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Additional info for Airplane design, vol.8 and errata (1990)
After the specimen has been positioned in the middle of the heater, shield 5 is released and allowed to drop by gravity, and the side face of the specimen is exposed to the heater. The instant at which the specimen fails is recorded by a piezoelectric sensor connected to the specimen through a sound 26 3 Methods of Modeling Tests duct 6; the signal from the sensor is transmitted through an amplifier to a recording oscillograph which is switched on automatically after shield release. 475 Th ; this makes determination of the thermal stress resistance a much simpler procedure.
D T = 2,900◦ C; 30 μ ×300 along the boundaries between them. They move into the voids and to the free surface of the sample (Fig. 8a–d) according to the mechanism proposed in [19, 21]. After overcoming the resistance of retainers on the definite part of the surface of the particles and their ‘activation’ the boundary diffusion viscosity becomes low and shrinkage sharply increases. Random boundaries that are not connected with initial boundaries between particles are formed. Shrinkage rate decreases with porosity decrease.
The influence of sintering parameters on the sintered ZrC structure and properties are showed on Figs. 9 accordingly. Sintering of ZrC samples by rapid nonisothermal heating takes place in a complicated manner. In the first stage of the sample heating to 1,300 K, for the first 2 s thermal elastic stresses of the order 30– 40 MPa (Fig. 7) are developed and are capable of creating local plastic deformation of the material on rough surfaces of the particles. 9 performed at a temperature of 290 K and subsequent heating to temperatures 600 and 850 K.