the AO irradiation [3].

[0054] FIG. 10 shows HRSEM images of the surface morphology of epoxy reference and POSS-epoxy SMPs, before and after AO attack. Before AO attack, smooth surfaces are shown (FIG. 10a and c) for both epoxy and POSS-epoxy samples. After AO attack, the epoxy-reference surface was eroded to a carpet-like morphology (FIG. 10b), while the surface of POSS-epoxy is characterized by a sponge-like morphology formed presumably by the SiO.sub.2 self-passivating network (FIG. 10d and e) [16], which increased its durability to AO attack.

[0055] Unique epoxy-carbon SMPAs were designed as building blocks for future space applications. Their SME parameters, electrical properties, as well as their durability in vacuum and AO environments, were evaluated. During resistive heating and deployment, a rapid decrease in the SMPAs' electrical resistance occurs. This effect is caused by temperature and by the SMPAs' deflection state. During deployment, the carbon fibers abruptly unbuckle, compression stresses are immediately released, and new electrical connecting points are formed between the fibers. Therefore, the carbon fibers serve two purposes—heating elements as well as deployment control detectors. The SMPAs' resistance measurement can serve as an important tool for controlling the recovery angle during deployment in space.

[0056] During resistive heating and deployment of the SMPA, electrical current passes through the carbon fibers and produces heat. At ambient pressure, the actuator loses heat mainly by convection and conduction to the surrounding environment; hence, long time and relatively high power are needed. In vacuum conditions, the deployment of the SMPA is faster and consumes less power (because less heat is lost), as the main mechanism of heat transfer to the surrounding environment is radiation. When the novel aluminum-coated SMPA is deployed in vacuum conditions, the coating preserves the SMPA's temperature more efficiently by an internal radiative heating process, as photons are reflected back to the bulk polymer by the reflective aluminum coating. In this manner, the aluminum coating can save power during the deployment process.

[0057] Copolymerization of POSS monomers with epoxy increases their AO erosion durability and reduces mass loss during irradiation by 70%. The surface of the AO post-irradiated POSS-epoxy is characterized by a sponge-like morphology. These results indicate the formation of a SiO.sub.2 passivation layer, which increases the POSS-epoxy SMP durability to AO.

[0058] It is important to note that the references mentioned above are only mentioned for ways to measure values or for reference purposes, and in no way anticipate the invention or make the invention obvious.

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