Thrust Measurement of an Integrated Multi-Sensor Micro-Newton Cold Gas Thruster


4.1. Thrust Range

In the course of a comprehensive thruster performance test, the thrust range is of primary interest. A closed-loop flow control method was adopted to give a specific flow value to the thruster. At the same time, a high-precision thrust test bench monitored and recorded, in real time, the pressure, thrust and displacement data generated by the thruster at the given flow rate. The displacement data were converted into needle valve opening values, and then a large amount of corresponding one-to-one experimental data was collected. After data analysis and processing, the corresponding relationship curves among flow, thrust, and the needle valve opening were constructed.

Figure 7 shows the thruster’s large flow dynamic range test and its corresponding thrust. In this test, the given flow was 2000 μg/s, and then the two higher flow points of 2100 μg/s and 2200 μg/s were tested, reaching the highest critical flow range of the thruster in the large flow mode. It can be observed in the figure that in the large flow mode, both the flow and thrust performance of the thruster were relatively stable. As the given flow increased, the thrust also increased steadily, and the thrust generated by the thruster stably exceeded 1000 μN when the flow reached 2000 μg/s and above. The needle valve opening gradually increased, which is due to the fact that the tank pressure gradually decreases with a large flow, and the needle valve opening has to be increased to keep the flow rate unchanged under the condition of closed-loop control.

The results are corroborated by the gradual decrease in pressure. This result demonstrates that the needle valve can move quickly under high flow conditions with closed-loop flow control, and that the thrusters have good performance stability, meeting the demand for higher thrust output under high flow conditions.

Figure 8 shows a step diagram of the flow rate, thrust, and opening in detail, showing the continuous change in the flow rate from 150 μg/s to 550 μg/s in steps of 50 μg/s, and then decreasing to 150 μg/s in the same step value. It can be seen in the figure that as the flow rate gradually increases, the corresponding thrust also shows a smooth change trend. This thrust output reflects the excellent continuous adjustment capability of the thruster in a wide flow range and also implies that in actual application, the thrust size can be flexibly adjusted according to different mission requirements to achieve precise space operations.
Figure 9 shows the results of a wide range thrust test on the actuator with a thrust range of up to 1300 μN. During the test, the thrust and flow rate were measured accurately, and the obtained thrust data were fitted linearly to obtain the relationship between the thrust and flow rate.

Using this relationship, we calculated the flow value corresponding to any thrust value within the range of 1300 μN and vice versa. This allowed us to obtain a more in-depth understanding of the thruster’s performance and to grasp its flow change law and overall operating characteristics under different thrust conditions.

Figure 10 illustrates the data correspondence between the displacement and thrust. To further explore the intrinsic relationship between displacement and thrust, we used the method of third-order polynomial fitting to obtain a fitting curve that reveals the correspondence between the displacement and thrust to some extent.

The fit has a certain deviation in the mean displacement. There are two main reasons for this problem. One is that the needle valve material itself has a hysteresis characteristic. Due to this characteristic, the relationship between the displacement and thrust of the needle valve in the process of movement is not completely linear, but has certain hysteresis and non-linear factors, which poses considerable challenges to the fitting work. Secondly, the change in tank pressure also affects the fitting accuracy. In the experimental process, the pressure is not always constant, and its fluctuation causes corresponding changes in the thrust, which in turn disrupt the normal correspondence between the displacement and thrust, making it difficult to fit the curve to the actual data.

4.2. Thrust Resolution

As a high-precision propulsion device, the design objective of the micro-Newton cold gas thruster is to achieve a wide range of thrust adjustments while ensuring high resolution and accuracy under the micro-Newton low-thrust output state. This is critical to meet the noise reduction requirements of spacecraft for complex space missions. During the experiment, a finely controlled small flow was input to the thruster, and the force frame results show that the output resolution in the small flow mode reached 0.1 μN.

Figure 11 shows in detail the thrust characteristics of the micro-Newton cold gas thruster, as the flow rate varied in steps of 0.2 μg/s and 0.3 μg/s. The initial flow rate of this test was set at 2 μg/s, and then the flow rate was stepped up and down in increments of 0.2 μg/s and 0.3 μg/s, enabling a comprehensive examination of the thrust response of the thruster at a high flow rate resolution.

It can clearly be seen in the figure that the flow sensor and displacement sensor of the thruster achieved the set accuracy, and the thrust test bench also detected the thrust change with this accuracy. When the flow rate changed by 0.2 μg/s, the resolution reached 0.1 μN. This result demonstrates that the thruster performed well in flow control accuracy and thrust output sensitivity and could sense and respond to small flow changes, thereby achieving precise adjustment of the corresponding thrust. The measurement accuracy of the force frame itself was also excellent, and it detected small thrust changes of 0.1 μN.

4.3. Thrust Noise

Figure 12 shows the thrust noise power spectrum density measured under different constant thrust conditions, covering various working conditions, such as thrust of 3 μN, 5 μN, 10 μN, as well the thruster being on but not given flow. It can be seen in the figure that under these different working conditions, the level of thrust noise was roughly equivalent to the standard noise level of the experimental environment, and both were of the same order of magnitude, showing that under normal thrust conditions, the thrust noise did not increase abnormally.

The frequency band of main concern is from 10−3 Hz to 1Hz. The band above 0.1 Hz had only one frequency point, 0.3 Hz, where the shear noise exceeded the set requirement threshold of 0.1 μN/Hz1/2. This frequency point corresponds to an oscillation period of approximately 3.3 s. In this case, the possible cause was the fluctuation in the flow rate. Rapid changes in the flow rate produce high-frequency disturbances, which are directly transferred to the thrust output and manifest themselves as high-frequency thrust noise. During the long-term operation of the thruster, due to the influence of various internal factors and the external environment, its performance may drift slowly. This drift will be reflected in the low-frequency fluctuation of the thrust, thereby affecting the stability of the thrust.

To further reduce thrust noise and improve thrust stability, the two key factors of voltage fluctuation and flow fluctuation can be optimized. For example, by adopting a more stable power supply system, the voltage can be precisely regulated to reduce the voltage fluctuation. At the same time, the flow control system can be optimized, and high-precision flow sensors and advanced control algorithms can be used to achieve precise control of the flow, thus reducing the flow fluctuation. To address the problem of drift in thruster performance, the monitoring and maintenance of the thruster can be strengthened, the performance of the thruster can be regularly calibrated and adjusted regularly, and problems that may cause performance drift can be detected and resolved on time to ensure that the thruster is always in a good operating state. By implementing these measures, it is expected that the thrust noise can be controlled at a lower level and meet more stringent performance requirements.



Source link

Songcai Lu www.mdpi.com