A nozzle in which the thermal energy of gases is converted into the kinetic energy of a gas jet is a basic element of the rocket engine. If the pressure in the external medium (or in the engine combustion chamber) varies, the conventional nozzle will not be optimal throughout the entire pressure range: it operates either in the underexpansion or overexpansion mode. The nozzle would be ideal if its expansion degree followed the changes in the external (internal) pressure, preserving an equality between environmental pressure and internal pressure at the nozzle cross section; but it is very difficult to realize this mode. There are various approaches to thrust-loss control in the case of overexpansion. For example, Semenov [1] proposed the use of air blow through an annular slot into the supercritical nozzle section operating in the overexpansion mode. However, this is only a singlestep variation in the degree of the nozzle off-design. The heat-resistant gas-permeable porous materials that are now available equalize, based on their gas permeability, the pressure inside the funnel with that in the environment at the nozzle section operating in the overexpansion mode, i.e., render the nozzle self-adjustable without any additional devices. Therefore, investigation of the effect of a porous insert on the nozzle thrust represents an urgent problem. To experimentally study this effect, we used a differential pendulum setup including reference and working nozzles. The installation was freely suspended on a bearing unit (Fig. 1) and was connected to the fixed base only by an elastic element of the strain-gauge balance; there were no other rigid bonds. The key measuring principle used in this installation is the comparison of the jet thrusts of two nozzles (working and reference), oriented in mutually opposite directions. To determine the effect of the porous insert on changes in the thrust of the nozzle, we performed two experiments with the same prechamber pressure p 0 . In the first experiment, the working nozzle with continuous walls was used, and, in the second, the porous insert was mounted in the supersonic section of the working nozzle (schematically shown by dashed lines in Fig. 2). As a result, the change in the thrust of the nozzle was determined from two experiments carried out with the identical prechamber pressure p 0 . The experimental procedure was described in more detail in [2]. The supersonic section of the nozzle was formed by a cone with a halfopening angle of α = 8i . The porous insert is the duralumin section x 1 < x < x 2 of the conic nozzle in which 1050 round holes approximately 1 mm in diameter with a total relative area of 18% were drilled. The radius of the minimum nozzle section is r * = 19.2 mm; the length of the supersonic section is x sr = 147 mm; and the coordinates of the porous section are x 1 = 82 mm and x 2 = 130 mm (Fig. 2).
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