Ablation mechanism of TaC coating fabricated by chemical vapor deposition on carbon-carbon composites
LI Guo-dong(李国栋)1, 2 , XIONG Xiang(熊 翔)1 , HUANG Ke-long(黄可龙)2
1. State Key Laboratory of Powder Metallurgy, Central South University, Changsha 410083, China;
2. School of Chemistry and Chemical Engineering, Central South University, Changsha 410083, China
Received 10 August 2009; accepted 15 September 2009
Abstract: Ablation characteristics and mechanism at high temperature for TaC coatings on carbon-carbon composites were investigated by ablation experiments with low power laser and oxyacetylene flame. The results show that the TaC coating is decomposed at the initial stage of laser ablation in atmosphere, and free carbon diffused to the surface, then oxidized to the melt including carbon, oxygen and tantalum. With the increase of ablation time, the melt is oxidized to low valent tantalum-oxide and Ta2O5 is formed finally. During the melt cooling, needle-like crystals of Ta2O5 are precipitated. Between the melt and TaC coating, there exists a diffusion transition layer with thickness of 1-2 mm. The transition layer consists of fine crystals and pores including carbon, oxygen and tantalum. The oxyacetylene flame ablation at 2 300 ℃ results in the rapid oxidation of TaC and formation of protective liquid films of tantalum oxide on the coating surface, where the liquid film can fill up the cracks and cover the coating. In such case, the oxidation mechanism of TaC is converted to the oxygen solution and diffusion control mechanism.
Key words: TaC coating; oxidation; ablation mechanism; carbon-carbon composites
1 Introduction
Carbon-carbon(C/C) composites are easy to be oxidized and ablated at high temperature and high-speed gas jet with rapid ablation rate exponential to the pressure of combustion chambers, which limits their potential application in new type and high performance aerospace vehicles[1-3]. To prepare coatings on C/C composites with good resistance to high temperature, oxidation, washout and ablation is an important method to promote the performance and application of C/C composites[4-7]. Coatings, such as SiC, Si3N4, MoSi2, borate glass, etc, exhibit good antioxidation, but their oxidation resistant temperatures are below 1 800 ℃ in general. The inoxidizability mechanism for coatings below 1 700 ℃ has been investigated by many researchers. LEE and HYEOK[8] found that the ablation property of the obtained SiC coating prepared by SiO2 deoxidizing carburization is enhanced with increasing the reaction time and synthesized temperature. In addition, the ablation performance of SiC coating is dependent on coating grain size and the crystal structure and orientation. The SiC coating ablation performance is similar to its inoxidizability below 1 650 ℃, while behaves abnormal at 1 800 ℃[8]. HUANG[9] and CUI[10] studied the ablation properties of C/C composites containing TaC coating, and found that it shows better ablation resistance than C/C composites.
TaC is one of the materials with higher melting point (3 880-4 000 ℃[11]), together with high hardness, good resistance to washout and erosion, and good chemical compatibility with C/C composites. Therefore, the TaC coating is an excellent choice for the C/C nozzle throat of solid rocket motor (SRM)[12-14]. However, there are few reports on the preparation of TaC ablation-resistance coatings and its ablation mechanism in detail. Accordingly, it is of great significance to study the oxidation ablation process and mechanism for TaC coatings at high temperature.
In this work, the TaC coatings were fabricated by chemical vapor deposition (CVD) method and their ablation properties were investigated by low power laser and oxyacetylene flame at 2 300 ℃. In addition, the oxidation process and ablation mechanism for TaC coating in the oxidation atmosphere over 2 000 ℃ were discussed.
2 Experimental
2.1 Sample preparation
The quasi-3D C/C composite with density of 1.82 g/cm3 was chosen as the matrix material. The sample size (diameter×length) was 30 mm×10 mm, and the ablation plane was parallel to the fiber felts. The TaC coating was prepared in the isothermal chemical vapor deposition furnace by the deposition technique reported in Refs.[14-15]. The coating structure and morphology were characterized by X-ray diffractometer (D/max 2550 VB) using Cu-Kα radiation and scanning electron microscope (JSM-6360LV) with energy dispersive X-ray spectrometer (EDS).
2.2 Ablation equipment and process
The laser ablation equipment is YAG(Nd) pulse laser (wave length 1.06 μm) with following parameters: frequency 20 Hz, pulse width 1 ms, laser spot diameter 2 mm, monopulse energy 40 J and working voltage 400 V, 440 V. The laser heating ablation was carried out on TaC coatings for 2, 30, and 120 s in atmosphere.
The oxyacetylene flame was adapted from the oxyacetylene torch. The large size torch blowpipe was adopted with the volume ratio of O2 to C2H2 4?1. Before testing, the flame temperature was measured by graphite blocks. After checking the temperature without fluctuation, the flow and height of oxyacetylene flame and the measuring position could be fixed. Then the thermometric graphite block was removed and test samples were placed on the measuring position. The ablation time and temperature were recorded, and after the given time, the test sample was removed rapidly and cooled in air.
3 Results and dicussion
3.1 Structure and morphology of TaC coating
Fig.1 shows the typical XRD pattern of the TaC coatings. It is seen that only the diffraction peaks of TaC peaks can be observed in a sharp profile, which indicates that the TaC coating obtained is pure. The SEM images of TaC coating are shown in Fig.2. Combining the energy spectrum analysis of the coating fracture surface (Fig.2(b)), it can be found that the Ta content is almost homogenous without impurity inside or outside the coating. The thickness of prepared coating is about 314 μm, exhibiting no surface and interlaminar cracks, with loose surface and dense interior layer, and firm combination with the C/C substrate. From the substrate to surface, the coating can be sequentially divided into the fine-grained dense area (<150 μm), coarse-grained dense area (150-250 μm) and surface loose area (250-341 μm). The TaC structure is uniform in all areas and the three areas have no obvious transition interface.
Fig.1 XRD pattern of TaC coating
Fig.2 SEM images of TaC coating: (a) Surface morphology; (b) Cross-section morphology
3.2 Ablation characteristics of TaC coating by low power laser
Fig.3 shows the surface morphologies of the TaC coating ablated for different time under the working voltage of 400 and 440 V. It can be seen that only local break-up and darkened color can be observed after laser ablation for 2 s (Fig.3(a)); obvious melt appears in small amount with irregular and bubble shape after laser ablation for 30 s (Fig.3(b) and (e)); the melt increases to form liquid plane without bubbles after laser ablation for 120 s (Fig.3(c), (f)).
Fig.3 Surface morphologies of TaC coating ablated by low power laser for different time: (a) Ablated for 2 s, 400 V; (b) Ablated for 30 s, 400 V; (c) Ablated for 120 s, 400 V; (d) Ablated for 2 s, 440 V; (e) Edge part of Fig.3(b); (f) Square area of Fig.3(c)
In conventional oxidation for TaC at low temperature (<1 500 ℃) in air, it is well known that TaC begins to be oxidized into Ta2O3 over 500 ℃, then form Ta2O5 particles over 700 ℃[16]. As far as laser ablation in a short time (2 s) is concerned, the appearance of fracture and break-up on the particle is due to the large expansion coefficient of TaC crystals and local high temperature caused by laser, which leads to the rapid fracture of TaC crystals. The warp deformation of particle shell results from the TaC oxidized to tantalum oxide of low melting point.
Fig.3(e) shows is a magnified description of the melt edge of Fig.3(b), where the temperature is a little lower and only a small quantity of melt occurs. There mainly exists white needle-like tantalum oxide aggregation with excellent wetting property to the melt.
Fig.3(f) shows the magnified middle melt region of Fig.3(c). It can be seen that many needle-like crystals precipitated from the melt, which characterizes Ta2O5 crystals from the melt during cooling. Such precipitates can effectively retard the crack extension for the solidified melt in cooling process.
Fig.4 shows the SEM images of the coating fracture surface after laser ablation for 120 s. Obviously, there is a transition region of 1-2 μm (region 2) between the cooled melt (region 1) and TaC coating (region 3). No apparent interface can be seen among the above three regions, and the transition region is composed of pores and fine crystals that were indicated as Ta, O and C by EDS. The occurrence of transition region is beneficial to the wetting and spreading of the surface tantalum oxide melt, and leads to the good bonding property of melt with the TaC coating.
Fig.4 Fracture SEM images of TaC coating after ablation for 120 s: (a) Fracture surface on the ablative marginal zone; (b) Fracture surface on the ablative center
3.3 Ablation process analyses for TaC coating by low power laser
With the increase of laser heating time, the temperature of coating surface rises rapidly up to 2 000 ℃. The coating oxidation is accelerated and the tantalum oxide melt occurs soon. After heating for 30 s, large-area melts can be observed (Figs.3(b) and (e)), and further heating results in more and thicker melts (Figs.3(c) and (f)), suggesting the increment of oxide. It is confirmed by EDS that the white melt transforms from the low valent tantalum oxide to Ta2O5 gradually with the prolonged heating.
It is noteworthy that the laser heating ablation can not be simply regarded as the heating oxidation process in atmosphere. It can be seen from Fig.3(d) that there is no melt in the region B, indicating the morphology of the coating broken up by laser heating. Region A suggests the melt resulting from the break up of region B and formed by the oxidizing and melting under laser heating. The chemical composition in Fig.3(d) was analyzed by EDS and listed in Table 1. It can be seen that the melt in region A contains oxygen while in other positions (such as region B), the main component is free carbon, together with rare oxygen and small amount of tantalum. This implies that at the initial stage of laser heating, the TaC coating is not mainly oxidized into CO or CO2, instead, it is obviously decomposed. Due to the large relative atomic mass of tantalum, the diffusion of Ta is slow. For the carbon has a small atomic mass, it can diffuse to the surface quickly. With the increase of laser power, the content of free carbon increases and even in the melt region A, considerable amount of free carbon can be obtained. Therefore, the oxidation process at the initial stage of laser ablation is different from that of slow heating. This phenomenon may be explained as follows: on the one hand, when the TaC coating is under the rapid heating of laser, the oxygen content is severely insufficient; on the other hand, the coating is composed of nanoparticles with high interface energy, porosity and specific area, which is easy to be endothermic. Then the local temperature will be excessively high, resulting in the occurrence of decomposition reaction. This is very meaningful to the mechanism analysis of oxidation ablation for the TaC coating applied in the solid rocket with high enthalpy and thermal shock.
The surface melt is thin with many bubbles (Fig.4(a)), resulting from the fact that the TaC coating is not completely covered by the melt and it is rapidly oxidized together with releasing of certain amounts of reaction gas. And the oxidation process is controlled by the reaction mechanism of oxygen and TaC coating. In Fig.4(b), it can be seen that the surface melt is thick without bubbles due to the complete covering of the TaC coating by Ta2O5 melt. Thus the coating is not exposed directly to oxygen; resulting in a slow oxidation rate. Besides, the low melt viscosity favors bubbles to be eliminated. Under this circumstance, the oxidation process is controlled by oxygen solution and diffusion mechanism. The oxidation experiment at high temperature has also proved that at 1 000-1 500 ℃ the oxidation of TaC coating increases rapidly with the increase of temperature, and the coating inoxidizability is rather poor; while over 2 000 ℃ the oxidation rate of TaC coating decreases obviously and its inoxidizability is largely enhanced. Thus, the melt for resisting oxygen diffusion does not appears on the surface, which is key to determine the oxidation control mechanism and oxidation rate of the TaC coating. The TaC coating covered by tantalum oxide melt will be oxidized or ablated depending on the solution concentration and diffusion velocity of the oxidized gas in the melt. Due to the much smaller amount of oxygen solved in the Ta2O5 melt and slower speed of the corresponding oxygen diffusion, as compared with those supplied by rocket combusting gas, the rapid oxidation of the TaC coating can be retarded and the ablation rate can be decreased. From Fig.4, the morphology and thickness of the transition layer are almost constant. To some extent, the oxidation macrokinetics for the TaC coating can be characterized by the moving rate of the transition layer.
Table 1 Chemical composition of TaC coating by EDS
Considering that the Ta2O5 melt has a large expansion coefficient and its temperature is higher than that of the substrate or the underlying coating, the occurrence of cracks during cooling is inevitable under the large cooling rate and temperature gradient. However, as shown in Fig.3(f), needle-like Ta2O5 crystals will be precipitated from the melt during slow cooling, which can effectively retard the crack propagation of solidified melt. It is also seen that lots of needle-like crystals appear on the ablative sample surface after ablation in the oxyacetylene flame at 2 300 ℃. The XRD results show that such needle-like crystals are tetragonal Ta2O5 crystals (Fig.5). Then the Ta2O5 melt during cooling will be strengthened similar to the mechanism of the Ta2O5 crystal whisker reinforced the Ta2O5 glass. When the Ta2O5 melt ruptures, the cracks deflect and increase (Fig.3(f)), thus effectively preventing the cooled melt from severe break-up during cooling process.
3.4 Ablation characteristic and process analysis of TaC coating by oxyacetylene flame
Fig.6 shows the SEM images of the TaC coating after oxyacetylene flame ablation at 2 300 ℃ for 60 s. Despite of the unevenness, the coating surface exhibits a thin melt with little pores and cracks on the melt surface (Fig.6(a)). XRD results show that the melt is tetragonal Ta2O5 crystals with some orthorhombic Ta2O5 crystals, which suggests that the melt has precipitated crystals during cooling. From the natural fracture in Fig.6(b), it can be seen that the coating after ablation can be divided into four parts: the surface is the melt layer starting precipitation of crystals(about 10 ?m thickness); next is the porous oxide precipitation layer (about 35-45 ?m thickness); the transition layer (about 5-15 ?m thickness) and the TaC coating without oxidation, which is closely connected with the transition layer.
Fig.5 XRD pattern of TaC coating oxidized by oxyacetylene flame at 2 300 ℃ for 60 s
Fig.6 SEM images of TaC coating after oxyacetylene flame ablation at 2 300 ℃ for 60 s: (a) Coating surface; (b) Cross-sectional morphology of fracture sample; (c) Local magnified surface morphology; (d) Magnified images from square area of Fig.6(b)
The as-fabricated TaC coating exhibits good thermal shock resistance as it has no break-up and large cracks during the whole ablation and cooling process. The cracks shown in Fig.6(b) suggest that there exists stress concentration in regions between the oxide precipitation and transition layer, so does in regions between the transition layer and TaC coating. The laminar cracks are caused by the stress release during the ruptures of the coating.
From the local magnified morphology (Fig.6(d)), the needle-like or columnar crystals can be clearly seen, and their arrays exhibit apparent orientation. The composition in this region is Ta and O with the atomic ratio of 2?(4.5-5) as determined by EDS. By combining with the XRD analysis, the needle-like crystals should be the tetragonal Ta2O5 crystal, which relates to the morphology of the columnar crystals of the TaC coating. The oxyacetylene flame ablation of the TaC coating is mainly an oxidation process at 2 300 ℃. In the beginning stage, the coating temperature is lower than the melting temperature of Ta2O5, and the surface coating is loose. When heated by the oxyacetylene flame that is rich in oxygen and flows quickly, the coating will soon be oxidized to form the fine tetragonal Ta2O5 crystals. Although the oxidation process of TaC is a process of the structure rearrangement, which involves the diffusion reaction of C to the outside and O to the coating interior, the movement of Ta atoms is rather small due to its heavy atomic mass, and the morphology of the TaC columnar crystal is largely inherited. That is why the fine crystal of tetragonal Ta2O5 grows in a preferred orientation and exhibits the needle-like morphology corresponding to the columnar character of the TaC coating. Some columns are parallel to the coating surface, resulting from the fact that the fine tetragonal Ta2O5 crystals are partially melt under the burning oxyacetylene flame flow, and the vertical needle-like crystals are toppled by the shear force of the gas flow or surface melt flow.
It can be seen from Fig.6(c) that after the surface generates the Ta2O5 liquid film and under the action of surface tension, the liquid film can fill in and cap the cracks that exist originally in the surface. Due to the impediment of the Ta2O5 liquid film, oxidants in the combusting gas will not be in direct touch with TaC, and the further oxidation of TaC will be achieved only by the solution and diffusion of oxygen through the Ta2O5 liquid film melt. It follows that the TaC oxidation mechanism is transformed to the oxygen solution and diffusion control type, which agrees well with the results from laser ablation and this is the major reason for the TaC coating with good oxidation and ablation resistance.
4 Conclusions
1) The ablation process of the TaC coating by low power laser in air is as follows: the initial thermal shock leads to the local break-up, the decomposition of the TaC coating and the diffusion of free carbon to surface. Then, lots of free carbon are diffused to the surface and oxidized as tantalum oxide melt containing carbon, and the melt is further oxidized to the Ta2O5 melt gradually. The melt occurrence changes the oxidation mechanism of the TaC coating from the interface reaction control mechanism to the diffusion mechanism in the way that oxygen is solved and diffused speed in the melt. Between the melt and TaC, there exists the diffusion transition layer with thickness of 1-2 mm that consists of fine crystals and pores. The transition layer is mainly composed of carbon, oxygen and tantalum. The occurrence of the transition layer favors the enhancement of the wetting property of the melt and coating and ablation resistance of coating.
2) The oxyacetylene flame ablation of the TaC coating at 2 300 ℃ for 60 s is mainly an oxidation process during which TaC is rapidly oxidized to needle-like Ta2O5. Then Ta2O5 is melted and the protective liquid film of tantalum oxide is formed on the coating surface, which can fill in and cap the cracks. The further oxidation mechanism of the TaC coating is transformed to the oxygen solution and diffusion control type.
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(Edited by ZHAO Jun)
Foundation item: Project(2007AA03Z110) supported by the National Hi-tech Research and Development Program of China; Project(50721003) supported by the National Natural Science Foundation of China; Project(20070420822) supported by China Postdoctoral Science Foundation; Project(2007RS4027) supported by the Postdoctoral Science Foundation of Hunan Province, China; Project(2007) supported by the Postdoctoral Science Foundation of Central South University, China
Corresponding author: LI Guo-dong; Tel: +86-731-88830899; E-mail: lgd63@163.com