Study on magnetostriction characteristics under different measurement conditions under an externally compressive stress

1. Introduction

The magnetostriction characteristics of grain-oriented electrical steel are the main reason to make the vibration and acoustic of electrical equipment such as transformer and reactor. In order to better study the characteristics of grain-oriented electrical steel in reactor, the main research in this paper is the magnetostriction characteristics of grain-oriented electrical steel under compressive stress.

2. Magnetostriction measurement system

The BROCKHAUSE MST magnetostriction measurement system was used in this paper, as shown in Fig. 1. The measurement system includes power supply system, magnetic circuit which composed of yokes and windings, laser transmitting and receiving system, vibration-free table and applied stress device. The emission frequency of the laser transmitter is 100 Hz and the test resolution reaches 10 nm/m.

The effective size of the test specimen is 100 mm×500 mm. The surface of the test specimen shall be flat and smooth without damage. The test specimen was placed in the gap between the two yokes of the measurement system. The laser beam shall be parallel to the axis of the windings and yokes in order to prevent measurement offsets due to vertical and lateral vibrations of the test specimen. The measuring device calculates the deformation of the test specimen by detecting the change of the distance between the laser emission and the laser target.

Fig. 1The magnetostriction measurement system

The size of the test specimen 30SQGD105 is 100 mm×600 mm, and its Rolling Direction and Transverse Direction are as Fig. 2.

The epoxy plates placed on the test specimen between the two ends and the free deformation distance should be enough for the magnetostriction measurement and the blocks were between the upper yoke and the plate as Fig. 3.

Fig. 2The test specimen (30SQGD105)

Fig. 3Measurement process under compressive stress

3. Measurement process and results

4. Magnetostriction measurement under compressive stress

There are three measurement conditions were measured as Table 4.

The magnetostriction parameters, such as zero-to-peak value ${\lambda }_{z-p}$ and peak-to-peak value ${\lambda }_{p-p}$, under different compressive stress were obtained through repeated measurements, ensuring the repeatability. The magnetostriction parameters on 1.2T are shown in Tables 5-6, and Fig. 4(a-d).

It can be concluded from the figures and tables that when a certain weight was placed on the test specimen, the magnetostriction of the grain-oriented electrical steel was decrease with the increase of the weights under zero stress conditions.

It is well know that mechanical stress in grain-oriented electrical steel has a strong influence on magnetostriction. The magnetostriction of grain-oriented electrical steel was more sensitive to the applied compressive stress than other steels. The weight placed on the test specimen to prevent the deformation becomes very important. According to the test, Case 2 was thought better than Case 1 and Case 1was better than Case 3.

Fig. 4Comparison of magnetostriction parameters on 1.2T

a) Comparison of ${\lambda }_{z-p}$

b) Comparison of ${\lambda }_{p-p}$

c) Comparison of AWV

d) Comparison of butterfly loop under –4 MPa

5. Conclusions

The influence of the weight placed on the test specimen on the magnetostriction test results is fully considered in this paper and find the optimal measurement method of magnetostriction measurements under an externally compressive stress, which improves the accuracy and reliability of magnetostriction measurement effectively.

In the case of zero stress, the magnetostriction parameters of the grain-oriented electrical steel, ${\lambda }_{z-p}$ [nm/m], ${\lambda }_{p-p}$ [nm/m] and AWV [DBA], was decrease with increase of the weights placed on the test specimen. So, no weight, except the optical target, shall be placed on the test specimen when the magnetostriction measurement at zero stress.

In the case of under an externally compressive stress, a weight should be placed on the test specimen to prevent a deformation of test specimen. The selection of the weight placed on the test specimen to prevent the deformation becomes very important. The selected weight is too small, the deformation of the test specimen still occurs, and which cause the magnetostriction measurement offset.

It is the most accurate measurement when the placed weight can prevent the deformation of test specimen and at the same time ensure the free movement of magnetic domain of grain-oriented electrical steel. The optimal weight placed on the test specimen needs to be determined according to different brand and thickness of test specimen.

When the weight placed on the test specimen is very large, the free movement of the magnetic domain in grain-oriented electrical steel will be greatly limited, resulting in the magnetostriction, ${\lambda }_{z-p}$ [nm/m], ${\lambda }_{p-p}$ [nm/m] and AWV [DBA] significant decrease, like Case 3. At this case, the magnetostriction data can’t reflect the magnetostriction properties of grain-oriented electrical steel.

Magnetostriction of grain-oriented electrical steel plays an important role in the simulation and design of transformer and reactor because magnetostriction is the main reason to make the vibration and acoustic. Accurate measurement of magnetostriction under the compressive stress is good for product design and simulation.