Convective Heat Transfer in the Pre-Nozzle Volume of a Solid Rocket Motor with a Recessed Nozzle

Benderskii, B. Ya.; Chernova, A. A.

doi:10.1007/s10891-022-02576-x

Cited by 1 publication

(1 citation statement)

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“…The flow also tends to stabilize during this stage, known as the equilibrium stability stage (Figure 10, approximately 0.33 ≤ t ≤ 5.7 ms; Figure 11b, approximately t 2 ~5.7 ms). Research suggests that the response process of injection is related to the free volume [25]. Preceding the injection of the secondary flow, the combustion chamber pressure stands at 5.12 MPa.…”

Section: Openingmentioning

confidence: 99%

Transient Characteristics of Fluidic Pintle Nozzle in a Solid Rocket Motor

Yan,

Zhao,

Song

et al. 2024

Aerospace

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The fluidic pintle nozzle, a new method to control the thrust of a solid rocket motor, has been proposed in recent years by combining the pintle with the aerodynamic throat (fluidic throat). The study of static characteristics has proved that it has a remarkable effect on thrust control. To study the transient characteristics of the fluidic pintle nozzle, 2D transient simulations of a fluidic pintle nozzle propulsion system were conducted, employing dynamic meshing techniques. The Reynolds-averaged Navier–Stokes equations were meticulously solved, implementing a k–ω SST turbulence model. The thrust control principle of the fluid pintle nozzle was studied, and the wave structure was summarized. The transient characteristics of the secondary flow opening, secondary flow closing, pintle moving forward (pressure rise), and pintle moving backward (pressure drop) were obtained, and the effects of the injection angle and injection port position were studied. The response process after injection can be roughly divided into three stages: pressure propagation, pressure oscillation, and equilibrium stability, with time distributions of 0.4%, 5.39%, and 94.21%, respectively. In the process of the pintle moving forward, the rate of combustion chamber pressure increases and thrust decreases gradually because of the arc wall of the nozzle throat upstream, and the process of throats moving backward is just the opposite. Compared with the condition with a maximum throat opening and no secondary flow, the thrust of the condition with a minimum throat opening and a 0.3-flow-ratio secondary flow is increased by 80.95%. Under conditions of constrained flow ratio, the injection angle of the secondary flow ostensibly exerts negligible influence on the dynamic modulation of thrust. Nevertheless, it remains evident that a reduction in throat opening accentuates the impact of reverse injection. Furthermore, the proximity of the injection port to the head of the pintle is directly proportional to the efficacy of thrust control.

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Section: Openingmentioning

confidence: 99%