网刊加载中。。。

使用Chrome浏览器效果最佳,继续浏览,你可能不会看到最佳的展示效果,

确定继续浏览么?

复制成功,请在其他浏览器进行阅读

Transfer Force Measurement of Electric Compressor with Low-Profile 3-Axis Force Sensor  PDF

  • ZHANG Junfang 1
  • KUSADA Takashi 1
  • HYAKUTAKE Tetsuya 1
  • SUMIYA Satoshi 2
  • MARUYAMA Kenichi 2
1. SOKEN Inc., 4700111 Aichi, Japan; 2. DENSO Corporation, 4488661 Aichi, Japan

CLC: U461TB535

Updated:2022-08-11

DOI:10.11908/j.issn.0253-374x.22753

  • Full Text
  • Figs & Tabs
  • References
  • Authors
  • About
CN CITE
OUTLINE

Abstract

An electric compressor generates a mechanical vibration that is transmitted from the engine to the vehicle body and then the vibration of the vehicle body creates a vehicle interior noise. The noise can be calculated by a transfer force from the electric compressor to the engine and transfer characteristics from the electric compressor to the vehicle cabin. The transfer force can be measured with a force sensor installed between the electric compressor and the engine. However, the force sensor interferes with other components and changes the vibration mode of the electric compressor. Therefore, the conventional force sensor cannot measure the transfer force of the actual phenomenon. In this paper, a new low-profile 3-axis force sensor was developed by use of piezoelectric quartz crystals, which achieved measuring the transfer force in as close to the actual phenomenon as possible.

In recent years, the market demands of the vehicle quietness are increased, therefore the reduction of the vibration and noise from an electric compressor is required

1-3. The electric compressor generates a mechanical vibration that is transmitted from the engine to the vehicle body and then the vibration of the vehicle body creates a vehicle interior noise4. In general, the noise can be calculated by measuring transfer force by use of a 3-axis force sensor screwed with bolts between the electric compressor and the engine5.

Then, the influence on vibration mode of the electric compressor is present in this paper by installing a 3-axis force sensor. Test pieces of different thickness are installed between an engine and the electric compressor, and a resonance frequency variation of the electric compressor is measured by shaking it up and down. The experimental system configuration is shown in Fig.1 and the measurement results are shown in Figs. 2 and 3. As shown in Fig.2, the resonance frequency variation of the electric compressor increases as the thickness of the force sensor rises, and the vibration mode differs from that of the actual equipment. The change in vibration mode is caused by the increased length between the engine and the electric compressor due to the installation of the force sensor, which increased the overhang of the electric compressor. Therefore, low-profile 3-axis force sensors are required to measure the force under actual situation.

Fig.1  Experimental system configuration with 3-axis load sensor

Fig.2  Resonance frequency between test pieces of different thickness

Fig.3  Resonance frequency variation

1 3-axis force sensor

1.1 Configuration of 3-axis force sensor

The low-profile 3-axis force sensor developed in this paper is shown in Fig.4. The inner diameter of the force sensor is ϕ 12.6 mm, the outer diameter is ϕ 20.0 mm, and the thickness is 1.95 mm. The principle is piezoelectric effect with quartz crystals

6. The crystal has an electrical axis, a machine axis, and an optical axis. An electrical charge is generated when a force is applied in the direction of the electrical axis. The piezoelectric quartz crystals to measure the force in the compression direction are cut out from the crystal to align the compression direction with the electrical axis while the piezoelectric quartz crystals to measure the force in the shearing direction are cut out from the crystal to align the shearing direction with the electrical axis. That is why the force sensor can measure the force in 3-axis direction.

Fig. 4  3-axis force sensor

The internal structure of the 3-axis force sensor is shown in Fig.5. The sensor laminates six pieces of piezoelectric quartz crystals which output the electric charge in the 3-axis direction and seven electrodes.

Fig. 5  Internal structure of 3-axis force sensor

1.2 Piezoelectric quartz crystal

The principle of the piezoelectric quartz crystal to measure the force in the shearing direction is shown in Fig.6 and the principle to measure the force in the compression direction is shown in Fig.7.

a  The electrical charge output is amplified twice

b  The electrical charge is canceled out

Fig.6  Principle to measure shearing load

a  The electrical charge is canceled out

b  The electrical charge output is amplified twice

Fig.7  Principle to measure compression load

The electrical axes of two crystals are aligned with the shearing direction, one crystal is placed in the opposite direction to another one, and machine axes of the crystals are aligned in the same direction as shown in Fig.6. The electrical charge output is amplified twice on the load in the shearing direction; on the other hand, the electrical charge is canceled out on the load in the compression direction.

The electrical axes of two crystals are aligned with the compression direction, one crystal is placed in the opposite direction to another one, and machine axes of the crystals are aligned in the same direction as shown in Fig.7. According to this configuration, the electrical charge output is amplified twice on the load in the compression direction; on the other hand, the electrical charge is canceled out on the load in the shearing direction.

1.3 Force division structure

The 16 kN load in the axis direction generates in the 3-axis force sensor at screwing bolt. In case that the piezoelectric quartz crystal incurs all load, it will be destroyed. The 3-axis force sensor developed divides the load into the crystal and the housing, whose safety factor ensures 2.3. The load distribution image is shown in Fig. 8.

Fig.8  Load distribution image

1.4 3-axis force sensor accuracy

The calibration method of the 3-axis force sensor in the shearing direction is shown in Fig.9, and the calibration method of the sensor in the compression direction is shown in Fig.10. The sensor is installed on a surface plate and then a block where the load is applied is screwed together as shown in Fig.9. The sensor in the shearing direction is calibrated by measuring electrical charge output when the load in the shearing direction, which applies to the block, is changed.

Fig. 9  Calibration for shearing direction

Fig.10  Calibration for compression direction

The calibration method for compression direction as shown in Fig.10 is to add another block on the block shown in Fig.9. The sensor in the compression direction is calibrated by measuring electrical charge output when the load in the compression direction, which applies to the block, is changed.

The calibration results are shown in Fig.11. The electrical charge output bears a proportionate relationship to the load in each direction.

Fig.11  Calibration Results of 3-axis Force Sensor

2 Load of electric compressor

2.1 Measurement system configuration

The electric compressor is mounted on three places of stay that simulates the engine, and the load generates on the fastening places is measured when the electric compressor is operating. The 3-axis force sensor is installed between the electric compressor and stay and screwed together. The system configuration is shown in Fig.12 and the picture of the sensor is shown in Fig.13.

Fig.12  System configuration of load measurement

Fig.13  Picture of 3-axis force sensor

2.2 Test result

The measurement load in the axis direction when the electric compressor is operating is shown in the Fig.14. The first-order load component of the electric compressor is measured not to be buried in the electromagnetic noise. Therefore, our developed low-profile 3-axis force sensor can be utilized to load measurement in a state close to the actual phenomenon.

Fig.14  Load Test Result of electric compressor

3 Conclusions

A low-profile 3-axis force sensor was developed. The machine axes of the two piezoelectric quartz crystals were installed in parallel and the electrical axes were installed in opposite. Thus, the electrical charge output was amplified twice on the load of the measuring axis and canceled on the other axes. The load was divided with the piezoelectric quartz crystals and housing, then the safety rate of the crystals was ensured. The first-order load component of the electric compressor was measured not to be buried in the electromagnetic noise. An experiment was conducted to confirm that the developed sensor could measure the load transferred from the electric compressor to the engine in a state close to the actual phenomenon.

References

1

MICHIHITO TSEKINE HITOH M. Comparison between wave theory and energy method in acoustic prediction of HVAC duct networks[J]. Proceedings of Building Simulation1999993):1389. [Baidu Scholar] 

2

MARTINI JCUCUZ S. Sound power determination of A/C-Compressors[C]// SAE 2002 World Congress. DetroitSAE20021. [Baidu Scholar] 

3

GRAS TAUBRY OMENON Aet al. Blocked forces characterization of an air-conditioning compressor-application to the norm ISO-21955 [C]// INTER-NOISE and NOISE-CON Congress and Conference Proceedings. [S. l.]Institute of Noise Control Engineering20192593): 6668. [Baidu Scholar] 

4

CHEN YifanFENG Huihua. An overview of NVH problems caused by changes in the excitation source of HEV[C]// IOP Conference Series: Materials Science and Engineering. LondonIOP Publishing202111941): 012009. [Baidu Scholar] 

5

DER AUWERARE H VMAS PDOM Set al. Transfer path analysis in the critical path of vehicle refinement: the role of fast, hybrid and operational path analysis[J]. SAE Technical Paper20071): 2352. [Baidu Scholar] 

6

OKAHATA YFURUSAWA H. Biosensor using crystal oscillator microbalance method[J]. Journal of the Institute of Electrical Engineers of Japan E (Sensor/ Micro Machine Division)200312311): 459. [Baidu Scholar]