It is well known that vehicles traveling with high speed excite the air to high temperature, then air is ionized and the asreceived plasma gas forms on the boundary layer. The nosetip material will be ablated by the aero-heating air, such as fused, decomposition, sublimation or chemical reactions. [1] Furthermore, the dielectric properties of one material will change with the increasing temperature, which has an effect on the radar-wave transmission characters. [2] So a radar window for a supersonic vehicle should process critical property, such as a high resistance to stress failure induced by large thermal load and a high ablation resistance. In our previous work, [3] the 2.5 dimensional silica fibers reinforced the nitride-based composites (2.5D SiO 2f /Si 3 N 4 -BN) were prepared by preceramic polymer impregnation and pyrolysis (PIP) method through repeated infiltration of hybrid precursor polyborosilazane (PBSZ). Results showed that the composites had an excellent mechanical, dielectric and ablation properties. In this paper, the ablation property and ablation mechanism under an arc-jet stream were investigated.
Experimental Procedures
Composites PreparationAccording to literature, [3] PBSZ was used to infiltrate 3-dimensional silica fiber fabric (3D SiO 2f ), the 3D-SiO 2f reinforced nitride-based composites (3D-SRNC) were prepared by PIP method. The silica fibers, produced by JingZhou Feilihua Silica Glass Corporation (China), have a diameter of 6 ∼ 8 lm, a density of 2.2 g/cm 3 , a room temperature tensile strength of 1 700 MPa and an elastic modulus of 78 GPa. To form a 3D-braided silica fiber fabric, with the fiber volume fraction 50 %, those fabrics were woven by Beijing Fiberglass Research & Design Institute (China). The infiltration-curepyrolysis cycles were repeated for five times and then the density of the 3D-SRNC reaches 1.71 ∼ 1.74 g/cm 3 .
CharacterizationSpecimens with the dimension size 30 × 40 mm were characterized using an arc-jet stream ablation tester. Ablation temperature was above 4500°C and ablation time was 10 s. The average mass loss rate (defined as the weight loss per unit time) and linear ablation rate (defined as the thickness loss per unit time) of the specimens were measured after the ablation test. Scanning electron microscopy (SEM, JSM-5600LV) was used to observe the ablation surfaces morphology. Energy-dispersive X-ray spectroscopy (EDS) was carried