METHOD FOR IMPROVING MATERIAL MECHANICAL PROPERTIES BY CHANGING GRADIENT NANOTWINNED STRUCTURE OF METAL MATERIAL

Abstract

A method for improving mechanical properties by changing a gradient nanotwinned structure of metallic materials is the technical field of nanostructured metallic materials. The method uses the inherent principles of microstructure and mechanical properties of metallic materials to improve materials mechanical properties. The metallic materials has a gradient nanotwinned structure. The principles of microstructure and mechanical properties of the metallic materials mean that the mechanical properties of the metallic materials are adjusted by changing the structural gradient scale of the nanotwinned structure. The method combines two strengthening methods of nanotwins and gradient structure, and can obviously improve the mechanical properties of the metallic materials. For pure copper materials of the gradient nanotwinned structure prepared by an electrodeposition technology: the yield strength is 481±15 MPa, the tensile strength is 520±12 MPa, the uniform elongation can be 7±0.5%, and the elongation to failure can be 11.7±1.3%.

Claims

1. A method for improving materials mechanical properties by changing a gradient nanotwinned structure of metallic materials, characterized in that the method uses the principles of microstructure and mechanical properties of metallic materials to improve materials mechanical properties; the metallic materials has a gradient nanotwinned structure; and the principles of microstructure and mechanical properties of the metallic materials mean that the mechanical properties of the metallic materials can be adjusted by changing the gradient size of the nanotwinned structure.

2. The method for improving materials mechanical properties by changing the gradient nanotwinned structure of metallic materials according to claim 1, characterized in that the grain size or the twin thickness in each gradient layer presents a gradual change from small to large or from large to small from bottom to top; the corresponding microhardness in each gradient layer also presents a gradual change from large to small or from small to large from bottom to top; therefore, the change of the hardness within a unit distance along a gradient direction is used to represent the change speed of the microstructure (the grain size or the twin lamellae) from bottom to top, and is defined as a structural gradient.

3. The method for improving materials mechanical properties by changing the gradient nanotwinned structure of metallic materials according to claim 2, characterized in that in the principles of the microstructure and mechanical properties of the metallic materials, the structural gradient is increased, the yield strength and work hardening rate of the metallic materials are increased simultaneously, and an elongation to failure is unchanged.

4. The method for improving materials mechanical properties by changing the gradient nanotwinned structure of metallic materials according to claim 2, characterized in that the use of the principles of the microstructure and mechanical properties of metallic materials to improve the mechanical properties means that, the structural gradient of the gradient nanotwinned structure is increased to increase the yield strength and the work hardening rate of bulk metal materials and simultaneously keep the elongation to failure unchanged.

5. The method for improving materials mechanical properties by changing the gradient nanotwinned structure of metallic materials according to claim 1, characterized in that under the conditions of room temperature and tensile rate of 5×10.sup.−3 s.sup.−1, when the structural gradient of pure copper materials is 1-50 GPa/mm, the yield strength is 300-500 MPa, the tensile strength is 350-600 MPa, a uniform elongation is 5-15% and the elongation to failure is 10-20%; and when true strain is 1%, the work hardening rate is 1-3 GPa.

Description

DESCRIPTION OF DRAWINGS

[0023] FIG. 1 is a microstructure diagram of gradient nanotwinned copper in the thickness direction under a scanning electron microscope in embodiment 1.

[0024] FIG. 2 shows sample cross-sectional microhardness distribution of gradient nanotwinned copper along the thickness direction in embodiment 1.

[0025] FIG. 3 shows engineering stress-strain curves of gradient nanotwinned copper and uniform nanotwinned copper in embodiments 1-3.

[0026] FIG. 4 is a microstructure diagram of gradient nanotwinned copper in the thickness direction under a scanning electron microscope in embodiment 2.

[0027] FIG. 5 shows sample cross-sectional microhardness distribution of gradient nanotwinned copper along the thickness direction in embodiment 2.

[0028] FIG. 6 is a microstructure diagram of gradient nanotwinned copper in the thickness direction under a scanning electron microscope in embodiment 3.

[0029] FIG. 7 shows sample cross-sectional microhardness distribution of gradient nanotwinned copper along a thickness direction in embodiment 3.

[0030] FIG. 8 shows change of yield strength and tensile strength of gradient nanotwinned copper with structural gradient.

[0031] FIG. 9 shows change of work hardening rate of gradient nanotwinned copper with structural gradient when true strain is 1%.

[0032] FIG. 10 shows change of elongation to failure of gradient nanotwinned copper materials with structural gradient.

DETAILED DESCRIPTION

[0033] The gradient nanotwinned copper materials in the following embodiments were prepared by a direct current electrodeposition technology. The specific preparation process and parameters are as follows:

[0034] Electrodeposition device: DC stabilized voltage and stabilized current power supply;

[0035] Requirements for an electrolyte used for electrodeposition: MOS grade purity CuSO.sub.4 solution; the metal impurity content of the electrolyte was strictly controlled; the water used for preparing the electrolyte was high-purity deionized water; analytically pure H.sub.2SO.sub.4 was used to adjust the pH value of the electrolyte; and the electrolyte was pH=1.

[0036] The following additives were added to the above CuSO.sub.4 solution:

[0037] A gelatin aqueous solution with a concentration of 5 wt. % prepared by analytically pure gelatin was used, and addition amount is 1 mL/L;

[0038] A NaCl aqueous solution with a concentration of 10 wt. % prepared by high-purity NaCl was used, and addition amount is 0.6 mL/L.

[0039] Cathode and anode requirements: a cathode was a pure copper plate with purity higher than 99.99%, and an anode was a pure titanium plate.

[0040] Electrodeposition process parameters: current density was 30 mA/cm.sup.2; DC electrodepositing: the distance between the cathode and the anode was 100 mm; the area ratio of the cathode to the anode was 15:1; and the cathode and the anode were placed in parallel (center symmetry).

[0041] In the deposition process, the structural gradient of pure copper materials was controlled by controlling the temperature change of the electrolyte. The control of the temperature change of the electrolyte refers to controlling the temperature of the electrolyte to gradually increase or decrease with time; the grain size of the obtained pure copper materials in the direction perpendicular to a deposition surface (gradient direction) and the twin thickness increased or decreased accordingly; the scale of structural gradient of the pure copper materials was controlled by controlling the temperature increasing or decreasing rate of the electrolyte; and in the deposition process, the temperature range of the electrodeposition was: 5-60° C., and the electrodeposition time was 0.1-500 hours.

[0042] The present invention is illustrated below in detail in combination with the drawings and the embodiments.

Embodiment 1

[0043] The total thickness of a copper materials of gradient nanotwinned structure was 400 μm. The sample was composed of micron-sized columnar grains which grow along the deposition direction. The grains contain high-density twin boundaries, and most twin boundaries are parallel to a growth surface. In the present embodiment, the pure copper has one gradient layer. The grain size and the twin thickness in the materials present a monotonically increasing gradient change along the thickness direction; the average grain size was gradually changed from 2.5 μm to 15.8 μm; and the average twin thickness was gradually changed from 29 nm to 72 nm, as shown in FIG. 1.

[0044] In the present embodiment, the microhardness of the gradient nanotwinned copper materials gradually decreased along the thickness direction from 1.5 GPa to 0.8 GPa, which accomplished gradient distribution; and the structural gradient was 1.75 GPa/mm, as shown in FIG. 2.

[0045] In the present embodiment, room temperature tension of the gradient nanotwinned copper materials: curve 1 in FIG. 3 is an engineering stress-strain curve of the electrodeposited gradient nanotwinned copper sample of the present embodiment at room temperature. When the tensile rate is 5×10.sup.−3 s.sup.−1, the yield strength of the gradient nanotwinned copper is 364±12 MPa, the tensile strength is 397±11 MPa, the uniform elongation is 9.8±1.7%, and the elongation to failure is 12.9±1.9%.

Embodiment 2

[0046] Embodiment 2 is different from embodiment 1 in that:

[0047] The gradient nanotwinned copper materials has two gradient layers. The grain size and the twin thickness in the materials present a symmetrical gradient change that increased at first and then decreased along the thickness direction, as shown in FIG. 4.

[0048] In the present embodiment, the cross-sectional hardness of the gradient nanotwinned copper decreased at first and then increased along the thickness direction; and the structural gradient is 3.2 GPa/mm, as shown in FIG. 5.

[0049] In the present embodiment, room-temperature tension of the gradient nanotwinned copper materials: when the tensile rate is 5×10.sup.−3 s.sup.−1, the yield strength is 437±19 MPa, the tensile strength is 471±18 MPa, the uniform elongation is 9.2±1%, and the elongation to failure is 14±1.9%, as shown by curve 2 in FIG. 4.

Embodiment 3

[0050] Embodiment 3 is different from embodiment 1 in that:

[0051] The gradient nanotwinned copper materials has eight gradient layers. The grain size and the twin thickness in the materials present a four-period gradient change that increased at first and then decreased along the thickness direction, and the microstructure diagram of the materials is shown in FIG. 6.

[0052] In the present embodiment, the hardness of the gradient nanotwinned copper presents a four-period gradient change that decreased at first and then increased along the thickness direction; and the structural gradient is 11.6 GPa/mm, as shown in FIG. 7.

[0053] In the present embodiment, room-temperature tension of the gradient nanotwinned copper materials: when the tensile rate is 5×10.sup.−3 s.sup.−1, the yield strength is 481±15 MPa, the tensile strength is 520±12 MPa, the uniform elongation is 7±0.5% and the elongation to failure is 11.7±1.3%, as shown by curve 3 in FIG. 4.

[0054] It can be seen from the above embodiments that the structural gradient increased from 1.75 GPa/mm to 11.6 GPa/mm, the yield strength of the pure copper materials increased from 364±12 MPa to 481±15 MPa, and the elongation to failure is substantially unchanged at 12-14%. FIG. 8, FIG. 9 and FIG. 10 respectively describe the effect of the structural gradient of the pure copper materials on strength, work hardening rate and elongation to failure, indicating that as the structural gradient increases, the yield strength, tensile strength and the work hardening rate of the pure copper significantly increases and the elongation to failure is unchanged. It shows that the change of the structural gradient can effectively regulate the mechanical properties of the metallic materials, so that the metallic materials has both high strength and good plasticity.

Comparative Example 1

[0055] When ordinary annealed coarse-grained pure copper (the grain size is about 25 μm) was tensioned at room temperature, the yield strength is 50 MPa, the tensile strength is about 200 MPa and the elongation to failure is about 50%. After cold rolling deformation, the yield strength and the tensile strength of the copper can be respectively increased to 250 MPa and 290 MPa, respectively, and the elongation to failure is about 8%.

Comparative Example 2

[0056] Australian scientists F. Dalla Torre et al. used the equal channel angular pressing (ECAP) severe plasticity technology to treat pure copper. After two passes of treatment, the microstructure evolved into a uniform layer sheet structure with a sheet layer thickness of about 200 nm. Tensile test results show that the yield strength is about 440 MPa, but the elongation to failure is less than 5% and the uniform elongation is less than 1%.

Comparative Example 3

[0057] Lei Lu research group in Institute of Metal Research, Chinese Academy of Sciences in China used direct-current electrodeposition to prepared a nanotwinned copper sample. The sample is composed of micron-sized columnar grains which grow along the deposition direction. The grains contain high-density twin boundaries, and most twin boundaries are parallel to a growth surface. The tensile properties of the materials depend on the microstructure of the materials (the grain size and the twin lamellae thickness). When the average twin lamellae thickness of the sample (A sample in FIG. 4) is 29 nm and the average grain size is 2.5 μm, the yield strength is 446±10 MPa, the tensile strength is 470±11 MPa and the elongation to failure is only 2±1%. When the average twin thickness of the sample (B sample in FIG. 4) is 95 nm and the average grain size is 18 μm, the yield strength is 223±9 MPa, the tensile strength is 272±4 MPa and the elongation to failure is 29±3%.

Comparative Example 4

[0058] Ke Lu research group in Institute of Metal Research, Chinese Academy of Sciences in China used surface mechanical grinding technology to treat pure copper rods with a diameter of 6 mm. The obtained microstructure is a gradient nanograined structure with a coarse-grained structure (the grain size is about 25 μm) in the core gradually transitioned to nanograins (the grain size is about 20 nm) at the surface. A gradient nanograined layer is located within 150 μm of the surface of the materials, a deformed coarse-grained layer is in a position from 150 μm to 700 μm, and the remaining core is a coarse-grained matrix that was not affected by the deformation. When the materials was tensioned at room temperature, the yield strength was 150 MPa, and the elongation to failure was 50%.

[0059] The results of the above embodiments and comparative examples show that, compared with the conventional strengthening methods (rolling deformation, severe plasticity deformation, introduction of nanotwinned structure, and introduction of gradient structure), the strengthening method using the gradient nanotwinned structure has obvious strengthening advantages. For example, compared with the rolling method, the strengthening method using the gradient nanotwinned structure can obtain materials with higher strength and better ductility. Compared with the nanolayered structure obtained by the severe plasticity deformation, the gradient nanotwinned structure can maintain higher strength and better ductility. Compared with the uniform nanotwinned structure, the strengthened gradient nanotwinned structure has the strength greater than the strength of the strongest uniform nanotwinned materials A, and also has better ductility, and overcomes the disadvantage that high-strength uniform nanotwinned materials has almost no ductility, which makes the advantage of the gradient structure apparent. Compared with the gradient nanograined structure, the gradient nanotwinned structure has the strength which is higher by about 4 times, has considerable ductility, and overcomes the disadvantage that the gradient nanostructure with good ductility has lower strength, which makes the advantage of the nanotwinned structure apparent. In conclusion, the gradient nanotwinned structure combines the advantages of the nanotwinned structure and the gradient structure, and can solve the problem that the metallic materials is difficult to simultaneously have high strength and good ductility. The structural gradient size of the gradient nanotwinned structure is also adjusted to effectively regulate the mechanical properties of the metallic materials.