Home The optimization of friction disc gear-shaping process aiming at residual stress and machining deformation
Article Open Access

The optimization of friction disc gear-shaping process aiming at residual stress and machining deformation

  • Hanjun Gao , Xin Li , Qiong Wu EMAIL logo , Wanhao Zhang , Guowen Dai and Guohong Zhang
Published/Copyright: December 20, 2021
Become an author with De Gruyter Brill

Abstract

Friction disc is the key part of the frictional clutch. But there is a lack of in-depth studies on the effect of the cutting parameters on residual stress and machining deformation. In this study, the simulation model for friction disc gear shaping was established and the effect of the typical cutting parameters on surface residual stress and machining deformation was studied. Based on the study’s results, the optimization experiment of friction disc gear shaping was carried out and a method was proposed to reduce machining deformation and to improve the fatigue life. Applying the proposed method, the residual stress on the tooth bottom increased from −122.50 to −371.33 MPa, an increase of 203.13% that increases the fatigue life greatly. Meanwhile, the front and bottom face deformation of the outer ring as well as the deformation of the front and bottom tooth tip can be decreased effectively. This study can provide technical support for improving the comprehensive performance of the friction disc and transmission system.

Graphical abstract

1 Introduction

The frictional clutch transmits torque depending on the friction between the multiple friction discs within it. As core components, the friction disc plays an irreplaceable role in the process of power transmission due to its characteristic high relative speed, compact structure, and large transmission power. However, the high impact load, high temperature, and other harsh working conditions make the friction disc prone to erosion, wear, deformation, and even fracture, which significantly affect the reliability and stability of the transmission device.

The large amount of friction heat generated by the relative motion between friction discs will significantly affect the temperature and stress field of the system, which is the key factor leading to the increase of material wear rate, local burning, surface warping, hot cracking, and even failure [1]. Jen and Nemecek [2] analyzed the temperature rise caused by the relative motion between the friction disc and solved the total energy of the system. Based on the expression of the temperature and stress fields as modal expansions, Li and Barber [3] applied the fast speed expansion method to solve the transient thermo-elastic contact problem.

The surface morphology and characteristics of the material significantly affect its service life and dynamic performance, and its parameters have a strong nonlinear effect on the wear of the friction material. Zou et al. [4] studied the surface characteristics under different contact loads as well as the effects of load and sliding speed on the friction coefficient, and discussed the relationship between the surface characteristics of clutch disc materials and friction performance. Based on the contact model and sliding friction work model, Zhu et al. [5] established the wear mathematical model of the friction disc respectively, and used the model to predict the fatigue life of the friction disc. It has a certain guiding significance on the effective use of the friction disc.

The temperature rise and wear discussed above are the two most common problems in the working process of the friction disc, to which researchers attach great importance. In addition, researchers have also conducted a lot of research on the design, manufacture, and performance of the friction disc. In design, the choice of material is the first consideration. 30CrMnSiA alloy steel emerges due to its superior comprehensive mechanical and technological properties, such as the high strength, toughness, hardenability, and good fatigue resistance. In terms of structure, Ning et al. [6] proposed a variable damping design method to reduce the impact load and improve fatigue life. Some scholars studied the oil groove on the surface of the friction disc [7], which has the function of increasing the friction coefficient and heat dissipation.

Common gear machining methods include gear milling, gear hobbing, gear shaping, gear grinding, and so on refs [8,9,10,11]. Considering the applicable scope of each processing method, the structural characteristics, and machining efficiency, the gear-shaping process was selected to machine the friction disc. In the aspect of gear shaping, Datta et al. [12] calculated the instant stress value of the gear-shaping cutter at different cutting strokes under different load conditions, and analyzed the stress distribution of the cutter edge. Li et al. [13] proposed a high-efficient gear-shaping method. In this method, the cutting area of each stroke of the gear-shaping cutter is kept approximately equal by changing the circumferential feed, which can improve machining efficiency by 40%.

In terms of gear-shaping simulation, Zhu [14] proposed a new efficient machining method of gear shaping based on constant cutting force to reduce the variation range of the cutting force and to improve machining accuracy. Erkorkmaz et al. [15] proposed a new model to accurately predict the geometry shape of the chip as well as the cutting force during the gear-shaping process. Katz et al. established a comprehensive virtual model of gear shaping to study the influence of kinematics, cutter-workpiece engagement, and cutting force as well as tool deflection in gear shaping on the gear tooth profile error [16,17]. They conducted a systematic simulation study and summary on the gear-shaping process.

The machining process will inevitably produce machining deformation, and excessive machining deformation has an adverse impact on the assembly as well as the performance of parts. There are many factors influencing machining deformation, such as material properties, cutting force, cutting heat, clamping conditions, the initial residual stress, as well as machining induced residual stress. Scholars have conducted a series of research to study them, and to predict and control machining deformation [18]. The research on machining deformation control mainly covers the following aspects: machining parameter optimization, clamping layout optimization, residual stress homogenization, auxiliary support technology, numerical control compensation technology, high-speed machining, etc. [19].

Residual stress is an important factor of deformation. It is the key characterization parameter of internal quality, which directly affects fatigue strength and service life. In recent years, residual stress has attracted much attention. Huang et al. discussed the formation mechanism of residual stress, deduced the analytical model of surface stress field, analyzed the influence of tool parameters and cutting parameters on residual stress, and did a comprehensive study and summary of residual stress in the orthogonal cutting process [20,21,22]. The introduction of compressive residual stress can improve mechanical properties and prolong fatigue life. However, the formation of residual stress is an extremely complex multi field coupling process. Although some scholars have studied how to controllably introduce compressive residual stress [23], its application in engineering is not mature. Additional auxiliary processes are mostly applied to reduce residual stress, such as heat treatment [24], vibratory stress relief [25], and shot peening [26].

The mechanical, tribological, and thermal characteristics of the material significantly affect its fatigue life, and technology can be applied to improve the surface properties, such as nitriding, carburizing, boriding, coating, laser quenching, and high current pulsed electron beam [27,28,29]. Their basic principle is to improve wear resistance and fatigue life by changing the microstructure or stress state of the material surface. Besides, Nguyen et al. [30] applied the optimized non-Newtonian fluid polishing technology to machine the gear surface, which significantly reduced the concentrated stress at the tooth root, and improved the fatigue resistance of the material. In addition to the above methods, some researchers have adopted nano-additive [31] or hard anti-wear coatings to reduce the wear [32].

From the above analysis it can be seen that a large number of achievements have been made in studying the friction disc, such as the optimization of structure, the means of improving surface quality, the methods of reducing temperature rise and wear, as well as the gear-shaping process. However, the research on gear-shaping technology mostly focuses on the gear-shaping cutter, cutting force, tooth profile accuracy, kinematics, cutting efficiency, etc. The research on axial deformation and fatigue life of the friction disc is relatively inadequate, and further in-depth study is needed.

Therefore, this study establishes a numerical simulation model of the friction disc gear-shaping process, studies the influence of typical cutting parameters on surface residual stress and machining deformation, optimizes the gear-shaping parameters and carries out corresponding experiments to verify it. Finally, a gear-shaping process method is proposed to reduce machining deformation and to improve fatigue life.

2 Theory

2.1 The calculation of the cutting area

The chip shape produced through the process of gear shaping is irregular, and the cutting area and cutting force vary periodically with the change in the machining position. Therefore, an analysis of the machining path of the gear-shaping cutter and the cutting area can provide the basis for selecting gear-shaping simulation parameters.

In order to facilitate understanding and to simplify simulation, the external meshing gear-shaping cutter single tooth model is established, in which the left and right edges as well as the top edge are mainly considered. As shown in Figure 1, ( O x , y ) , ( O 1 x 1 , y 1 ) , and ( O 2 x 2 , y 2 ) are the inertial coordinate system, gear-shaping cutter coordinate system, and workpiece coordinate system, respectively. Supposing that the involute profiles on both sides of a tooth are Involute 1 and Involute 2 , and their coordinates are ( x 2 L , y 2 L ) and ( x 2 R , y 2 R ) , respectively, the involute equations of the gear can be obtained through the matrix change as follows [33]:

(1) Involute 1 : x 2 L y 2 L 1 = r b 2 cos α k sin ( tan α k α k ) r b 2 cos α k cos ( tan α k α k ) 1 ,

(2) Involute 2 : x 2 R y 2 R 1 = cos 2 π β + 2 π z 2 sin 2 π β + 2 π z 2 0 sin 2 π β + 2 π z 2 sin 2 π β + 2 π z 2 0 0 0 1 × x 2 L y 2 L 1 ,

where

(3) β = 2 tan a cos r b 2 r a 2 a cos r b 2 r a 2 + S a 2 r a 2 ,

where r b 2 is the radius of the base circle, α k is the pressure angle, z 2 is the number of teeth, and r a 2 and S a 2 are the radius and tooth thickness of the addendum circle respectively, and a is the center distance between the gear and the gear-shaping cutter.

Figure 1 
                  Coordinate system for solving the involute profile of the gear shaper cutter [33].
Figure 1

Coordinate system for solving the involute profile of the gear shaper cutter [33].

The involute tooth profile of the gear-shaping cutter is conjugate with that of the gear. Through coordinate transformation, the involute tooth profile of the gear-shaping cutter named Tool 1 and Tool 2 can be obtained, and their equations are as follows:

(4) Tool 1 = cos i θ sin i θ 0 sin i θ cos i θ 0 0 0 1 1 cos θ sin θ 0 sin θ cos θ a 0 0 1 Involute 1 ,

(5) Tool 2 = cos i θ sin i θ 0 sin i θ cos i θ 0 0 0 1 1 cos θ sin θ 0 sin θ cos θ a 0 0 1 Involute 2 ,

where i is the transmission ratio, and θ is the rotation angle of the gear.

Through the continuous contact condition, the relationship between θ and α k can be established, so that formulas (1)–(5) have the same unique variable α k , whose range is fixed and known. The curve equation of the top edge is a simple arc equation. Thus the mathematical model of the external meshing gear-shaping cutter can be accurately established. Through coordinate transformation, the model of the external gear-shaping cutter is transformed to that of the internal gear-shaping cutter. The machining process of internal gear-shaping is calculated in MATLAB, and the machining path is shown in Figure 2.

Figure 2 
                  The machining position trajectory calculation by MATLAB.
Figure 2

The machining position trajectory calculation by MATLAB.

The cutting area is the intersection of the two adjacent machining paths of the gear-shaping cutter and the workpiece blank. The obtained machining position trajectory is discretized into several points and imported into AutoCAD. The removal amount is calculated by the Boolean operation with VBA programming, and then it is equivalent to the regular rectangle. Figure 3 shows 29 groups of the area removal amount under 30 machining positions. Therefore, if the cutting thickness (width) is determined, the corresponding equivalent cutting width (thickness) could be calculated through the given cutting area.

Figure 3 
                  The cutting area under different machining positions.
Figure 3

The cutting area under different machining positions.

2.2 The calculation of the cutting force

The calculation of the cutting force F z ( N ) and cutting power P m ( kW ) in the process of gear shaping is as follows:

(6) F z = 0.475 m 2 f c z 0.09 p ,

(7) P m = F z v 1 6 × 10 4 ,

where z is the number of gear teeth, m is the module, p is the unit cutting force (see Table 1), f c is the circumferential feed rate ( mm dst 1 ) , v 1 is the cutting speed, which is related to the number of stroke N 0 , and the stroke length l of the gear-shaping cutter. The computational expression is shown in formula (8):

(8) v 1 = 2 N 0 l 1 , 000 .

Table 1

Unit cutting force in the gear-shaping process

Material Mechanical property (GPa) Unit cutting force p ( N mm 2 )
Structural steel σ b = 0.59 0.69 1 , 668 1 , 766
σ b = 0.78 0.98 3 , 139 3 , 433

2.3 The calculation of roughness

Formula (9) is the calculation expressing turning surface roughness:

(9) R a = 1 , 000 f 2 8 r ,

where R a is the surface roughness and its unit is μm ; f is the feed rate per revolution, and r is the arc radius of the tool tip.

Like the formula for the calculation of turning surface roughness, the formula for friction disc tooth root surface roughness in the gear-shaping process can be expressed in the form shown in formula (10):

(10) R a = 1 , 000 f c 2 8 r ,

where R a is the surface roughness ( μm ); f c is the circumferential feed rate in single stroke ( mm dst 1 ) ; and r is the addendum circle radius of the gear-shaping cutter ( mm ) .

3 Simulation and experiment

3.1 The simulation and experiment under original process

3.1.1 The simulation of cutting force and residual stress

3.1.1.1 Simulation environment settings

Due to the same relative motion, AdvantEdge’s two-dimensional broaching model is used to simulate the gear-shaping process under single stroke. The constitutive parameters and physical parameters of the friction disc material 30CrMnSiA are assigned to the selected Johnson-Cook model, and HSS-Co-M35 high speed steel in the material library is selected as the cutting tool material. The bottom area of the workpiece is fixed, the immersion cooling medium is used, the cutting tool and workpiece are meshing with the default mesh size, and their initial temperature field is set at 20°C.

The actual and simulation cutting parameters are shown in Table 2. In actual processing, several friction discs are clamped together for machining to increase efficiency. But in the simulation model, only the finish machining of one friction disc is solved to explore the relationship between cutting parameters and machining quality.

Table 2

Analysis of actual and simulation cutting parameters

Actual parameters Simulation parameters Explanation
The number of stroke 80 Cutting speed (m·min−1) 20 Calculated by formula (8)
The stroke length (mm) 125
Circumferential feed rate (mm·dst−1) 0.26 Cutting thickness (mm) 0.26 According to the relative movement relationship between gear shaping and broaching, the cutting thickness equals the circumferential feed rate
Radial feed rate (mm·dst−1) 0.02 Cutting width (mm) 0.91 Calculated by the maximum cutting area (0.237052 mm2)
Cutting length (mm) 5 Tooth thickness of the friction disc plus certain allowance (3.9 + 1.1)
3.1.1.2 The analysis of simulation results

The results of the cutting force, cutting temperature, strain, stress, etc. can be obtained in the post-processing. This study focuses on the analysis of the cutting force in the cutting process and the machining induced residual stress on the workpiece surface. The results of the cutting force and residual stress are shown in Figure 4, respectively. The analysis results are as follows.

Figure 4 
                        The simulation of cutting force and residual stress.
Figure 4

The simulation of cutting force and residual stress.

In the cutting process of gear shaping, the cutting force increases sharply in the beginning, then it rapidly enters the stable cutting stage, and its value tends to be steady. The average values of the main cutting force (Force-X) and feed resistance (Force-Y) are about 1471.37 and 1129.51 N, respectively. After cutting, the residual stress on the workpiece surface is compressive stress, with a value of −83 MPa. The maximum compressive stress reaches about −150 MPa at 0.02 mm from the surface. With the increase in the distance from workpiece surface, the residual stress changes to tensile stress rapidly and then gradually decreases to 0 or so at a depth of about 0.4 mm.

3.1.2 The simulation of machining deformation

In ANSYS software, the SOLID278 element is defined for the model of the friction disc and the material properties of 30CrMnSiA are assigned. The inner diameter and outer diameter of the friction disc are 363 and 428.5 mm, respectively, and its thickness is 3.9 mm. The heat treatment process of the model is simulated, and the results of stress field are read as the initial state for the cutting process. The nodes around the outer diameter of the friction disc are fully constrained to simulate the clamping conditions in the actual gear-shaping process. On this basis, the cutting force calculated by AdvantEdge software is applied to the model, and the Birth and Death Element Method is utilized to simulate the full gear-shaping process and to solve the machining deformation of the friction disc.

The following information can be obtained from the results of the deformation nephogram (Figure 5): the distribution of axial deformation is basically symmetrical after the gear-shaping process. The axial deformation value decreases gradually from the outer ring to the inner ring, from the front to the bottom. The maximum positive deformation is 0.0233 mm, which is located near the front outer edge, while the maximum negative deformation is 0.0476 mm, located at the bottom tooth tip.

Figure 5 
                     The nephogram results of machining deformation: (a) the front face and (b) the bottom face.
Figure 5

The nephogram results of machining deformation: (a) the front face and (b) the bottom face.

The reasons for the above results are as follows: during the gear-shaping process, the surface of the friction disc is clamped and fixed. The negative deformation occurs at the cutting position due to the extrusion action of the gear-shaping cutter, while the positive deformation arises near the outer edge due to the warping action. The closer to the edge, the greater the moment, and greater the deformation.

3.1.3 The verification of the simulation model

3.1.3.1 The machining and detection of friction disc

The residual stress on the friction disc blank after heat treatment was measured by X-ray diffractometer and electrochemical corrosion technology. The results showed that the values of the circumferential and radial residual stresses are very small, which can be explained by the fact that the residual stress on the friction disc after gear shaping is mainly induced by the machining process.

The YK5180BX3 CNC gear-shaping machine (located in the powder metallurgy plant of Hangzhou Qianjin Gearbox Group Co., Ltd.) was used to carry out the gear-shaping experiment on the friction disc blank using the cutting parameters in Table 2. After testing its M value to be qualified, the GLOBAL S coordinate measuring machine (located in the Jiangsu Institute of Information Technology), the SmartSite RS X-ray diffractometer (located in the Beijing Xiangbo Technology Co., Ltd.), and the MicroXAM 3D optical profiler (located in the Youerhongxin Testing Technology (Shenzhen) Co., Ltd.) were used to detect the machining deformation, residual stress, and surface roughness, respectively, and to verify the accuracy of the simulation model. Figure 6 shows the machining and detection worksite of the friction disc.

Figure 6 
                        The experimental and detection equipment: (a) the worksite of gear shaping, (b) MicroXAM 3D optical profiler, (c) the detection of residual stress, and (d) the detection of machining deformation (1, gear-shaping cutter; 2, annular pressing plate; 3, the friction disc to be machined; 4, the fixture; 5, the rotary table of the gear-shaping machine; 6, concentric stop block; 7, level indicator; 8, the friction disc to be detected; 9, RS X-ray diffractometer; 10, tiger bench clamp; 11, coordinate measuring machine; 12, the probe; 13, the friction disc to be detected; 14, workbench).
Figure 6

The experimental and detection equipment: (a) the worksite of gear shaping, (b) MicroXAM 3D optical profiler, (c) the detection of residual stress, and (d) the detection of machining deformation (1, gear-shaping cutter; 2, annular pressing plate; 3, the friction disc to be machined; 4, the fixture; 5, the rotary table of the gear-shaping machine; 6, concentric stop block; 7, level indicator; 8, the friction disc to be detected; 9, RS X-ray diffractometer; 10, tiger bench clamp; 11, coordinate measuring machine; 12, the probe; 13, the friction disc to be detected; 14, workbench).

3.1.3.2 The accuracy verification of the simulation model
3.1.3.2.1 The cutting force

The experiment demonstrated that the tensile strength of the friction disc is 1.042 GPa. According to Table 1, the unit cutting force value 3,524 ( N mm 2 ) is calculated by the linear interpolation method. The parameters of the friction disc and machining process are brought into formula (6) to obtain the cutting force:

F z = 0.475 m 2 f c z 0.09 p = 0.475 × 3 2 × 0.26 122 0.09 × 3 , 524 = 2542.08 N .

The simulation average values of Force-X and Force-Y are 1471.37 and 1129.51 N, respectively. So their resultant force is 1854.91 N. Compared to F z , the relative error is 27.03%. Since the simulation model is a simplified two-dimensional model without considering the radial force, the relative error of 27.03% is acceptable. Under this condition, the cutting power can be calculated as follows:

P m = F z v 1 6 × 10 4 = 2542.08 × 20 6 × 10 4 = 0.85 kW .

3.1.3.2.2 The machining deformation

The data and analysis of machining deformation are shown in Table 3: the average deformation errors of the outer ring and inner ring are 19 and 28% respectively. Except for the A2 inner ring, the measured and simulation values are in good agreement. In view of the good consistency of the other test data, it is considered that the reason for the larger deformation of A2 inner ring is not only the difference between material properties and ideal values, but is also related to the position of clamping during the gear-shaping process.

Table 3

The comparison between measured and simulation maximum machining deformation (unit: mm)

Group Simulation Measured Relative error (%) Average relative error
Outer ring Inner ring
A1 Outer ring 0.023 0.02 15 19% 28%
Inner ring 0.048 0.05 4
A2 Outer ring 0.023 0.03 23
Inner ring 0.048 0.10 52

In addition, the powder metallurgy layer would be bonded on the face of the friction disc after gear shaping, and then there will be a fine grinding process. So the deformation of the outer ring that happened during gear shaping will be compensated in the follow-up process.

3.1.3.2.3 The residual stress

The simulation results of Figure 4 show that the surface residual stress is −83 MPa, and the average residual stress measured by the X-ray diffractometer is −110.5 MPa, as is shown in Table 4, with a relative error of 24.89% compared to the simulation value.

Table 4

The comparison and analysis of the measured and simulation residual stress (unit: MPa)

Group Measured value Average value Simulation value Relative error
A1 −91.6 −110.5 −83 24.89%
A2 −129.5
3.1.3.2.4 The roughness

Figure 7 and Table 5 are the detection and analysis results of roughness. It can be seen that the machined surface has a certain fluctuation in the circumferential direction, while the consistency in the axial direction is very good. The measured average roughness is 1.712  μm . Bring f c and r into formula (10), and the theoretical value of the tooth bottom surface roughness is calculated as follows:

R a = 1 , 000 f c 2 8 r = 1 , 000 × 0.13 2 8 × 1 = 2.11 μm .

Figure 7 
                           The surface profile image of roughness detection.
Figure 7

The surface profile image of roughness detection.

Table 5

The comparison and analysis of roughness (unit: μm)

Group R a Average value Theoretical value Relative error
A1-1 1.905 1.712 2.11 18.86%
A1-2 1.627
A1-3 1.779
A2-1 1.522
A2-2 1.876
A2-3 1.596

The relative error between the theoretical value and simulation value is 18.86%, which indicates that this formula has high accuracy and is suitable for the calculation of tooth bottom roughness.

To sum up, the established finite element model is reliable and can be further utilized for process optimization analysis.

3.2 Process optimization

3.2.1 Optimizing parameters to improve residual stress

The cutting parameters of the gear-shaping process include the stroke number, stroke length, circumferential feed rate, radial feed rate, etc. The stroke number can characterize the cutting speed due to the usually invariant stroke length. In the actual gear-shaping process, the workpiece is fixed on the workbench for circumferential feed movement. After the gear-shaping cutter moves to the required position along the radial direction according to the set radial feed rate, it maintains its own rotation movement and axial cutting movement. The radial feed rate determines the distance of each radial feed. Therefore, the parameters of cutting speed and circumferential feed rate are the two factors that have a greater impact on the forming performance.

In AdvantEdge, the effect of cutting speed on residual stress is studied by changing the value of the cutting speed keeping the other parameters unchanged. Figure 8 demonstrates the results. With the increase in cutting speed, the maximum tensile stress first slightly decreases and then increases slowly, while the maximum compressive stress presents a very slowly decreasing trend. The cutting speed has little effect on the residual stress and 20–25 m·min−1 is a better choice. The stroke number range is 80–100 with the stroke distance of 125 mm remaining unchanged.

Figure 8 
                     The effect of cutting speed and circumferential feed rate on residual stress.
Figure 8

The effect of cutting speed and circumferential feed rate on residual stress.

The circumferential feed rate is set as the parameter of cutting thickness in the finite element simulation. According to the reference manual, the circumferential feed rate is usually 0.2–0.5 mm·dst−1. The cutting thickness is changed to study the effect of the circumferential feed rate on residual stress. As is shown in Figure 8: with the increase in the circumferential feed rate, the stress values of the surface and subsurface decrease first and then increase. Among the five levels studied, the stress state is the most ideal when the circumferential feed rate is 0.30 mm·dst−1. Taking into account the levels not studied, its value can be taken in the range of 0.25–0.35 mm·dst−1 during machining.

3.2.2 Adding circular gasket to reduce machining deformation

Different cutting parameters lead to different cutting forces and different degrees of machining deformation. Based on the parametric model, the cutting force is adjusted to study its influence on the machining deformation of friction disc in ANSYS software. The simulation result is shown in Figure 9: with the increase in cutting force, the maximum positive deformation gradually decreases, while the maximum negative deformation increases gradually, and the difference value is almost unchanged. That is to say, it is not feasible to reduce machining deformation by changing the cutting force. It is necessary to find other ways to reduce deformation.

Figure 9 
                     The influence of cutting force on machining deformation.
Figure 9

The influence of cutting force on machining deformation.

In the transmission system of mechanical equipment, a layer of high temperature resistant metallurgical powder is plated on the upper and lower surfaces of the friction disc to increase the friction coefficient and improve transmission efficiency. Therefore, there is a certain gap between the different friction discs in the gear-shaping process, resulting in the position to be machined suspended and forming a cantilever structure. Consequently, a circular gasket can be designed and placed in the gap to increase the rigidity of the friction disc and reduce machining deformation.

As shown in Figure 10, its thickness is slightly higher than twice the thickness of the metallurgical layer, so that it comes into close contact with the upper and lower friction discs, and its outer diameter is slightly smaller than the inner diameter of the metallurgical layer to achieve the clearance fit. The simulation results demonstrate that the axial maximum negative deformation of the friction disc’s inner ring bottom face before and after adding the circular gasket decreases from 0.0195 to 0.00383 mm, that is, a reduction of 80.36%. The axial deformations of the other gear-shaping parts are also reduced by about 60%. Therefore, adding the circular gasket can significantly reduce machining deformation during the gear-shaping process.

Figure 10 
                     The position of the circular gasket in the gear-shaping process.
Figure 10

The position of the circular gasket in the gear-shaping process.

3.2.3 Experimental verification of optimization effect

Based on previous research, gear-shaping experiments were carried out to optimize the cutting speed and circumferential feed rate. The setting of experimental cutting parameters is shown in Table 6. The cutting parameters in groups B3 and B4 are the same and there is a circular gasket between the bottom of B3 and the front of B4 to verify its inhibition effect on machining deformation. After the gear-shaping process, the machining deformation and residual stress of each friction disc are tested to verify the optimization effect. The experimental equipment is the same as the one used in Section 3.1.3 to ensure consistency of the other data as much as possible.

Table 6

The design scheme of the optimization experiment

Group N 0 f c Gasket or not Explanation
B1 80 0.26 No The original process
B2 80 0.30 No Change the circumferential feed rate compared to B1
B3 100 0.30 Yes Change the cutting speed compared to B1, and verify the effect of the gasket
B4 No

4 Results and discussion

4.1 Machining deformation

Figure 11 and Table 7 show the results of the analysis of machining deformation data detected by the coordinate measuring machine:

  1. Compared to B1, the front and bottom face deformation of B2 outer ring decreased by 0.0279 mm (38.38%) and 0.0102 mm (19.62%), respectively, and the deformation of the front and bottom tooth tip increased by 0.005 mm (5.52%) and decreased by 0.0168 (14.18%), respectively. Although the deformation of the front tooth tip increased slightly, in general, the deformation of the B2 friction disc is significantly reduced when compared with the original process.

  2. Compared with B1 and B2, the deformation of the friction discs in group B3 and B4 are significantly increased, which indicates that increasing the cutting speed will have an adverse effect. At the same time, it is worth noting that the deformation of the bottom tooth tip in group B3 and the front face deformation of B4 outer ring is reduced by 21.19 and 10.31%, respectively. And when compared with B3, the front face deformation of the B4 outer ring is reduced by 5.3%, which indicates that the existence of the circular gasket can significantly reduce machining deformation.

Figure 11 
                  The analysis of the friction disc machining deformation.
Figure 11

The analysis of the friction disc machining deformation.

Table 7

The detection data and analysis of the friction disc machining deformation (mm)

Group Outer ring Inner ring
Front face Relative error (%) Bottom face Relative error (%) Front face Relative error (%) Bottom face Relative error (%)
B1 0.0727 0 0.052 0 0.0906 0 0.1185 0
B2 0.0448 −38.38 0.0418 −19.62 0.0956 5.52 0.1017 −14.18
B3 0.0773 6.33 0.0874 68.08 0.1012 11.70 0.0934 −21.19
B4 0.0652 −10.31 0.0947 82.12 0.0964 6.40 0.3297 178.28

From the experimental results, it can be seen that in the selected cutting parameters, increasing the number of strokes will increase machining deformation, increasing the circumferential feed rate will reduce machining deformation, and adding the circular gasket can significantly reduce machining deformation. This is consistent with the previous simulation results.

In addition, the bottom face of the inner ring deformation of B4 is significantly larger than the other deformation, which may be caused by other unexpected reasons, such as insufficient heat treatment resulting in its small stiffness. However, from the overall experimental results, this value does not affect the above analysis on the influence of the law of cutting parameters on machining deformation.

4.2 Residual stress

Table 8 shows the detection results of residual stress: the stress value under original process is about −122.50 MPa. Compared to B1, the surface compressive stress of group B2 increases to −371.33 MPa, an increase of 203.13%. The stress values of B3 and B4 are −150.5 and −170 MPa, respectively, which are both improved to some extent. However, the improvement in group B2 is the most significant.

Table 8

The residual stress data of friction disc (unit: MPa)

Group The residual stress Average value Relative error (%)
B1 −128 ± 27 −122.50 0
−117 ± 24
B2 −313 ± 31 −371.33 203.13
−471 ± 49
−330 ± 70
B3 −141 ± 21 −150.5 22.86
−160 ± 44
B4 −179 ± 46 −170 38.78
−161 ± 30

The experimental result is consistent with the simulation results in Section 3.2.1. Therefore, selecting the parameters of the circumferential feed rate with 0.30 mm·dst−1 and maintaining other parameters at their original values are most effective in improving the residual stress on the machined surface.

4.3 The simulation of fatigue life

In order to efficiently study the influence of residual stress on fatigue life, the loading condition of the friction disc is simplified, and normal pressure is applied to the tooth profile surface to solve the stress field under this pressure, and then the FE-SAFE software is applied to solve the fatigue life under the load.

First, complete the basic settings and read the result file calculated by ANSYS software. Second, the properties of 30CrMnSiA material are given to the friction disc. Then, set the periodically varying load, set different surface stress, select the stress correction algorithm, and let the other settings remain at default values. Finally, submit the calculation to solve the fatigue life.

Table 9 shows the values of fatigue life calculated under different surface stresses, and the curve in Figure 12 shows the relationship between logarithmic fatigue life and surface stress. Some results can be analyzed as follows:

  1. The logarithmic fatigue life of the friction disc is basically negatively correlated with the surface stress, and the fatigue life decreases rapidly with the decrease in surface compressive stress.

  2. Under the original process, the fatigue life of friction disc is 7.82 × 104. When the compressive stress increases to −330 MPa, the fatigue life increases to 5.22 × 105, an improvement of 567.76%. When the compressive stress reaches −350 Mpa, the fatigue life is high enough and the software has been thinking that it has no damage.

  3. Under the cutting process of group B2, the compressive stress of the tooth bottom is as high as −371 MPa. Compared to the original process, the optimized process can remarkably improve the fatigue life of the friction disc.

Table 9

The fatigue life under different residual stress

Residual stress (MPa) Fatigue life Logarithmic fatigue life
−350 Unlimited life Unlimited life
−330 522,170 5.717811917
−320 480,167 5.681392309
−300 405,201 5.607670508
−250 261,813 5.417991207
−200 165,996 5.220097623
−150 103,097 5.013246028
−122 78,197 4.893190092
−100 62,602 4.796588208
−50 37,081 4.569151438
0 21,370 4.329804522
50 11,946 4.07722251
100 6,454 3.809828961
Figure 12 
                  The curve of the logarithmic fatigue life versus the surface residual stress.
Figure 12

The curve of the logarithmic fatigue life versus the surface residual stress.

The compressive stress distributed in a certain depth can partially offset the tensile stress produced by the alternating external load, and has a closure effect on microcracks to prevent its propagation. So it can significantly improve fatigue life.

There are still some shortcomings in this study that has to be improved. For example, the fatigue failure of the friction disc is a very complex process because the magnitude and position of the fatigue load are always changing. Simplifying the load as a constant value on the tooth profile could reflect the effect of the surface residual stress on fatigue life, but the results of the fatigue life are not very accurate. Therefore, the calculation method of fatigue life can be further studied in future studies.

5 Conclusion

In this study, the simulation model of the friction disc gear shaping is established and verified by the theoretical analysis and experimental detection of machining deformation, residual stress, and surface roughness. Then, based on the verified simulation model, the influence of the process parameters on machining introduced residual stress, the influence of the cutting force on machining deformation, as well as the inhibitory effect of the circular gasket on machining deformation are studied. Finally, a process optimization scheme of reducing machining deformation, increasing residual compressive stress, and improving fatigue life is summarized. The conclusions are as follows:

  1. During the selected parameter range in the optimization experiment, the machining deformation can be reduced by reducing the number of strokes, increasing the circumferential feed rate, or by placing a circular gasket in the gap between adjacent friction discs.

  2. According to the experimental results, the process parameter in group B2 is the best. Compared to the original process, the machining deformation decreases and the residual compressive stress on the tooth bottom surface increases significantly.

  3. The logarithmic fatigue life of the friction disc is basically negatively correlated with the surface stress. Compared to the original process, the optimized process of group B2 can remarkably improve the fatigue life of the friction disc.

  4. A set of methods are summarized to reduce machining deformation and to improve the fatigue life of the friction disc, that is, placing a circular gasket in the gap between the different friction discs, and applying the cutting parameters of the circumferential feed rate with 0.30 mm·dst−1 and stroke number with 80. The other parameters are the same as in the original process.

Acknowledgment

We acknowledge financial supports from the Aeronautical Science Foundation of China (2019ZE051002), National Defense Basic Scientific Research program of China (JCKY2018601C002, JCKY2019601C003, JCKY2020601C004), SAST Foundation (SAST2020-095), and the China Academy of Lanch Vehicle Technology Foundation (CALT2020-TS09).

  1. Funding information: The study was financially supported by the Aeronautical Science Foundation of China (2019ZE051002), the National Defense Basic Scientific Research program of China (JCKY2018601C002, JCKY2019601C003, JCKY2020601C004), the SAST Foundation (SAST2020-095), and the China Academy of Lanch Vehicle Technology Foundation (CALT2020-TS09).

  2. Authors contribution: Qiong Wu: Conceptualizetion; Hanjun Gao: methodology, simulation, review and editing; Xin Li: experiment, original draft and formal analysis; Wanhao Zhang: investigation; Guowen Dai: validation; Guohong Zhang: resources.

  3. Conflict of interest: We declare that we have no conflict of interest.

  4. Data availability statement: The data used to support the findings of this study are available from the corresponding author upon request.

References

[1] Abdullah, O. I. and J. Schlattmann . Thermal behavior of friction clutch disc based on uniform pressure and uniform wear assumptions. Friction, Vol. 4, No. 3, 2016, pp. 228–237.10.1007/s40544-016-0120-zSearch in Google Scholar

[2] Jen, T. C. and D. J. Nemecek . Thermal analysis of a wet-disk clutch subjected to a constant energy engagement. International Journal of Heat & Mass Transfer, Vol. 51, No. 7–8, 2008, pp. 1757–1769.10.1016/j.ijheatmasstransfer.2007.07.009Search in Google Scholar

[3] Li, J. and J. R. Barber . Solution of transient thermoelastic contact problems by the fast speed expansion method. Wear, Vol. 265, No. 3–4, 2008, pp. 402–410.10.1016/j.wear.2007.11.010Search in Google Scholar

[4] Zou, Q. , C. Rao , G. Barber , B. Zhou , and Y. C. Wang . Investigation of surface characteristics and tribological behavior of clutch plate materials. Wear, July 10–12, 2017, Journal of Physics Conference Series, Vol. 842, 012070.10.1016/j.wear.2012.10.024Search in Google Scholar

[5] Zhu, M. Y. , X. T. Liu , F. C. Kan , and Z. Y. You . Life cycle prediction and evaluation of clutch friction plate considering wear models and thermal stress. Journal of Tribology-Transactions of the Asme, Vol. 143, No. 4, 2021, id. 9.10.1115/1.4048383Search in Google Scholar

[6] Ning, K. Y. , Y. Wang , D. C. Huang , and L. Yin . Impacting load control of floating supported friction plate and its experimental verification. 12th International Conference on Damage Assessment of Structures, Journal of Physics Conference Series, Vol. 842, 2017. id. 012070.10.1088/1742-6596/842/1/012070Search in Google Scholar

[7] Jia, Y. H. Research on friction disk’s surface temperature distribution and oil groove configuration in wet friction clutch. Applied Mechanics & Materials, Vol. 148–149, 2007, pp. 1218–1222.10.4028/www.scientific.net/AMM.148-149.1218Search in Google Scholar

[8] Dong, X. , C. Liao , Y. C. Shin , and H. H. Zhang . Machinability improvement of gear hobbing via process simulation and tool wear predictions. International Journal of Advanced Manufacturing Technology, Vol. 86, No. 9–12, 2016, pp. 2771–2779.10.1007/s00170-016-8400-3Search in Google Scholar

[9] Karpuschewski, B. , H. J. Knoche , and M. Hipke. Gear finishing by abrasive processes. Cirp Annals-Manufacturing Technology, Vol. 57, No. 2, 2008, pp. 621–640.10.1016/j.cirp.2008.09.002Search in Google Scholar

[10] Bouzakis, K. D. , E. Lili , N. Michailidis , and O. Friderikos. Manufacturing of cylindrical gears by generating cutting processes: A critical synthesis of analysis methods. Cirp Annals-Manufacturing Technology, Vol. 57, No. 2, 2008, pp. 676–696.10.1016/j.cirp.2008.09.001Search in Google Scholar

[11] Svahn, M. , C. Andersson , and L. Vedmar . Prediction and experimental verification of the cutting forces in gear form milling. International Journal of Advanced Manufacturing Technology, Vol. 82, No. 1–4, 2016, pp. 111–121.10.1007/s00170-015-7309-6Search in Google Scholar

[12] Datta, P. P. , T. K. Chattopadhyay , and R. N. Banerjee . Computer aided stress analysis of Fellow’s gear-shaping cutter at different stages of a cutting stroke. Proceedings of the Institution of Mechanical Engineers Part B-Journal of Engineering Manufacture, Vol. 218, No. 10, 2004, pp. 1297–1306.10.1243/0954405042323432Search in Google Scholar

[13] Li, L. , L. Zhang , B. Yu , K. Wang , and F. Liu. An efficient spur gear shaping method based on homogenizing cutting area through variational circular feed rate. Proceedings of the Institution of Mechanical Engineers Part B-Journal of Engineering Manufacture, Vol. 231, No. 9, 2017, pp. 1587–1598.10.1177/0954405415601639Search in Google Scholar

[14] Zhu, H. Study on machining technology of gear shaping with constant cutting force, Master’s thesis, Hubei University of Technology, 2019 (In Chinese).Search in Google Scholar

[15] Erkorkmaz, K. , A. Katz , Y. Hosseinkhani , D. Plakhotnik , M. Stautner , and F. Ismail. Chip geometry and cutting forces in gear shaping. Cirp Annals-Manufacturing Technology, Vol. 65, No. 1, 2016, pp. 133–136.10.1016/j.cirp.2016.04.040Search in Google Scholar

[16] Katz, A. , K. Erkorkmaz , and F. Ismail . Virtual model of gear shaping-Part I: Kinematics, cutter-workpiece engagement, and cutting forces. Journal of Manufacturing Science and Engineering-Transactions of the Asme, Vol. 140, No. 7, 2018. id. 071007 10.1115/1.4039646Search in Google Scholar

[17] Katz, A. , K. Erkorkmaz , and F. Ismail . Virtual model of gear shaping-Part II: Elastic deformations and virtual gear metrology. Journal of Manufacturing Science and Engineering-Transactions of the Asme, Vol. 140, No. 7, 2018, id. 071008.10.1115/1.4039651Search in Google Scholar

[18] Wang, L. and H. Si. Machining deformation prediction of thin-walled workpieces in five-axis flank milling. The International Journal of Advanced Manufacturing Technology, Vol. 97, No. 9, 2018, pp. 4179–4193.10.1007/s00170-018-2248-7Search in Google Scholar

[19] Yue, C. , J. Zhang , X. Liu , Z. Chen , S. Y. Liang , and L. Wang. Research Progress on machining deformation of thin-walled parts in milling process. Acta Aeronautica et Astronautica Sinica, Vol. 42, 2021, pp. 1–27. (In Chinese).Search in Google Scholar

[20] Huang, K. and W. Yang . Analytical analysis of the mechanism of effects of machining parameter and tool parameter on residual stress based on multivariable decoupling method. International Journal of Mechanical Sciences, Vol. 128, 2017, pp. 659–679.10.1016/j.ijmecsci.2017.05.031Search in Google Scholar

[21] Huang, K. and W. Yang . Analytical modeling of residual stress formation in workpiece material due to cutting. International Journal of Mechanical Sciences, Vol. 114, 2016, pp. 21–34.10.1016/j.ijmecsci.2016.04.018Search in Google Scholar

[22] Huang, K. , W. Yang , and Q. Chen . Analytical model of stress field in workpiece machined surface layer in orthogonal cutting. International Journal of Mechanical Sciences, Vol. 103, 2015, pp. 127–140.10.1016/j.ijmecsci.2015.08.020Search in Google Scholar

[23] Zhang, Y. , W. H. Wang , and A. L. Greer. Making metallic glasses plastic by control of residual stress. Nature Materials, Vol. 5, No. 11, 2006, pp. 857–860.10.1038/nmat1758Search in Google Scholar PubMed

[24] Nakonieczny, D. S. , A. Sambok , M. Antonowicz , M. Basiaga , Z. K. Paszenda , C. Krawczyk , et al. Ageing of zirconia dedicated to dental prostheses for bruxers part 2: influence of heat treatment for surface morphology, phase composition and mechanical properties. Reviews on Advanced Materials Science, Vol. 58, No. 1, 2019, pp. 218–225.10.1515/rams-2019-0027Search in Google Scholar

[25] Gao, H. , Y. Zhang , Q. Wu , and J. Song . Experimental investigation on the fatigue life of Ti-6Al-4V treated by vibratory stress relief. Metals, Vol. 7, No. 5, 2017, pp. 62–67.10.3390/met7050158Search in Google Scholar

[26] Zhang, J. , W. Li , H. Wang , Q. Song , L. Lu , W. Wang , et al. A comparison of the effects of traditional shot peening and micro-shot peening on the scuffing resistance of carburized and quenched gear steel. Wear, Vol. 368, 2016, pp. 253–257.10.1016/j.wear.2016.09.029Search in Google Scholar

[27] Yan, M. F. , Y. X. Wang , X. T. Chen , L. X. Guo , C. S. Zhang , Y. You , et al. Laser quenching of plasma nitrided 30CrMnSiA steel. Materials & Design, Vol. 58, 2014, pp. 154–160.10.1016/j.matdes.2014.01.052Search in Google Scholar

[28] Sugianto, A. , M. Narazaki , M. Kogawara , A. Shirayori , S. Y. Kim , and S. Kubota . Numerical simulation and experimental verification of carburizing-quenching process of SCr420H steel helical gear. Journal of Materials Processing Tech, Vol. 209, No. 7, 2009, pp. 3597–3609.10.1016/j.jmatprotec.2008.08.017Search in Google Scholar

[29] Ochoa, E. A. , D. Wisnivesky , T. Minea , M. Ganciu , and F. Alvarez. Microstructure and properties of the compound layer obtained by pulsed plasma nitriding in steel gears. Surface and Coatings Technology, Vol. 203, No. 10–11, 2009, pp. 1457–1461.10.1016/j.surfcoat.2008.11.025Search in Google Scholar

[30] Nguyen, D. , D. ThanhPhong , C. Prakash , S. Singh , A. Pramanik , G. Krolczyk , et al. Machining parameter optimization in shear thickening polishing of gear surfaces. Journal of Materials Research and Technology-Jmr&T, Vol. 9, No. 3, 2020, pp. 5112–5126.10.1016/j.jmrt.2020.03.028Search in Google Scholar

[31] Wu, H. , J. Zhao , W. Xia , X. Cheng , A. He , J. H. Yun , et al. A study of the tribological behaviour of TiO2 nano-additive water-based lubricants. Tribology International, Vol. 109, 2017, pp. 398–408.10.1016/j.triboint.2017.01.013Search in Google Scholar

[32] Lepicka, M. and M. Gradzka-Dahlke . The initial evaluation of performance of hard anti-wear coatings deposited on metallic substrates: thickness, mechanical properties and adhesion measurements – A brief review. Reviews on Advanced Materials Science, Vol. 58, No. 1, 2019, pp. 50–65.10.1515/rams-2019-0003Search in Google Scholar

[33] Yu, B. Research on variable circumference feed high efficiency gear shaping machining method of large gear shaping machine based on equal cutting area, Master’s thesis, TianJin University, 2012 (In Chinese).Search in Google Scholar

Received: 2021-07-27
Revised: 2021-09-08
Accepted: 2021-09-09
Published Online: 2021-12-20

© 2021 Hanjun Gao et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Review Articles
  2. A review on filler materials for brazing of carbon-carbon composites
  3. Nanotechnology-based materials as emerging trends for dental applications
  4. A review on allotropes of carbon and natural filler-reinforced thermomechanical properties of upgraded epoxy hybrid composite
  5. High-temperature tribological properties of diamond-like carbon films: A review
  6. A review of current physical techniques for dispersion of cellulose nanomaterials in polymer matrices
  7. Review on structural damage rehabilitation and performance assessment of asphalt pavements
  8. Recent development in graphene-reinforced aluminium matrix composite: A review
  9. Mechanical behaviour of precast prestressed reinforced concrete beam–column joints in elevated station platforms subjected to vertical cyclic loading
  10. Effect of polythiophene thickness on hybrid sensor sensitivity
  11. Investigation on the relationship between CT numbers and marble failure under different confining pressures
  12. Finite element analysis on the bond behavior of steel bar in salt–frost-damaged recycled coarse aggregate concrete
  13. From passive to active sorting in microfluidics: A review
  14. Research Articles
  15. Revealing grain coarsening and detwinning in bimodal Cu under tension
  16. Mesoporous silica nanoparticles functionalized with folic acid for targeted release Cis-Pt to glioblastoma cells
  17. Magnetic behavior of Fe-doped of multicomponent bismuth niobate pyrochlore
  18. Study of surfaces, produced with the use of granite and titanium, for applications with solar thermal collectors
  19. Magnetic moment centers in titanium dioxide photocatalysts loaded on reduced graphene oxide flakes
  20. Mechanical model and contact properties of double row slewing ball bearing for wind turbine
  21. Sandwich panel with in-plane honeycombs in different Poisson's ratio under low to medium impact loads
  22. Effects of load types and critical molar ratios on strength properties and geopolymerization mechanism
  23. Nanoparticles in enhancing microwave imaging and microwave Hyperthermia effect for liver cancer treatment
  24. FEM micromechanical modeling of nanocomposites with carbon nanotubes
  25. Effect of fiber breakage position on the mechanical performance of unidirectional carbon fiber/epoxy composites
  26. Removal of cadmium and lead from aqueous solutions using iron phosphate-modified pollen microspheres as adsorbents
  27. Load identification and fatigue evaluation via wind-induced attitude decoupling of railway catenary
  28. Residual compression property and response of honeycomb sandwich structures subjected to single and repeated quasi-static indentation
  29. Experimental and modeling investigations of the behaviors of syntactic foam sandwich panels with lattice webs under crushing loads
  30. Effect of storage time and temperature on dissolved state of cellulose in TBAH-based solvents and mechanical property of regenerated films
  31. Thermal analysis of postcured aramid fiber/epoxy composites
  32. The energy absorption behavior of novel composite sandwich structures reinforced with trapezoidal latticed webs
  33. Experimental study on square hollow stainless steel tube trusses with three joint types and different brace widths under vertical loads
  34. Thermally stimulated artificial muscles: Bio-inspired approach to reduce thermal deformation of ball screws based on inner-embedded CFRP
  35. Abnormal structure and properties of copper–silver bar billet by cold casting
  36. Dynamic characteristics of tailings dam with geotextile tubes under seismic load
  37. Study on impact resistance of composite rocket launcher
  38. Effects of TVSR process on the dimensional stability and residual stress of 7075 aluminum alloy parts
  39. Dynamics of a rotating hollow FGM beam in the temperature field
  40. Development and characterization of bioglass incorporated plasma electrolytic oxidation layer on titanium substrate for biomedical application
  41. Effect of laser-assisted ultrasonic vibration dressing parameters of a cubic boron nitride grinding wheel on grinding force, surface quality, and particle morphology
  42. Vibration characteristics analysis of composite floating rafts for marine structure based on modal superposition theory
  43. Trajectory planning of the nursing robot based on the center of gravity for aluminum alloy structure
  44. Effect of scan speed on grain and microstructural morphology for laser additive manufacturing of 304 stainless steel
  45. Influence of coupling effects on analytical solutions of functionally graded (FG) spherical shells of revolution
  46. Improving the precision of micro-EDM for blind holes in titanium alloy by fixed reference axial compensation
  47. Electrolytic production and characterization of nickel–rhenium alloy coatings
  48. DC magnetization of titania supported on reduced graphene oxide flakes
  49. Analytical bond behavior of cold drawn SMA crimped fibers considering embedded length and fiber wave depth
  50. Structural and hydrogen storage characterization of nanocrystalline magnesium synthesized by ECAP and catalyzed by different nanotube additives
  51. Mechanical property of octahedron Ti6Al4V fabricated by selective laser melting
  52. Physical analysis of TiO2 and bentonite nanocomposite as adsorbent materials
  53. The optimization of friction disc gear-shaping process aiming at residual stress and machining deformation
  54. Optimization of EI961 steel spheroidization process for subsequent use in additive manufacturing: Effect of plasma treatment on the properties of EI961 powder
  55. Effect of ultrasonic field on the microstructure and mechanical properties of sand-casting AlSi7Mg0.3 alloy
  56. Influence of different material parameters on nonlinear vibration of the cylindrical skeleton supported prestressed fabric composite membrane
  57. Investigations of polyamide nano-composites containing bentonite and organo-modified clays: Mechanical, thermal, structural and processing performances
  58. Conductive thermoplastic vulcanizates based on carbon black-filled bromo-isobutylene-isoprene rubber (BIIR)/polypropylene (PP)
  59. Effect of bonding time on the microstructure and mechanical properties of graphite/Cu-bonded joints
  60. Study on underwater vibro-acoustic characteristics of carbon/glass hybrid composite laminates
  61. A numerical study on the low-velocity impact behavior of the Twaron® fabric subjected to oblique impact
  62. Erratum
  63. Erratum to “Effect of PVA fiber on mechanical properties of fly ash-based geopolymer concrete”
  64. Topical Issue on Advances in Infrastructure or Construction Materials – Recycled Materials, Wood, and Concrete
  65. Structural performance of textile reinforced concrete sandwich panels under axial and transverse load
  66. An overview of bond behavior of recycled coarse aggregate concrete with steel bar
  67. Development of an innovative composite sandwich matting with GFRP facesheets and wood core
  68. Relationship between percolation mechanism and pore characteristics of recycled permeable bricks based on X-ray computed tomography
  69. Feasibility study of cement-stabilized materials using 100% mixed recycled aggregates from perspectives of mechanical properties and microstructure
  70. Effect of PVA fiber on mechanical properties of fly ash-based geopolymer concrete
  71. Research on nano-concrete-filled steel tubular columns with end plates after lateral impact
  72. Dynamic analysis of multilayer-reinforced concrete frame structures based on NewMark-β method
  73. Experimental study on mechanical properties and microstructures of steel fiber-reinforced fly ash-metakaolin geopolymer-recycled concrete
  74. Fractal characteristic of recycled aggregate and its influence on physical property of recycled aggregate concrete
  75. Properties of wood-based composites manufactured from densified beech wood in viscoelastic and plastic region of the force-deflection diagram (FDD)
  76. Durability of geopolymers and geopolymer concretes: A review
  77. Research progress on mechanical properties of geopolymer recycled aggregate concrete
Downloaded on 10.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/rams-2021-0069/html?lang=en
Scroll to top button