Lili Nadaraia, Nikoloz Jalabadze, Levan Khundadze, Levan Lortkipanidze and Givi Sharashenidze Georgian Technical University, Republic Center for Structure Researches (RCSR) nadaraia@gtu.ge Ultra-High Temperature Ceramics Borides Carbides Compositions TiC TiB2-TiC, B4C-SiC, Ti3SiC2 TiB2 ZrB2 HfB2 B4C SiC Application Armor low density high hardness Nozzles Abrasives Abrasion resistance Nuclear applications as neutron radiation absorbent UHTC wear resistance Refractory applications high melting poin thermal stability Manufacturing methods of UHTC Methods producing the Powder Methods producing the Dense bodies • reaction of elemental boron and carbon powder between reagents • carbothermal synthesis, • carbothermal vapor–liquid– solid growth mechanism • self-propagating hightemperature synthesis (SHS) = Combustion Synthesis (CS), • arc melt process, • etc… • hot press, • hot isostatic pressing (HIP), • Cold compaction and high temp. sintering • pressureless sintering, • self-propagating hightemperature synthesis (SHS) under the pressure, • Spark Plasma Sintering, • etc….. Advantages and disadvantages of spark plasma sintering Advantages of spark plasma sintering: Fast sintering process; Uniform sintering; Low grain growth (nano-grain materials may be prepared); Compaction and sintering stages are combined in one operation; Binders are not necessary; Better purification and activation of the powder particles surfaces; Different materials (Metals, Ceramics, composites) may be processed; High energy efficiency; Easy operation. Disadvantages of spark plasma sintering: Only simple symmetrical shapes may be prepared; Expensive pulsed DC generator is required. Expensive SPS device Fig.1. Scheme of the SPS the process of sintering – PDC - pulsed DC, GD - graphite die, S – powder sample, P – pressure loading, EC- electric current, s – spark, sp – spark plasma and p- powder particles. SPS mechanism by SPS SYNTEX INC Company; (a) I- Flow direction of electrons during DC current, (b) I- Flow directions of electrons during AC current. DC current shapes Pulse DC current Shape in the developed device: a- at the frequency of 400 Hz, b- during different frequencies (T), different duration pulses (t) and different duration pauses (T-t); Current Shapes to be used after retrofitting the SPS device: during different frequencies (T), different duration pulses (t) and different duration pauses (T-t); SPS Device Press molds for synthesize nanopowder (a) and sintering dense bodies (b) of composite materials 1-upper plug, 2-lower plug, 3-Matrix. Self-propagating high-temperature synthesis (SHS), (combustion synthesis CS) Poly SHS A. G. Merzhanov. 2006, Advances in Science and Technology, 45, 36- 44. Sintering process a: Self-Propagating HighTemperature Synthesis (SHS), b: SPS accompanied with poly SHS. Borides B4C B4C 2TiO2 2HfO2 3C 3C B4C 2ZrO2 2HfB2+4CO 2TiB2+4CO 3C HfB2 TiB2 2ZrB2+4CO ZrB2 Titanium Diboride X-Ray and SEM images of Titanium Diborides a- TiB2 powder synthesis at 10000C 1h, b- sintered via SPS at 16000C ; C- SEM image of sintered via SPS at 16000C TiB2 Zirconium Diborides ZrB2 X-Ray and SEM images of Zirconium Diborides a- ZrB2 powder synthesis at 10000C 1h, b- sintered via SPS at 16000C ; C- sintered via SPS at 17000C SEM images of Zirconium Diborides sintered via SPS at 17000C Hafnium Diborides HfB2 X-Ray and SEM images of Hafnium Diborides sintered via SPS at 18000C ; Carbides Si C 4B Ti C C SiC B4C TiC Carbides TiC SiC X-Ray images of Titanium Carbide sintered via SPS at 14000C -3 min; X-Ray images of Silicium Carbide sintered via SPS at 18000C -1 min; Boron Carbide B4C a- XRD pattern of B 4C powder (SPS 14000C-3 min) b- SEM image of B4C bulk material (SPS 17000C-10min) A-XRD patterns of B 4C powder materials obtained by standard (a), SPS methods (b) ; B- SEM image of nanopowder B 4C obtained by SPS method (1400 0C-3min). Composition Si 4B 2C B4C - SiC SPS sintered B4C – SiC (17000C-5min): a-X-ray diffraction pattern; c- SEM image B4C – SiC Sintered via SPS b- SEM image of B4C – SiC powder produce via SPS. Composition Si 3Ti 2C Ti3SiC2 X –Ray of Ti3SiC2 composition of sintered via SPS at 14500C Composition B4C 2TiO2 3C TiB2 - TiC Vickers hardness 29.5 Gpa TiB2 TiC X –Ray and SEM images of TiB2 - TiC composition of sintered via SPS at 14500C SPS OPERATING MODES WITH RELATIVELY DENSITY SPS TiB2 SPSSPSTiB2B4C-SiC TiC 9.2/2060 10/2700 9/2700 9.5/2300 10/2700 9/2700 1700 1800 1600 1700 1700 1450 5 10 5 5 5 5 6 0 20 20 25 20 30 30 - 94 85 92 95 98 97 SPSSample# SPSB4C Regime BC powder 4 SPSCurrent (V/A) Temp. 9/1370 (0C) 1600 Holding Time (min) Pressure MPa Density (% of theoretical) SPS HfB2 SPS Ti3SiC2 Shapes of materials sintered via SPS Ballistic Testing Test is conducting according Standards of National Institute of Justice (NIJ) (type-IV) Additional energy is absorbed by each successive layer of material in the ballistic panel. http://www.bodyarmornews.com/ ¤ Size of the plate -120x120mm; ¤ Size of the plate fragments Bullet direction ¤ Hard Blend (B4C, SiC, B4C-TiB2, B4C-SiC ) ¤ Backing material Plastic (Ti-6Al-4V)/textile ¤ 60x60mm; Weight - 50-100g. The plate presented a package armored with ballistic textile (Kevlar, tvarin, denima); Weight of the package was 0,6 – 0,8 kg; Fire tests were provided by shooting from the Mosin’s Rifle; • Bullets - armor-piercing • Bullet Mass – 10.8±0,1; • Bullet speed - 869±10 m/sec. Standard shooting method, distance - 10m towards a plasticine target. Ballistic testing 120mm BFS NIJ requirements - Max Back face signature (BFS) depth is 44mm 40mm Conclusion There was developed new technology for manufacturing of nanocrystalline composite materials. Poly SHS process were detect during SPS and were use for UHTC materials fabrication Diborides of transaction metals Ti, Zr, Hf, were produced Nanocrystalline Powders of carbides of metals Ti, Si, and B were obtain after Poly SHS process Effective composition materials TiB2 - TiC, Ti3SiC2, B4C - SiC were developed. Ballistic testing gives promising results and further effort will be directed to improve the characteristics. Modernization of SPS device is undergoing process (replacing of pulse DC current unit with pulse AC current unit). Further work will be directed to detect impacte of DC current at the sintering process and at the materials properties. ACKNOWLEDGEMENT The part of research described in this presentation was made possible in scope of projects funded by Shota Rustaveli National Science Foundation. Project # 12/34 Presidential Grants for Young Scientists. nadaraia@gtu.ge