HB-CESIC COMPOSITE FOR SPACE OPTICS AND STRUCTURES

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16 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS HB-CESIC COMPOSITE FOR SPACE OPTICS AND STRUCTURES Matthias R. Krödel * Tsuyoshi Ozaki ** * ECM Ingenieur-Unternehmen für Energie- und Umwelttechnik GmbH, Ridlerstr. 31d, D-80339 Munich, Germany + 49/8123/4045 or kroedelm@ec-muenchen.de ** Advanced Technology R&D Center, Mitsubishi Electric Corporation, 1-1-57 Miyashimo, Sagamihara, Kanagawa, 229-1195, Japan Keywords: Ceramic material, Composite material, Mirror, low CTE, SiC, Cesic Abstract One of the key technologies for next generation space telescopes requiring largescale reflectors are light-weight materials having high specific strength, high specific stiffness, low coefficient of thermal expansion and high coefficient of thermal conductivity. Several candidates, such as fused silica, beryllium, silicon carbide and carbon fiber reinforced composites, have been evaluated. An example of the latter material is a Hybrid Carbon-Fiber Reinforced SiC composite or HB-Cesic a trademark of ECM which has been developed by ECM and MELCO to meet the stringent space telescope requirements. Mechanical performance, such as stiffness, bending strength and fracture toughness, were significantly improved using HB-Cesic compared to our classic Cesic material. Thermal expansion and thermal conductivity of HB-Cesic at cryogenic temperatures are now partly established and excellent performance for large future space mirrors and structures are expected. In this paper we will report on the current status of development of HB-Cesic and describe the first successful applications made with this new improved material. 1. Introduction to HB-Cesic HB-Cesic is a ceramic matrix composite that is manufactured by ECM. It is characterized by high stiffness and mechanical strength, high thermal conductivity, low thermal expansion, and quick, relatively inexpensive manufacturing times. These characteristics make HB-Cesic an ideal material at reasonable cost for large highprecision space optical and structural applications. The starting material in the manufacturing of HB-Cesic is a short, chopped, randomly oriented carbon fiber material. A typical microstructure is shown in the following figure. Fig. 1. REM microphotograph of the greenbody The fibers are mixed with a phenolic resin and molded into a blank, which then is heattreated under vacuum. The result is a lightweight, porous, relatively brittle C/C greenbody (Fig. 1). At the present time circular blanks are available in sizes up to 1 m, with a thickness up to 200 mm. In the future greenbody blocks up

to 2 m in size or larger will become available as circular or square blocks. Through the use of ECM s large CNC controlled milling machine of 2.5 x 1.75 m, we are able to manufacture large lightweighted monolithic structures, such as mirrors and components for optical benches. For example, in the manufacture of optical mirrors, curved face sheets (including off-axis designs) can be machined with reinforcing ribs as thin as 1 mm and of any geometry, including ribs with holes or with T-shape. Upon machining the greenbody is infiltrated under vacuum conditions with liquid silicon at temperatures above 1600 C. Capillary forces wick the silicon throughout the porous greenbody, where it reacts with the carbon matrix and the surfaces of the carbon fibres to form carbon-fiber reinforced SiC -- HB-Cesic. The density of the infiltrated HB- Cesic composite is typically 2.98g/cm³. After controlled cool-down, the HB- Cesic structure is carefully examined visually and/or by other NDT methods such dye penetrant or ultrasonic tests. The HB-Cesic structure can then be micro-machined with suitable diamond tools or by EDM machining to achieve the required surface figure and interface geometry (e.g., mirror adaptation and mounting). EDM machining is possible because of HB-Cesic 's electrical conductivity. This machining method is fast compared to grinding, it is relatively inexpensive, and it yields a surface and location (e. g., screw holes and mounts) accuracy of about 10 µm tolerance over a large area. Manufacturing times of HB-Cesic mirrors and other structures are typically only a few weeks, upon procurement of the C/C raw material, which is much shorter than the manufacturing times of other ceramic or glass structures. Highly complex and large projects take somewhat longer, e.g., mirrors with closed backs, meter-plus-class mirrors that require precision joining of the greenbody or infiltrated segments, and large multi-segmented optical benches. The maximum size of HB-Cesic components is only limited by the size of the Si-infiltration furnaces. ECM's current largest furnace has a useable diameter of 2.4 m with up to three levels, each of height 1.2 m. In the following figures the large ECM facility for infiltration is shown. Fig. 2. ECM XL facility for infiltration Fig. 3. Heater unit designed for best thermal homogeneity 2. C/C material for HB-Cesic In the past three years ECM and MELCO developed a new improved C/C raw material compared to the ECM classic C/C material for Cesic in order to improve the homogeneity

and thermo-mechanical characteristics of the final, Si-infiltrated product, especially for cryogenic mirror applications. The following figure shows the manufacturing process of the new C/C raw material: Molding Heat treatment Raw materials prior to molding CFRP Preform C/C Green Body Fig. 4. Manufacturing process of the new C/C raw material We call the new composite material HB- Cesic to distinguish it from our classic Cesic material (type MF Cesic ). As we will describe in Section 4, we have conducted several tests of the new HB-Cesic material and demonstrated that it possesses superior mechanical and thermal performance characteristics compared to classic Cesic. Thus, ECM can propose with confidence HB- Cesic for future cryogenic ultra-lightweighted mirrors and structures. This C/C raw material is composed out of a mixture of different chopped short carbon fibers and this is the reason why it is called hybrid (HB). 3. Manufacturing process of HB-Cesic The machining of greenbodies uses standard tooling and technologies, such as ECM s 3-D CAD/CAM controlled machine, to mill, turn and drill holes. All light-weighting operations are also done in the greenbody stage and, therefore, are fast compared to the volume of carbon to be removed. The C/C greenbody is not fragile, so very thin walls can be machined as, for example, ribs down to 1 mm thickness with a height of up to 120 mm. The possibility of manufacturing very thin plates and complex shaped elements and of joining at the greenbody stage before or after machining allows the rapid manufacture of complex, ultralightweighted HB-Cesic mirrors and structures, to meet the challenges of future space requirements. Greenbody blocks can be joined by gluing after machining, but before Si-infiltration, which allows the manufacture of large, monolithic HB-Cesic components. Siinfiltration transforms the glued section into HB-Cesic without any discontinuities. In the near future, we plan to carry out bending tests of samples manufactured from continuous and joined C/C greenbodies to confirm, as in the case of our classic Cesic material, that joining does not introduce any mechanical or thermal discontinuities. After greenbody machining the C/C greenbody is infiltrated at high temperature with liquid silicon. This is a cost effective and fast process with a rapid heat cycle, the cold to cold cycle duration being less than 72 hours. One of the main advantages of the HB- Cesic manufacturing process is the very low shrinkage during infiltration of only 0.6% ±0.05% compared to other silicon carbide materials, some of which have a shrinkage up to 20 % with a deviation of ±1%. I.e., our process is near-net-shape. The low shrinkage of HB-Cesic during infiltration allows a highly accurate prediction of the machining at the greenbody stage, limiting the final overthickness needed for corrective machining after infiltration. This small shrinkage also limits residual stresses during infiltration and cooldown, as all the parts of the structure undergo only very small contractions. 3.1. Final maching of HB-Cesic to prepare high precision interfaces After infiltration, HB-Cesic components can be machined with high accuracy and 3

without any risks using Electro-Discharge Machining (EDM). The ability to EDMmachine HB-Cesic components is due to the material s good electrical conductivity, which is rather high for a ceramic and a major advantage compared to other silicon carbide materials. EDM-machining allows no risk, highprecision finishing of surfaces in local areas inside and outside the structure in preparation for adding screw inserts or bolting fixation devices. It can also be used to reduce section or thickness at the final machining stage and to make, for example, integrated filtering blades (mounting devices) on mirrors, as we successfully demonstrated with our classic Cesic in past programs. Of course, HB-Cesic can be also ground by traditional techniques over large surface areas. 3.2. HB-Cesic mirrors polishing of surfaces In the past year ECM and MELCO investigated the polishing performance of HB- Cesic mirrors. For mirrors of sizes up to 160 mm we demonstrated that bare HB-Cesic surfaces i.e., surfaces without any cladding or overcoatings can be polished to a surface roughness of 3-5 nm rms. The following picture shows an optical measurement of the micro-roughness of a bare HB-Cesic surface. 4. Material characterization and thermomechanical properties ECM and MELCO have recently measured several mechanical and thermal properties of HB-Cesic : CTE near RT CTE from RT down to 100K initial tests 4-point bending Young s modulus 4.1. CTE measurement facility The CTE measurements were done in a cryo chamber, which is shown in the following picture. The test facility is located at Mitsubishi Electric Corporation, Japan. Fig. 6. Laser thermal expansion indicator, LIX-1(ULVAC) Fig. 5. HB-Cesic Microroughness Fig. 5. HB-Cesic Microroughness The total number of HB-Cesic samples measured was six: 3 samples in the X-direction and 3 samples in Y-direction. The samples shape is illustrated in Fig. 7, with sizes 3t x 5w 15L according to Melco internal standards, corresponding to 3 x 5 x 15 mm.

15 13 Fig. 7. Shape of the CTE samples The measurement principle of the facility is shown in the next picture. 3 complete initial temperature uniformity. With these test conditions we were able to successfully obtain an overall thermal deformation between 300 K and 110 K with an accuracy of about 0.1 micron, 5 The results of the CTE measurements are shown in the next two figures. 250 200 Laser Reflection 1 Chamber Specimen Reflection 2 Strain, ppm 150 100 50 0 100 150 200 250 300 Temperature, K X- 1 X- 2 X- 3 Fig. 8. Measurement principle To avoid any impact of the environment on the measurements such as vibration, the whole measurement system was isolated using rubber pads and placed on a stiff optical bench table. From the data, CTE is calculated as: CTE= 4.2 Results of CTE-testing (Displacement change) (Distance between targets) x (Temperature change) Before the start of the measurements, the system was calibrated with a specified aluminum sample, for which the exact cryo data were available. After this calibration, the HB-Cesic samples were installed in the cryo chamber. For all the CTE-measurements, just one silicon diode was used for the measurements of the HB-Cesic samples and one for the copper plate temperature. Both diodes were calibrated before measurements. Before cooling to cryogenic temperatures, the samples were maintained at a temperature of 310 K for two hours to achieve Strain, ppm 250 200 150 100 50 0 Fig. 9. CTE in X-direction 100 150 200 250 300 Temperature, K Y- 1 Y- 2 Y- 3 Fig. 10. CTE in Y-direction 4.3 Four-point bending test of HB-Cesic 4.3.1 Test Set-up Description The bending tests for HB-Cesic were performed at Thales Alenia Space (TAS), Cannes, France: Compression/strain machine: Zwick Z250 Strength sensor: 100 kg Acquisition system: MGC Catman, Solartron captor conditioner 5

Loading speed: 0.5 mm/min NIRSpec bending tool, two superior points articulated Span length: 40mm/ 80mm Log radius: 20 mm LVDT sensor placed under the sample in order to measure precisely the displacement in the load axis. Articulated points LVDT sensor Fig. 11. Sample in 4-point bending test configuration at TAS. Test-setup shown is for a sample of length 240 mm. The HB- Cesic tests were made with samples of length 120 mm 4.3.2 Sample Description The tests were performed on HB-Cesic samples with the dimensions 120 x 20 x 3 mm. The surface of load implementation (120 x 20 mm) and the length side (120 x 3 mm) were ground. 4.3.3 Test Results Direction Strength (MPa) Modulus(GPa) XY 266 351 Z 244 337 Table 1. Mechanical results of 4-point bending test 4.3.4 Comparison to Classic Cesic (type MF) The following table compares Young s modulus and 4-point bending strength of classic Cesic (type MF) and HB-Cesic. Cesic MF HB-Cesic Increase to Cesic MF E XY 258 351 36% E Z 218 337 55% σ XY 126 266 110% σ Z 115 224 95% Table 2. Young s modulus and strength of classic Cesic compared to different HB-Cesic batches The test results demonstrate the superior mechanical properties of HB-Cesic compared to classic Cesic. 4.3.5 Weibull modulus Fig. 12. Size of HB-Cesic 4-point bending samples Number of samples: 55 XY samples 5 Z samples XY-direction (length axis of sample perpendicular to pressing direction). Z-direction (length axis of sample in parallel to pressing direction). Fig. 13. Experimental curve for Weibull modulus

We calculated the Weibull modulus for HB-Cesic by the least square fitting method and obtained the following value: m = 12.2 5. Recent applications out of HB-Cesic ECM has used HB-Cesic in the manufacture of a number of components: Beside some demonstration parts, ECM has manufactured a 320-mm mirror out of HB- Cesic. The following pictures show this mirror during optical polishing and optical measuring. Also, ECM manufactured structural parts, such as a focal plane structure with dimensions of 410 mm x 210 mm and designed for 24 CCD s, in order to demonstrate the high stiffness and thermo-mechanical performance of the HB-Cesic material compared to traditional focal plane materials. Due to the fact that this project is classified we cannot show any pictures. As part of this project we demonstrated the extraordinary machining possibilities with HB-Cesic. For instance, we machined HB- Cesic screws, nuts and threads. The threads were machined directly into the focal plane structure. See figures 16 and 17. Fig. 14. Mirror during polishing Fig. 16. HB-Cesic srew and nut Fig. 17. HB-Cesic thread inside structure Fig. 15. Mirror during optical measurements 7