# Experimental Study on the Tensile Property of a Novel Oriented Linear Porous Metal

Authors: Bin Liu; Xin-gang Wang; Yong Tang; Wei Yuan; Chao-bin Fang; Zhen-ping Wan
Journal: Advances in Materials Science and Engineering
 (2016)

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## Abstract

A novel oriented linear porous metal (OLPM) with high porosity was fabricated through solid-sintering method with cutting copper fibers. In this study, tensile experiments were conducted to investigate the fracture process of the OLPM and the effects of porosity and sintering parameters on the tensile properties. The typical tensile stress-strain plot of this material was obtained based on a large number of tensile test results. The plot can be divided into three stages, namely, initial linear elastic stage, plastic deformation stage, and tensile fracture stage. Based on the results, the fracture mechanism of the OLPM was further studied. Moreover, the porosity and sintering parameters were also varied to investigate their influence on the tensile properties. Tensile strength and plastic deformation were found to decrease with increasing porosity ranging from 70% to 90%. A higher sintering temperature produced a higher tensile strength for the OLPM sintered in the temperature range of 700°C–900°C, but the strength decreased at 1000°C. In addition, the extension of holding time could also slightly affect the tensile strength. Finally, the tensile properties of the OLPM are significantly higher than those of commercial porous metal and porous metal fiber sintered sheet.


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## Body

## 1. Introduction

Porous metals with unique structural and functional properties have received extensive attention because of the interesting combinations of their outstanding thermal, acoustic, electrical, and mechanical properties [1, 2]. Porous metal fiber sintered sheet (PMFSS), which is a new type of porous metal, has a three-dimensional reticulated structure characterized by high porosity and large specific surface area, and this material exhibits great potential for various applications in industry. To date, PMFSS is being widely used in defense and military, petrochemical industry, metallurgical machinery, environmental protection for its excellent performance in filtration and separation [3], flow field and gas diffusion [4], energy absorption [5], biomedical device [6], catalytic reaction [7, 8], heat transfer [9], and other applications. With the expansion of their application fields and the increasing complexity of their working environment, some special requirements for their properties of porous metals are becoming increasingly strict. In this study, a novel oriented linear porous metal (OLPM) with oriented linear porous structure and large porosity feature was produced, and this material has shown good potential in flow distribution and pressure drop, and it has been used in methanol steam reforming and presented a good performance [10, 11].To broaden the application of this material, the relationship between its mechanical properties and its special structure should be elucidated.In the past decades, many research groups have given significant attention to the fabrication, characterization, and application of porous metals [12, 13]. Thus far, many studies have developed new fabrication methods and improved the mechanical properties of porous metals. Markaki and Clyne [14, 15] produced novel porous sheets using liquid phase sintering method of short stainless steel fibers with 100 μm diameter. They found that the porous sheets had a porosity varying from 75% to 95% and a tensile strength below 1 MPa. Liu et al. [16, 17] developed a porous steel wire mesh material with open porosities prepared by the metallurgical route. The effect of the forming pressure and sintering parameters on the porous structure and mechanical behavior were further discussed. Moreover, Xi et al. [18, 19] fabricated a PMFSS using the vacuum sintering of stainless steel fibers with a diameter of 100 μm, and they introduced several methods to study the compressive and shear properties of PMFSS. Recently, Jin et al. [20] proposed a two-dimensional micromechanics random beam model to investigate the elastic-plastic behavior of PMFSS. In our previous studies [21–23], the tensile, compressive, and shear properties of the PMFSS have been investigated through experimental testing and microstructure observation method. These results provide an effective guideline in improving the design and manufacture methods of PMFSS for different engineering applications.However, only a few studies have been conducted in the field of oriented linear porous metal. Huang et al. [24] fabricated a kind of porous copper with long cylindrical pores through directional solidification, and the compressive properties were investigated through experimental methods. Liu et al. [25] fabricated lotus-type porous copper bars with 45 mm diameter and 120 mm length through unidirectional solidification and the compressive deformation process was investigated, and the deformation mechanism was analyzed and discussed.The above reported studies show that detailed research on the tensile properties of oriented linear porous metal using cutting metal fibers is lacking in the current literatures. This study investigated the tensile fracture process of this material produced by the solid-sintering of copper fibers. After the microstructures are examined, the tensile properties of the oriented linear porous metal are further analyzed and discussed by varying the porosity and sintering parameters. Finally, the tensile property of OLPM was compared with the commercial porous metal and the PMFSS.


## 2. Experimental Procedure

### 2.1. Manufacturing Process of OLPM

As reported previously [10], the preparation of oriented linear porous metal mainly includes three processes, namely, the fabrication of cutting fibers, the mold-pressing of parallel fibers, and the sintering with high temperature in a protective gas atmosphere.First, long copper fibers were fabricated by a multitooth tool on a horizontal lathe. Figure1 shows the schematic drawing of the multitooth tool; Figure 2 shows the fiber manufacturing process. The tool was installed on the turret with a setting angle of 45 degrees, and it has multiple tiny teeth fabricated through wire electrical discharge machining for achieving the simultaneous fabrication of multiple fibers. The distance and height of the tiny teeth were 0.3 mm and 0.2 mm, respectively. The diameter of the cutting fibers was approximately 100 μm. The cutting fibers were collected by twining the fibers in a slab parallel to one another.Figure 1
Schematic drawing of the multitooth tool.Figure 2
In situ photo of copper fiber manufacturing.Second, the copper fibers were cut into several segments with fixed length of 120 mm. Thereafter, multiple segments of copper fibers were uniformly arranged in parallel and put into the packing chamber of a mold pressing equipment, in which multiple stainless steel plates patterned with hollow chamber were first stacked and then tightened with four screws and two end plates. Through this means, the semifinished OLPM with the same shape as the predetermined packing chamber was obtained.Later, the mold pressing equipment was put into a box-type furnace, which provided the hydrogen gas atmosphere with a constant pressure of 0.3 MPa. The sintering temperature was set in the range of 700°C to 1000°C and was controlled by a programmable temperature controller. Stage heating method was used to optimize the heating rate. The heating rate was kept at 300°C/h when the temperature was below 800°C, whereas it reduced to 200°C/h as the temperature rose above 800°C. The holding times were set as 30 min, 60 min, 90 min, or 120 min. When the sintering process was completed, the furnace was cooled to 150°C, and then the mold pressing equipment was taken out of the furnace and continued to cool down to room temperature. Lastly, the mold pressing equipment was disassembled and hence the OLPM with uniform thickness was formed.The average porosity of the OLPM can be calculated using the quality-volume method formulated by the following because the obtained porous metal has a regular geometric shape:(1)
θ
%
=
1
-
M
ρ
V
×
100
,where θ is the porosity of the porous metal, V is the volume of the porous metal (cm3), M is the mass of the porous metal (g), and ρ is the density of red copper (g/cm3).The dimension of the OLPM sample is 120 mm∗ 15 mm ∗ 2 mm. Before being tested, the sample was cleaned ultrasonically with acetone for 5 min and then with deionized water for 5 min; finally, it was left to dry in air at ambient temperature. The microscopic morphology of the OLPM was observed using a scanning electron microscope (JSM-6380LA, Japan).


### 2.2. Tensile Test of OLPM

The tensile test was carried out on a PC-controlled electronics universal testing machine (RGL-20A) with a maximum load of 20 kN, performing both test control and data acquisition. Before test, the sample was clapped in the machine to make sure that the test part was 60 mm in length. To avoid the deformation of the three-dimensional network structure in the clamping process, rubber pads were placed between clamps. All the samples were pulled to failure at a constant tensile rate of 1.5 mm/min; and the tensile direction was the same with the direction of metal fibers. During each test, the load and displacement were recorded continuously. The strain is defined as the ratio between the sample elongation and the initial gauge length. The tensile stress is calculated by dividing the pulling force by the initial section of the sample. The maximum stress in the stress-strain plots was determined as the tensile strength of the OLPM. In order to obtain an accurate value of tensile strength, three specimens were tested in each case, and the average was taken.


## 2.1. Manufacturing Process of OLPM

As reported previously [10], the preparation of oriented linear porous metal mainly includes three processes, namely, the fabrication of cutting fibers, the mold-pressing of parallel fibers, and the sintering with high temperature in a protective gas atmosphere.First, long copper fibers were fabricated by a multitooth tool on a horizontal lathe. Figure1 shows the schematic drawing of the multitooth tool; Figure 2 shows the fiber manufacturing process. The tool was installed on the turret with a setting angle of 45 degrees, and it has multiple tiny teeth fabricated through wire electrical discharge machining for achieving the simultaneous fabrication of multiple fibers. The distance and height of the tiny teeth were 0.3 mm and 0.2 mm, respectively. The diameter of the cutting fibers was approximately 100 μm. The cutting fibers were collected by twining the fibers in a slab parallel to one another.Figure 1
Schematic drawing of the multitooth tool.Figure 2
In situ photo of copper fiber manufacturing.Second, the copper fibers were cut into several segments with fixed length of 120 mm. Thereafter, multiple segments of copper fibers were uniformly arranged in parallel and put into the packing chamber of a mold pressing equipment, in which multiple stainless steel plates patterned with hollow chamber were first stacked and then tightened with four screws and two end plates. Through this means, the semifinished OLPM with the same shape as the predetermined packing chamber was obtained.Later, the mold pressing equipment was put into a box-type furnace, which provided the hydrogen gas atmosphere with a constant pressure of 0.3 MPa. The sintering temperature was set in the range of 700°C to 1000°C and was controlled by a programmable temperature controller. Stage heating method was used to optimize the heating rate. The heating rate was kept at 300°C/h when the temperature was below 800°C, whereas it reduced to 200°C/h as the temperature rose above 800°C. The holding times were set as 30 min, 60 min, 90 min, or 120 min. When the sintering process was completed, the furnace was cooled to 150°C, and then the mold pressing equipment was taken out of the furnace and continued to cool down to room temperature. Lastly, the mold pressing equipment was disassembled and hence the OLPM with uniform thickness was formed.The average porosity of the OLPM can be calculated using the quality-volume method formulated by the following because the obtained porous metal has a regular geometric shape:(1)
θ
%
=
1
-
M
ρ
V
×
100
,where θ is the porosity of the porous metal, V is the volume of the porous metal (cm3), M is the mass of the porous metal (g), and ρ is the density of red copper (g/cm3).The dimension of the OLPM sample is 120 mm∗ 15 mm ∗ 2 mm. Before being tested, the sample was cleaned ultrasonically with acetone for 5 min and then with deionized water for 5 min; finally, it was left to dry in air at ambient temperature. The microscopic morphology of the OLPM was observed using a scanning electron microscope (JSM-6380LA, Japan).


## 2.2. Tensile Test of OLPM

The tensile test was carried out on a PC-controlled electronics universal testing machine (RGL-20A) with a maximum load of 20 kN, performing both test control and data acquisition. Before test, the sample was clapped in the machine to make sure that the test part was 60 mm in length. To avoid the deformation of the three-dimensional network structure in the clamping process, rubber pads were placed between clamps. All the samples were pulled to failure at a constant tensile rate of 1.5 mm/min; and the tensile direction was the same with the direction of metal fibers. During each test, the load and displacement were recorded continuously. The strain is defined as the ratio between the sample elongation and the initial gauge length. The tensile stress is calculated by dividing the pulling force by the initial section of the sample. The maximum stress in the stress-strain plots was determined as the tensile strength of the OLPM. In order to obtain an accurate value of tensile strength, three specimens were tested in each case, and the average was taken.


## 3. Results and Discussion

### 3.1. Microstructure of OLPM

The SEM image of the OLPM sintered at 800°C for 30 min is shown in Figure3. It can be seen from Figure 3 that there are many sintering joints and pore structures in the OLPM. The contact points among metal fibers transferred into sintering joints and formed the pore structure and the three-dimensional network structure of the OLPM during the sintering process. The pore structure formed among the parallel fibers and sintering joints showed different appearance, like long strip pore structure and point pore structure, but they are all along with the direction of the metal fiber. We can get a wide range of porosity (60%–98%) by changing the quantity of metal fibers and the molding pressure.Figure 3
SEM image of the OLPM.By further investigation of Figure3, we can see that there are many microstructures on the surface of metal fibers. These rough surface morphologies are the unique features of the OLPM compared with other commercial porous metals shown in Figure 4. The surface of the metal fiber in the Biało et al. research is also very smooth [26]. These metal fibers are fabricated by melt-extraction [27] or bundle drawing method [28].Figure 4
SEM image of the CPM.What is more, the rough surface can favor the sintering joints and improve the mechanical properties of the oriented linear porous metal. The rough surface increases the friction between fibers and provides an additional occlusal force that makes the fibers bond tightly, thus forming a relatively strong structure. More importantly, the rough surface can provide higher specific surface area and can promote adhesive strength of the primer to the metallic support when the OLPM is used as catalyst support [10, 11].


### 3.2. Tensile Fracture Process of OLPM

Figure5 shows the representative tensile stress-strain curve of an OLPM sample with 70% porosity sintered at 700°C for 30 min. It can been seen from this figure that the tensile behavior of the OLPM sample can be divided into three stages: (a) initial linear elastic stage, (b) plastic deformation stage, and (c) fracture stage, which correspond to OA, AB, and BC in the curve, respectively.Figure 5
Typical tensile stress-strain curve of an oriented linear porous metal sample.The figure shows that the engineering stress increased linearly with the increasing strain in the initial stage, namely, the OA part of the plot. This process only lasts for a short time, and the elastic deformation of this sample is about 2%. The relationship between stress and strain fits well with Hooke’s law of elasticity. That is to say, in the initial elastic process, the oriented linear porous metal elongated in the tensile direction, and only a slight deformation occurs on the three-dimensional reticulation.After the elastic process, the sample reaches the plastic deformation process quickly. In this stage, deformation begins to occur in some metal fibers first, where the local stress concentration occurs, fibers reach the yield limitation first, and the plastic deformation starts here. The local plastic deformation results in stress release and redistribution, which leads to a greater plastic deformation of more fibers with tension continuously increasing. As the plastic deformation capacity of the three-dimensional reticulated skeleton is exhausted, the stress reached the ultimate tensile strength.With the fracture of the metal fiber gradually evolving into the sintering joint and the entire three-dimensional reticulated structure, the three-dimensional structure becomes prone to fracture. And the porous metal reaches the fracture stage; the engineering stress decreased sharply with the increasing strain in this stage; and this phenomenon lasts until the structure cannot undertake any load. And finally, the sample fails completely.


### 3.3. Tensile Fracture Mechanism of OLPM

To get a better understanding of the fracture of the OLPM, the facture mechanism of this new material was investigated in this study. The fracture process and the fractured samples were observed and analyzed.The fracture image of the OLPM in the thickness direction was shown in Figure6. It is clearly shown in Figure 6 that the fracture region becomes thicker and looser than any other part of the material because the fracture process first occurs in the surface of the material, where the restriction of the fibers is relatively smaller than that in the center of the material and where the deformation is larger than that in the center.Figure 6
Fracture image of the OLPM in the thickness direction.In addition, an obvious necking phenomenon is observed in the width direction along with the tensile load during the fracture process, as shown in Figure7. This figure indicates that the oriented linear porous metal is a typical plastic material. Besides that, there is no obvious fracture trace in the fracture region of the OLPM. These phenomena are quite different from our previous studies with PMFSS [21], which is also a porous material made from metal fiber. This phenomenon can be caused by the following reasons. First, the metal fibers in the OLPM are parallel to one another, and the sintering joints are also found along with the direction of the metal fiber; that is, all the metal fibers in the OLPM are almost in the same condition, and this condition is good for the material to maintain the plastic property of the metal fiber itself. Figure 8 shows the fracture morphology of metal fibers in the OLPM. It clearly shows that the metal fiber also undergoes a necking deformation under the tensile strength and maintains the original performance itself. Second, unlike the PMFSS, no fiber-to-fiber cross sintering joints and no pore structure perpendicular to the fiber direction restrict the elongation and deformation in the load direction. So the material can extend in the tensile direction. This structure is helpful to strengthen the mechanical properties and the ductility of the OLPM.Figure 7
Appearance of the fractured OLPM.Figure 8
SEM image of fractured metal fibers in OLPM.


### 3.4. Influence of Porosity

Porosity is one of the most important factors of porous metals, and it greatly influences the mechanical properties of porous metals [29, 30]. To analyze the influence of porosity on the tensile property of the OLPM, a single factor experiment was conducted. Three kinds of OLPM sintered at 800°C for 30 min with porosities of 70%, 80%, and 90% were used to investigate the effect of porosity on the tensile property.Figure9 shows the tensile stress-strain plots of the OLPM with different porosities sintered at 800°C for 30 min. The tensile strength of the OLPM decreases greatly with the increase of porosity. As shown in Figure 8, the tensile strength of the sample with 70% porosity is 16.68 MPa, whereas those of the samples with the porosities of 80% and 90% are only 10.12 MPa and 7.37 MPa, respectively. This result fits well with the result of Qiao et al. [19]. This result is mainly attributed to the following two aspects. On the one hand, the OLPM sample with lower porosity has more fibers and sintering joints in its cross-section to withstand the tensile force. Conversely, the sample with higher porosity has less fibers and contact regions to form sintering joints. On the other hand, in order to obtain high porosity, sparse fibers are distributed in the mold and low compaction force is applied, which hinder the formation of solid-sintering joints and lead to the sintering joints weaker than those of low porosity. And the stress concentration first occurs at them. These two aspects both result in low tensile strength in high porosity.Figure 9
Tensile stress-strain curves of the oriented linear porous metal with different porosities.In addition, Figure9 also illustrates that the sample with lower porosity shows a longer plastic stage. The total deformation of OLPM with 70% porosity is 20.85%, while the ductility of OLPMs with 80% and 90% porosity is 16.97% and 15.66%, respectively. That is because higher porosity means less metal fibers in the OLPM, and the faster the fracture process transfer into the three-dimensional structure of the OLPM, the smaller the deformation of the whole process.After the plastic deformation stage, the fracture rates of the samples with different porosities are not identical. The stress-strain curve of the sample with lower porosity drops more sharply, which means that the sample fractures faster.


### 3.5. Influence of Sintering Parameters

As important manufacturing parameters, sintering temperature and sintering time greatly influence the forming process of the oriented linear porous metal.


#### 3.5.1. Sintering Temperature

Four samples with 70% porosity sintered at 700°C, 800°C, 900°C, and 1000°C for 30 min were selected to investigate the influence of sintering temperature on the tensile strength of the oriented linear porous metal. Figure10 shows the tensile strength plot of the OLPM samples sintered at different temperatures.Figure 10
Tensile strength of the oriented linear porous metal with different sintering temperatures.Obviously, the tensile strength of the OLPM increases with sintering temperatures between 700°C and 900°C, but it decreases at 1000°C. This mainly because the formation of sintering joints is controlled by atom diffusion, which is a random thermal motion. High sintering temperature increases the energy of copper atoms [31, 32]. On the one hand, it increases the number of activated copper atoms and the opportunity of copper fibers forming the sintering joints. On the other hand, it is beneficial for the migration of copper atoms, thus accelerating the sintering process [33]. Therefore, the number of sintering joints increases and sintering joints grow larger. These phenomena will lead to the improvement of the tensile property of the OLPM. Therefore, in the range of 700°C to 900°C, the tensile strength increases with sintering temperature. However, during the sintering process, the metal fiber undergoes a heat treatment process, the increasing sintering temperature enlarges the grain size of the copper fiber when the temperature is higher than the recrystallization temperature, and the microstructure on the surface of the metal fiber will disappear at high temperature [34]. These phenomena will all lead to the decrease of tensile property at 1000°C. This situation provides us with a guide that a reasonable sintering temperature to fulfill different requirements could be chosen.


#### 3.5.2. Holding Time

The tensile property of the porous metal with the porosity of 70% sintered at 800°C for 30 min, 60 min, 90 min, and 120 min is shown in Figure11. From Figure 11, we can conclude that holding time has slight effect on the tensile property of OLPM. When the sintering time was extended from 30 min to 60 min, the tensile strength increased from 16.68 MPa to 16.92 MPa. However, the sintering time of 60 min leads to the maximum tensile strength at the sintering temperature of 800°C, and the tensile strength decreases to 16.65 MPa and 15.16 MPa when the sintering time increases to 90 min and 120 min, respectively. The difference between different holding time is 11%.Figure 11
Tensile strength of the oriented linear porous metal with different holding times.The results are caused by the following two aspects. On the one hand, sintering joints formed between fibers become larger with the increase of sintering time, leading to the improvement of the tensile properties of the porous metal. Meanwhile, the increase of sintering time caused the grain of the copper fibers to become coarse, leading to the decrease in the mechanical property of the fiber itself and then to the decrease of the tensile properties of the material. The combination of the two aspects leads to the result. In addition, the lengthening of the sintering time increases the manufacturing cost of the oriented linear porous metal. Therefore, improving the tensile strength of the porous metal by extending the sintering time is not logical.


### 3.6. Comparing with Commercial Porous Metal and PMFSS

The tensile strength of the oriented linear porous metal was compared with the commercial porous metal and the porous metal fiber sintered sheet [21]. Figure 12 shows the tensile strengths of three kinds of materials sintered at 800°C for 30 min and 60 min with 80% porosity. The figure shows that the tensile strength of the OLPM is significantly higher than those of the other two kinds of materials. This result is because that the surface of the metal fiber in CPM is smooth, as shown in Figure 4. It is relatively difficult for the metal fiber to form sintering joints between the smooth surfaces [35], so the tensile strength is relatively lower than that of the oriented linear porous metal. The metal fibers in the PMFSS occlude one another, and not all the metal fibers can resist the tension force, so the tensile strength is significantly lower than that of the oriented linear porous metal.Figure 12
Tensile strength of three different porous metals.These results obtained provide us with an important technical guideline for different potential applications of the OLPM, especially for the conditions with the tensile loading.


## 3.1. Microstructure of OLPM

The SEM image of the OLPM sintered at 800°C for 30 min is shown in Figure3. It can be seen from Figure 3 that there are many sintering joints and pore structures in the OLPM. The contact points among metal fibers transferred into sintering joints and formed the pore structure and the three-dimensional network structure of the OLPM during the sintering process. The pore structure formed among the parallel fibers and sintering joints showed different appearance, like long strip pore structure and point pore structure, but they are all along with the direction of the metal fiber. We can get a wide range of porosity (60%–98%) by changing the quantity of metal fibers and the molding pressure.Figure 3
SEM image of the OLPM.By further investigation of Figure3, we can see that there are many microstructures on the surface of metal fibers. These rough surface morphologies are the unique features of the OLPM compared with other commercial porous metals shown in Figure 4. The surface of the metal fiber in the Biało et al. research is also very smooth [26]. These metal fibers are fabricated by melt-extraction [27] or bundle drawing method [28].Figure 4
SEM image of the CPM.What is more, the rough surface can favor the sintering joints and improve the mechanical properties of the oriented linear porous metal. The rough surface increases the friction between fibers and provides an additional occlusal force that makes the fibers bond tightly, thus forming a relatively strong structure. More importantly, the rough surface can provide higher specific surface area and can promote adhesive strength of the primer to the metallic support when the OLPM is used as catalyst support [10, 11].


## 3.2. Tensile Fracture Process of OLPM

Figure5 shows the representative tensile stress-strain curve of an OLPM sample with 70% porosity sintered at 700°C for 30 min. It can been seen from this figure that the tensile behavior of the OLPM sample can be divided into three stages: (a) initial linear elastic stage, (b) plastic deformation stage, and (c) fracture stage, which correspond to OA, AB, and BC in the curve, respectively.Figure 5
Typical tensile stress-strain curve of an oriented linear porous metal sample.The figure shows that the engineering stress increased linearly with the increasing strain in the initial stage, namely, the OA part of the plot. This process only lasts for a short time, and the elastic deformation of this sample is about 2%. The relationship between stress and strain fits well with Hooke’s law of elasticity. That is to say, in the initial elastic process, the oriented linear porous metal elongated in the tensile direction, and only a slight deformation occurs on the three-dimensional reticulation.After the elastic process, the sample reaches the plastic deformation process quickly. In this stage, deformation begins to occur in some metal fibers first, where the local stress concentration occurs, fibers reach the yield limitation first, and the plastic deformation starts here. The local plastic deformation results in stress release and redistribution, which leads to a greater plastic deformation of more fibers with tension continuously increasing. As the plastic deformation capacity of the three-dimensional reticulated skeleton is exhausted, the stress reached the ultimate tensile strength.With the fracture of the metal fiber gradually evolving into the sintering joint and the entire three-dimensional reticulated structure, the three-dimensional structure becomes prone to fracture. And the porous metal reaches the fracture stage; the engineering stress decreased sharply with the increasing strain in this stage; and this phenomenon lasts until the structure cannot undertake any load. And finally, the sample fails completely.


## 3.3. Tensile Fracture Mechanism of OLPM

To get a better understanding of the fracture of the OLPM, the facture mechanism of this new material was investigated in this study. The fracture process and the fractured samples were observed and analyzed.The fracture image of the OLPM in the thickness direction was shown in Figure6. It is clearly shown in Figure 6 that the fracture region becomes thicker and looser than any other part of the material because the fracture process first occurs in the surface of the material, where the restriction of the fibers is relatively smaller than that in the center of the material and where the deformation is larger than that in the center.Figure 6
Fracture image of the OLPM in the thickness direction.In addition, an obvious necking phenomenon is observed in the width direction along with the tensile load during the fracture process, as shown in Figure7. This figure indicates that the oriented linear porous metal is a typical plastic material. Besides that, there is no obvious fracture trace in the fracture region of the OLPM. These phenomena are quite different from our previous studies with PMFSS [21], which is also a porous material made from metal fiber. This phenomenon can be caused by the following reasons. First, the metal fibers in the OLPM are parallel to one another, and the sintering joints are also found along with the direction of the metal fiber; that is, all the metal fibers in the OLPM are almost in the same condition, and this condition is good for the material to maintain the plastic property of the metal fiber itself. Figure 8 shows the fracture morphology of metal fibers in the OLPM. It clearly shows that the metal fiber also undergoes a necking deformation under the tensile strength and maintains the original performance itself. Second, unlike the PMFSS, no fiber-to-fiber cross sintering joints and no pore structure perpendicular to the fiber direction restrict the elongation and deformation in the load direction. So the material can extend in the tensile direction. This structure is helpful to strengthen the mechanical properties and the ductility of the OLPM.Figure 7
Appearance of the fractured OLPM.Figure 8
SEM image of fractured metal fibers in OLPM.


## 3.4. Influence of Porosity

Porosity is one of the most important factors of porous metals, and it greatly influences the mechanical properties of porous metals [29, 30]. To analyze the influence of porosity on the tensile property of the OLPM, a single factor experiment was conducted. Three kinds of OLPM sintered at 800°C for 30 min with porosities of 70%, 80%, and 90% were used to investigate the effect of porosity on the tensile property.Figure9 shows the tensile stress-strain plots of the OLPM with different porosities sintered at 800°C for 30 min. The tensile strength of the OLPM decreases greatly with the increase of porosity. As shown in Figure 8, the tensile strength of the sample with 70% porosity is 16.68 MPa, whereas those of the samples with the porosities of 80% and 90% are only 10.12 MPa and 7.37 MPa, respectively. This result fits well with the result of Qiao et al. [19]. This result is mainly attributed to the following two aspects. On the one hand, the OLPM sample with lower porosity has more fibers and sintering joints in its cross-section to withstand the tensile force. Conversely, the sample with higher porosity has less fibers and contact regions to form sintering joints. On the other hand, in order to obtain high porosity, sparse fibers are distributed in the mold and low compaction force is applied, which hinder the formation of solid-sintering joints and lead to the sintering joints weaker than those of low porosity. And the stress concentration first occurs at them. These two aspects both result in low tensile strength in high porosity.Figure 9
Tensile stress-strain curves of the oriented linear porous metal with different porosities.In addition, Figure9 also illustrates that the sample with lower porosity shows a longer plastic stage. The total deformation of OLPM with 70% porosity is 20.85%, while the ductility of OLPMs with 80% and 90% porosity is 16.97% and 15.66%, respectively. That is because higher porosity means less metal fibers in the OLPM, and the faster the fracture process transfer into the three-dimensional structure of the OLPM, the smaller the deformation of the whole process.After the plastic deformation stage, the fracture rates of the samples with different porosities are not identical. The stress-strain curve of the sample with lower porosity drops more sharply, which means that the sample fractures faster.


## 3.5. Influence of Sintering Parameters

As important manufacturing parameters, sintering temperature and sintering time greatly influence the forming process of the oriented linear porous metal.


### 3.5.1. Sintering Temperature

Four samples with 70% porosity sintered at 700°C, 800°C, 900°C, and 1000°C for 30 min were selected to investigate the influence of sintering temperature on the tensile strength of the oriented linear porous metal. Figure10 shows the tensile strength plot of the OLPM samples sintered at different temperatures.Figure 10
Tensile strength of the oriented linear porous metal with different sintering temperatures.Obviously, the tensile strength of the OLPM increases with sintering temperatures between 700°C and 900°C, but it decreases at 1000°C. This mainly because the formation of sintering joints is controlled by atom diffusion, which is a random thermal motion. High sintering temperature increases the energy of copper atoms [31, 32]. On the one hand, it increases the number of activated copper atoms and the opportunity of copper fibers forming the sintering joints. On the other hand, it is beneficial for the migration of copper atoms, thus accelerating the sintering process [33]. Therefore, the number of sintering joints increases and sintering joints grow larger. These phenomena will lead to the improvement of the tensile property of the OLPM. Therefore, in the range of 700°C to 900°C, the tensile strength increases with sintering temperature. However, during the sintering process, the metal fiber undergoes a heat treatment process, the increasing sintering temperature enlarges the grain size of the copper fiber when the temperature is higher than the recrystallization temperature, and the microstructure on the surface of the metal fiber will disappear at high temperature [34]. These phenomena will all lead to the decrease of tensile property at 1000°C. This situation provides us with a guide that a reasonable sintering temperature to fulfill different requirements could be chosen.


### 3.5.2. Holding Time

The tensile property of the porous metal with the porosity of 70% sintered at 800°C for 30 min, 60 min, 90 min, and 120 min is shown in Figure11. From Figure 11, we can conclude that holding time has slight effect on the tensile property of OLPM. When the sintering time was extended from 30 min to 60 min, the tensile strength increased from 16.68 MPa to 16.92 MPa. However, the sintering time of 60 min leads to the maximum tensile strength at the sintering temperature of 800°C, and the tensile strength decreases to 16.65 MPa and 15.16 MPa when the sintering time increases to 90 min and 120 min, respectively. The difference between different holding time is 11%.Figure 11
Tensile strength of the oriented linear porous metal with different holding times.The results are caused by the following two aspects. On the one hand, sintering joints formed between fibers become larger with the increase of sintering time, leading to the improvement of the tensile properties of the porous metal. Meanwhile, the increase of sintering time caused the grain of the copper fibers to become coarse, leading to the decrease in the mechanical property of the fiber itself and then to the decrease of the tensile properties of the material. The combination of the two aspects leads to the result. In addition, the lengthening of the sintering time increases the manufacturing cost of the oriented linear porous metal. Therefore, improving the tensile strength of the porous metal by extending the sintering time is not logical.


## 3.5.1. Sintering Temperature

Four samples with 70% porosity sintered at 700°C, 800°C, 900°C, and 1000°C for 30 min were selected to investigate the influence of sintering temperature on the tensile strength of the oriented linear porous metal. Figure10 shows the tensile strength plot of the OLPM samples sintered at different temperatures.Figure 10
Tensile strength of the oriented linear porous metal with different sintering temperatures.Obviously, the tensile strength of the OLPM increases with sintering temperatures between 700°C and 900°C, but it decreases at 1000°C. This mainly because the formation of sintering joints is controlled by atom diffusion, which is a random thermal motion. High sintering temperature increases the energy of copper atoms [31, 32]. On the one hand, it increases the number of activated copper atoms and the opportunity of copper fibers forming the sintering joints. On the other hand, it is beneficial for the migration of copper atoms, thus accelerating the sintering process [33]. Therefore, the number of sintering joints increases and sintering joints grow larger. These phenomena will lead to the improvement of the tensile property of the OLPM. Therefore, in the range of 700°C to 900°C, the tensile strength increases with sintering temperature. However, during the sintering process, the metal fiber undergoes a heat treatment process, the increasing sintering temperature enlarges the grain size of the copper fiber when the temperature is higher than the recrystallization temperature, and the microstructure on the surface of the metal fiber will disappear at high temperature [34]. These phenomena will all lead to the decrease of tensile property at 1000°C. This situation provides us with a guide that a reasonable sintering temperature to fulfill different requirements could be chosen.


## 3.5.2. Holding Time

The tensile property of the porous metal with the porosity of 70% sintered at 800°C for 30 min, 60 min, 90 min, and 120 min is shown in Figure11. From Figure 11, we can conclude that holding time has slight effect on the tensile property of OLPM. When the sintering time was extended from 30 min to 60 min, the tensile strength increased from 16.68 MPa to 16.92 MPa. However, the sintering time of 60 min leads to the maximum tensile strength at the sintering temperature of 800°C, and the tensile strength decreases to 16.65 MPa and 15.16 MPa when the sintering time increases to 90 min and 120 min, respectively. The difference between different holding time is 11%.Figure 11
Tensile strength of the oriented linear porous metal with different holding times.The results are caused by the following two aspects. On the one hand, sintering joints formed between fibers become larger with the increase of sintering time, leading to the improvement of the tensile properties of the porous metal. Meanwhile, the increase of sintering time caused the grain of the copper fibers to become coarse, leading to the decrease in the mechanical property of the fiber itself and then to the decrease of the tensile properties of the material. The combination of the two aspects leads to the result. In addition, the lengthening of the sintering time increases the manufacturing cost of the oriented linear porous metal. Therefore, improving the tensile strength of the porous metal by extending the sintering time is not logical.


## 3.6. Comparing with Commercial Porous Metal and PMFSS

The tensile strength of the oriented linear porous metal was compared with the commercial porous metal and the porous metal fiber sintered sheet [21]. Figure 12 shows the tensile strengths of three kinds of materials sintered at 800°C for 30 min and 60 min with 80% porosity. The figure shows that the tensile strength of the OLPM is significantly higher than those of the other two kinds of materials. This result is because that the surface of the metal fiber in CPM is smooth, as shown in Figure 4. It is relatively difficult for the metal fiber to form sintering joints between the smooth surfaces [35], so the tensile strength is relatively lower than that of the oriented linear porous metal. The metal fibers in the PMFSS occlude one another, and not all the metal fibers can resist the tension force, so the tensile strength is significantly lower than that of the oriented linear porous metal.Figure 12
Tensile strength of three different porous metals.These results obtained provide us with an important technical guideline for different potential applications of the OLPM, especially for the conditions with the tensile loading.


## 4. Conclusion

(1) A novel oriented linear porous metal with a three-dimensional network structure was produced through the solid-state sintering method with cutting copper fibers. With a special long strip pore structure and numerous microstructures on the surface of the metal fiber, this material exhibits unique properties during the tensile fracture process. And the tensile process of the OLPM included the following three stages: the elastic stage at low strain, the plastic deformation stage, and the damage and fracture of the overall network structure.(2) The tensile strength depends heavily on the porosity. The tensile strength of the OLPM decreased rapidly with the increasing porosity, and the extent of the deformation increases with the decreasing porosity.(3) The sintering parameters also play important role in the tensile properties of the OLPM. The tensile strength increases with sintering temperature from 700°C to 900°C and then decreases at 1000°C. The extension of holding time slightly affected the tensile strength of the OLPM, and 900°C is the optimal sintering temperature of this material.(4) The tensile strength of the OLPM is much higher than the PMFSS and the CPM. The results obtained in this work provide an important technical guideline for different potential applications of the OLPM, especially for the conditions with the tensile loading.



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*Source: 3930703-2016-01-11.xml*