Abstract
A quasi-static tensile test was performed on a 1.4 mm-thick TRIP780 steel strip with welding points. An MTS810 material test machine was used in the test, and a Split Hopkinson tension bar device was used in performing impact stretch loading at different strain rates. The dynamic tensile stress–strain curve of the spot welding material with different strain rates was obtained through the finely designed Hopkinson rod test, and the strain rate dependence of a TRIP780 steel spot welding material was discussed. According to the dynamic constitutive equation of the TRIP780 steel spot welding material, the test results were numerically simulated, the constitutive description and test curves were compared, and the simulation results and test results were discussed and analyzed. The fractures of the test recovery specimen were scanned with the scanning electron microscope, and the fracture mechanism of the TRIP780 steel spot welding material was explored by observing the fractures. The surfaces of the fractures surface showed obvious cleavage river patterns, and the evolution process of microcracks was determined and used in characterizing brittle fractures in specimen spot welding sample subjected to dynamic stretch loading.
1 Introduction
Welding is the most economical and effective method of permanently connecting metals. The dynamic mechanical characteristics of resistance spot welding materials is essential to automobiles, ships, or spacecraft with resistance spot welding structure and under impact load. The dynamic mechanical properties of metals have been at the forefront of research on impact dynamics, and substantial research progress has achieved recently [1,2,3,4,5,6,7,8,9]. Under quasi-static tensile load, research progress [10,11,12,13,14,15,16,17,18,19] of damage evolution can also be popularized and applied to dynamic tensile fractures. The dynamic mechanical properties of steel-based materials have been extensively studied. For example, Oliver et al. [20], Sun et al. [21], and Sung et al. [22] studied the correlation between the strain rate and the failure mode of DP steel. Slycken et al. [23] described the mechanical properties and the phase composition of a TRIP steel under high strain rate loading conditions. Finally, Kang et al. [24], Nicholas [25], and Huh et al. [26] developed and improved the Hopkinson pole tensile test for steel bars. The mechanical behavior of materials has been simulated at high strain rates [27,28].
The quasi-static tensile test was performed on a 1.4 mm-thick TRIP780 steel strip with welding points. An MTS810 material test machine was used in the test. The Split Hopkinson tension bar (SHTB) device was used for impact stretch loading at different strain rates. By using the finely designed Hopkinson rod test, the dynamic tensile stress–strain curve of the spot welding material with different strain rates was obtained, and the strain rate dependence of the welding material was explored. The results of the dynamic tensile test were numerically simulated using the dynamic composition equation of a welding spot material used in our another other study and compared with the stress–strain curve obtained through an experiment. The recovered sample was observed with a scanning electron microscope, and the results of microdamage evolution were obtained. Finally, the fracture pattern of the dynamic tensile fracture of the welding spot material was analyzed.
2 Quasi-static and dynamic tensile test
The TRIP780steel plate was 1.400 mm thick. The time interval between two welding processes was 20 ms, and the welding time and holding time were 130 and 250 ms, respectively. Initially, the welding pressure was 4.300 KN. The quasi-static tensile experiment was carried out on a specimen by using the MTS 810 material test machine, as shown in Figure 1. The quasi-static tensile experiment on TRIP780 steel single-piece specimens was carried out on the same test machine, and a solder pot was used. The stress–strain curve of the welding spot material was obtained, and the specimen and its size and design are shown in Figure 2. Resistance spot welding material was in the middle of the specimen, with a length of 3 mm.

MTS 810 material testing machine.

Size of the single-piece steel strip specimen with solder joints, unit: mm.
The quasi-static tensile test stress–strain curve is shown in Figure 3. The front end of the curve is not linear possibly because of a connection problem between the specimen and the loading device, and a relative slip occurs between the specimen and loading device at the start of loading.

Quasi-static tensile stress–strain curve.
The dynamic tensile test of the specimen was performed on the Hopkinson rod. The test device is shown in Figure 4. In the test, the specimen was connected to the incident and transmission bars. When the compressed gas drives a cylinder-shaped projectile with a length of

Hopkinson rod test device diagram
In the experiment, the diameters of the incident and transmission bars were 19 mm, with lengths of 2.7 and 1.5 m, respectively. The length of the bullet was 300 mm. The incident bar, transmission bar, target plate, and bullet were made of high-strength alloy steel with elastic modulus E of 190 GPa and Poisson ratio
where t is time;
The dynamic tensile test stress–strain curve of the specimen at different strain rates is shown in Figure 5. Stress and strain increase with the strain rate although the resulting curve is somewhat irregular. The curve indicates that the spot welding material has a certain strain rate dependence.

Dynamic tensile stress–strain curve.
The recycled photographs of the specimen for the quasi-static tensile and Hopkinson rod tests are shown in Figures 6 and 7, respectively. As shown in Figure 6, in the quasi-static tensile experiment, the specimen is sheared and broken, and the fracture is 45°. As shown in Figure 7, the specimen fracture is not an obvious 45° because of dynamic loading.

Recycling specimens under the quasi-static load test.

Recycling specimens under the dynamic tensile test.
3 Constitutive description
The HV test was performed on the RSW materials of TRIP780 steel. To disclose the HV values of BM, HAZ, and FZ on the RSW material samples, points were set on the left BM and HAZ, center FZ, and right HAZ and BM successively along a biased line that runs through the FZ center. Specifically, points were set horizontally along the center line of BM of the steel plate (1 mm), then turning to the FZ center from the outer edge of HAZ and running through the FZ center and to the horizontal direction of the outer edge of the opposite HAZ (1 mm). The interval between the two points was 0.200 mm. Distribution of the testing points is shown in the dotted line in Figure 8. This study set five points in the right and right BM zones, respectively; four points in the right and right HAZ zones, respectively; and 26 points in the center FZ zone. Therefore, a total of 44 hardness test points in the RSW zone were set.

The RSW cross-sectional micrograph and dot position.
For a clear display of the HV hardness values of different parts of the RSW material samples, experimental results and length of RSW material samples were placed in the same coordinate system, and a variation curve of the hardness with length was drawn (Figure 9).

Hardness–length curve.
In the welding process, bainites in BM are transformed into austenites. With the continuous increase of temperature, ferrites in BM can also be transformed into austenites. Under this circumstance, plastic deformation is developed in the welding zone under spot-welding pressure. With the reduction of temperature, structures are recrystallized and martensitic structures are obtained after cooling. Figure 9 shows that the hardness values of FZ and HAZ are relatively high, whereas that of BM is relatively low. The main reason is that FZ and HAZ are mainly composed of martensites, while BM is mainly composed of ferrites. The hardness values of martensites are higher than those of ferrites. The hardness values of FZ are different from those of HAZ because HAZ components include some residual ferrites relative to the components of FZ, thereby resulting in lower hardness of HAZ than that of FZ. In Figure 9, point S shows the softening point of hardness, which is less than the hardness of wood. The microhardness decreases as the steel plates receive fast thermal circulation at welding.
Roth and Mohr [29] decoupled the strain hardening effect, strain rate hardening effect, and temperature softening effect of materials with reference to the Johnson–Cook constitutive model, thereby obtaining the following dynamic constitutive equation:
where
The expression of
where
Model parameters of TRIP780 steel used in constitutive description of a typical experiment are listed in Table 1.
The modified Johnson–Cook model parameters for TRIP780 steel used in simulation
|
|
|
|
|
|
---|---|---|---|---|---|
1526.5 | 0.00519 | 0.242 | 0.00557 | 0.00321 | 1.025 |
|
|
|
|
|
|
---|---|---|---|---|---|
293 | 1806.7 | 185 | 0.33 | 420 | 7,850 |
As the material properties of the welding zone are significantly different from BM in the welding process, we hypothesized that only changes of yield stress in the welding zone are considered in the numerical model, and other mechanical properties and failure parameters are constant in the specimens, as mentioned by Nielsen [30]. It is hypothesized that a linear correlation exists between microhardness and yield stress. Therefore, hardness in the RSW zone is attributed to the hardness of BM. On this basis, the dynamic constitutive equation of the RSW zone of TRIP780 steel is obtained as follows:
where RSW represents RSW materials.
We use equation (6) to analyze the results of the dynamic tensile test performed on the specimen. Then, the stress–strain curve was obtained through constitutive description on the basis of the corresponding strain rate and compared with the experimental curve (Figure 10). The comparison results showed that the simulation and experimental results were basically in line with each other but not completely consistent. We believe that this result is related to the dynamic tensile test conditions and processes, including the machining accuracy of the specimen, the closeness of the connection between the specimen and the rod, and the paste quality of the strain gauge, which may have affected the experimental results.

Comparison between experimental results and constitutive description.
The fracture of metal material on a microscale is caused by the nucleation, growth, and aggregation of cavities or cracks, which result in ductile or brittle fractures. The increase in the number of cavities or cracks must be aggregated or combined to form a continuous surface and split the specimen. We used an electron microscope to scan a fracture of the dynamic tensile test and the recycling test (Figure 11). By observing the fracture, we observed an obvious cleavage river pattern and the evolution of microcracks. The specimen spot welding part was a brittle fracture.

Scanning electron microscope image of the specimen fracture.
4 Conclusion
The quasi-static tensile and Hopkinson rod tests were carried out on TRIP780 steel with solder joints, and the stress–strain curve under the quasi-static tensile was obtained, as well as the stress–strain curve under dynamic tensile at different strain rates. The test results show that the TRIP780 steel spot welding material has a certain strain rate dependence.
The experimental results were numerically simulated using the dynamic material of TRIP780 steel spot welding material obtained. The comparative results show that the constitutive description and test curves were basically in line with the results, and what caused the inconsistence was considered related to the test conditions and processes.
Through electron microscopy and dynamic tensile test, the fractures of the recycled specimen were scanned during the dynamic tensile test. The fracture had an obvious cleavage river pattern, microcrack evolution, and the specimen spot welding part was a brittle fracture.
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© 2020 Xiaomin Li and Jianrong Zhang, published by De Gruyter
This work is licensed under the Creative Commons Attribution 4.0 International License.
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- Energy equilibrium analysis in the effervescent atomization
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- Investigation on thermal-hydraulic performance prediction of a new parallel-flow shell and tube heat exchanger with different surrogate models
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- Effect of the inner-surface baffles on the tangential acoustic mode in the cylindrical combustor
- Special Issue on Future challenges of advanced computational modeling on nonlinear physical phenomena - Part I
- Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications
- Some new extensions for fractional integral operator having exponential in the kernel and their applications in physical systems
- Exact optical solitons of the perturbed nonlinear Schrödinger–Hirota equation with Kerr law nonlinearity in nonlinear fiber optics
- Analytical mathematical schemes: Circular rod grounded via transverse Poisson’s effect and extensive wave propagation on the surface of water
- Closed-form wave structures of the space-time fractional Hirota–Satsuma coupled KdV equation with nonlinear physical phenomena
- Some misinterpretations and lack of understanding in differential operators with no singular kernels
- Stable solutions to the nonlinear RLC transmission line equation and the Sinh–Poisson equation arising in mathematical physics
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- Standard routine techniques of modeling of tick-borne encephalitis
- Fractional residual power series method for the analytical and approximate studies of fractional physical phenomena
- Exact solutions of space–time fractional KdV–MKdV equation and Konopelchenko–Dubrovsky equation
- Approximate analytical fractional view of convection–diffusion equations
- Heat and mass transport investigation in radiative and chemically reacting fluid over a differentially heated surface and internal heating
- On solitary wave solutions of a peptide group system with higher order saturable nonlinearity
- Extension of optimal homotopy asymptotic method with use of Daftardar–Jeffery polynomials to Hirota–Satsuma coupled system of Korteweg–de Vries equations
- Unsteady nano-bioconvective channel flow with effect of nth order chemical reaction
- On the flow of MHD generalized maxwell fluid via porous rectangular duct
- Study on the applications of two analytical methods for the construction of traveling wave solutions of the modified equal width equation
- Numerical solution of two-term time-fractional PDE models arising in mathematical physics using local meshless method
- A powerful numerical technique for treating twelfth-order boundary value problems
- Fundamental solutions for the long–short-wave interaction system
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- Exact solutions of the Laplace fractional boundary value problems via natural decomposition method
- Special Issue on 19th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering
- Joint use of eddy current imaging and fuzzy similarities to assess the integrity of steel plates
- Uncertainty quantification in the design of wireless power transfer systems
- Influence of unequal stator tooth width on the performance of outer-rotor permanent magnet machines
- New elements within finite element modeling of magnetostriction phenomenon in BLDC motor
- Evaluation of localized heat transfer coefficient for induction heating apparatus by thermal fluid analysis based on the HSMAC method
- Experimental set up for magnetomechanical measurements with a closed flux path sample
- Influence of the earth connections of the PWM drive on the voltage constraints endured by the motor insulation
- High temperature machine: Characterization of materials for the electrical insulation
- Architecture choices for high-temperature synchronous machines
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- High-power density induction machines with increased windings temperature
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- Erratum
- Erratum to “Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications”