Abstract
In view of the problem of large earthquake displacement in the use of the original concrete engineering shear wall reinforcement method, the energy dissipation and damping structure is used to design the energy dissipation and damping structure reinforcement method in the concrete engineering shear wall. According to the design process of the set method, the anti-vibration coefficient of the concrete shear wall is tested. The energy dissipation structure is used to construct a shear damping wall, and the damper is added to the original shear wall. The concrete shear wall is strengthened by sticking steel technology. So far, the design of shear wall reinforcement method based on the energy dissipation structure has been completed. Compared with the original method, the displacement distance of this method is lower than that of the original method. In conclusion, the effect of shear wall reinforcement method based on the energy dissipation structure is better than that of the original method.
1 Introduction
With the development of social economy, the use performance and function of some existing houses have changed, increasing the overall load on the existing houses. Some of the existing houses have increased the use area at the parts with larger storey height or the roof, or arranged at the concave and convex parts of the ground to meet the energy saving requirements [1]. Even some buildings cannot meet the existing load bearing capacity, they need to be strengthened. Affected by the earthquake, local training buildings need to be strengthened in a small area. Therefore, the renovation and reinforcement of existing houses are increasing day by day. According to the development of the situation, architectural structural designers should be able to skillfully engage in the structural design of new buildings, and gradually be familiar with and master the transformation and reinforcement design of existing buildings [2]. With the rapid development of economy, the acceleration of urbanization, and the prosperity of construction industry, a large number of buildings have been built to meet the needs of people’s increasing material living standards. During this period, the number of buildings not only showed a blowout growth, but also constantly enriched and innovated in form and structure. However, with the passage of time, in these buildings gradually appear component aging, strength reduction, and other problems in the use stage, which have a great impact on the service performance of the structure, and the seismic capacity is significantly reduced [3]. According to statistics, at present, the urban housing area in China has exceeded 5 billion square meters, and more than half of them have been put into use for more than 40 years, which shows that the housing aging problem in China has become prominent [4]. In addition, due to improper design, construction defects, changes in the use of buildings, natural disasters, long-term acid, alkali, salt erosion or weathering, freeze–thaw cycle, and other reasons, the reliability of the structure will also be reduced, which cannot meet the requirements of seismic fortification, leaving a potential safety hazard. If these buildings are demolished and rebuilt, they will not only waste human, material, and financial resources, cause resource waste and environmental pollution, but also bring great inconvenience to people’s life and urban traffic. In view of this phenomenon, strengthening the building shear wall has become the first choice to improve the service life of concrete engineering.
Reference [5] puts forward the principle of distance interaction between particles in building mechanics. In the process of concrete engineering shear wall reinforcement, the relative function of shear wall balance is analyzed. Through the study of the thermodynamics of shear wall structure, the reinforcement of concrete engineering shear wall is completed, but the overall effect of this method still needs to be further strengthened. Reference [6] puts forward the limit evaluation method of high-strength concrete beam column reinforcement design. This method carries out experimental research on 12 high-strength concrete buildings, analyzes the different application degrees of the total amount of longitudinal reinforcement and concrete strength, respectively, and obtains the accurate limit evaluation method of beam column reinforcement, but the cost of this method is high and the overall efficiency is low. In reference [7], the shear force of reinforced concrete wall is designed. Under the condition of minimum shear reinforcement ratio, the yield strength of shear reinforcement is limited to 420 MPa. In order to clarify the influence of shear strength and minimum reinforcement ratio of reinforced concrete shear wall under different reinforcement conditions, a cyclic lateral load test is carried out under different reinforcement conditions to complete the shear design of reinforced concrete. However, the whole process of this method is complex and its applicability needs to be further improved.
Reinforced concrete shear wall is a kind of structural component which mainly bears the vertical and horizontal loads caused by wind or earthquake. It has good lateral stiffness and seismic performance, so it is also called seismic wall or wind wall. In the frame structure system, the problem of exposed beam and exposed column often occurs, and the shear wall can avoid this problem, make the internal space of the building more open and beautiful, and improve the space utilization rate, so that the shear wall can be widely used in multi-storey or high-rise buildings [8]. Shear wall is divided into four types: solid wall, small opening wall, joint wall, and wall frame. It is used to realize the seismic function of concrete buildings. Compared with the seismic strengthening of existing buildings, the seismic design of new buildings is simple and direct. On the basis of a large number of studies on the seismic performance of building materials and structure details, the current building structure design code puts forward many strict methods and regulations for the design of new buildings according to the expected building functions. In the design of new buildings, engineers can select reasonable, economic, and effective structural forms according to the requirements of the use of buildings, so that the seismic performance of new buildings can be easily controlled [9].
2 Materials and methods
In view of the existing concrete engineering shear wall reinforcement method in use, the seismic capacity is poor. The energy dissipation structure is used to improve the shortcomings of the original method. Energy dissipation is used to install energy dissipators (dampers) in the structure, artificially increase the structural damping, consume the vibration energy of the structure under the earthquake, reduce the vibration response of the structure, and achieve the purpose of earthquake resistance of the structure. The design mechanism of a concrete engineering shear wall reinforcement method is as follows [10].
Generally speaking, the seismic reinforcement of existing buildings includes: the restoration of buildings after disasters, including earthquakes and fires; and the reinforcement of existing buildings. By adopting reinforcement measures, the original state of the building can be effectively restored, the seismic performance of the building can be improved, and the seismic response of the building can be reduced. The shear wall reinforcement of concrete engineering mainly includes: repairing the damaged parts, improving the stiffness distribution of the building, strengthening the existing structure, setting the damping device, setting the vibration isolation device, and reducing the self-weight of the building. In this method design, the energy dissipation structure will be used to strengthen the seismic coefficient of the shear wall (Figure 1).

Design framework of the shear wall reinforcement method for concrete engineering based on the energy dissipation structure.
2.1 Detection of anti-vibration coefficient of the concrete shear wall
In this design, in order to ensure the effectiveness and pertinence of the reinforcement part, the anti-vibration coefficient of the concrete shear wall is first tested. The seismic evaluation of shear wall is a direct method to test the current use of shear wall, determine the feasibility of shear wall transformation scheme, and plan for the future use of the building. The existing seismic appraisal of a reinforced concrete structure needs to detect multiple seismic factors of the structure. The comprehensive seismic capacity analysis of the test results leads to the appraisal conclusions, including: the rationality of the overall layout of the structure, the concrete strength test, the mechanical properties of the reinforcement and the corrosion degree test, the component connection test, the component seismic bearing capacity test, etc. According to the current standard “standard for seismic evaluation of buildings” [11], the general steps for seismic evaluation of existing buildings are to check the original data of buildings, such as the calculation sheet of architectural design drawings and the completion acceptance documents. If the data are not complete, the buildings to be evaluated shall be surveyed on site. It is necessary to check whether the existing service conditions of the building are consistent with the design documents, the construction quality of the site survey, and the maintenance of the building, and find out the defects of the building in terms of earthquake resistance. According to the characteristics of the structural type of the building, the on-site inspection shall be carried out for the material strength, component reinforcement, and structural layout of the building. According to the test results and seismic bearing capacity analysis, the seismic evaluation report has to be made. If the appraised building conforms to the requirements of the standard for seismic evaluation of buildings, the subsequent service life of the building shall be stated and the handling method shall be proposed for the non-conformities. At present, there are many common methods to determine the anti-vibration coefficient of a shear wall. In order to ensure the feasibility of this design method, the method of comparing the advantages and disadvantages of the measurement method will be used to obtain the form suitable for concrete shear wall [12].
Through the above comparison results, in this design, the ultrasonic-rebound method is used to complete the wall anti-vibration test. In the process of reinforcement, the rebound instrument is used to deal with the shear wall in the project according to the above set detection steps. In order to effectively control the data in the detection and ensure its accuracy and operability, a special rebound instrument is selected to complete the work in this detection. The specific model of a rebound instrument is shown below (Figure 2).

Model and appearance of a rebound tester selected in the paper.
The anti-vibration coefficient of shear wall is tested by the above instrument. The evaluation of anti-vibration coefficient of existing buildings is based on the evaluation of anti-vibration measures and the calculation of anti-vibration bearing capacity. The identification of anti-vibration measures includes the arrangement of anti-lateral force members, abrupt change of stiffness distribution, identification of structural system, and strength detection of structural materials [13]. When the anti-vibration intensity is more than six degrees, it is necessary to check the anti-vibration bearing capacity, and at least check the anti-vibration bearing capacity in two directions of the main shaft. It is known that the strength of concrete is proportional to the elastic modulus when the type and proportion of concrete aggregate are fixed, while the propagation speed of wave in the medium is related to the elastic modulus and density, as shown in the following formula.
In the above formula,
The ultrasonic method is used to measure the propagation time of the wave in the concrete medium by the method of sending and receiving two probes, then calculate its velocity, and determine the concrete strength by the numerical curve. The specific calculation process is as follows [14].
In the above formula, E
C is the dynamic modulus of elasticity,
In the above formula,
In the above formula, V is the average value of ultrasonic wave, l measurement distance, and
2.2 Construction of a shear damping wall with energy dissipation structure
In this method design, the damper is used to complete the design of energy dissipation and damping structure of concrete buildings. According to the characteristics of concrete, dampers are selected to realize the energy dissipation and damping performance of shear walls. In order to ensure the effectiveness of reinforcement, a viscous damper is selected to complete the design. The viscous damper can be divided into fluid resistance type (hydraulic cylinder type) and shear resistance type according to the different damping methods of viscous materials. The shear resistance type can also be divided into (three-way) tubular viscous damper and viscous damping wall, as shown in the figure below (Figure 3) [15].

Classification of viscous dampers.
According to the above classification, the viscous damping wall is selected as the design basis of the energy dissipation and damping structure. Viscous fluid damper is mainly composed of steel, damping materials, and sealing materials. Due to the rustproof treatment of steel and the chemical stability of sealing materials, the durability of a viscous fluid damper depends on the durability of damping materials. A damping material is not easy to age, and there is almost no change during normal use: under the action of cyclic stress, the characteristics of a damping material do not change, and its fatigue resistance is good; a damping material is extremely stable for ozone and ultraviolet, and its weather resistance is good; a damping material does not undergo change when it is immersed in water, and its water resistance is excellent. Through the installation of dampers in shear wall joints, the energy dissipation and damping performance of shear wall is strengthened. The damper models selected in this paper are as follows (Figure 4).

Viscous damper.
The above dampers are used for energy dissipation and vibration reduction of shear walls. The location optimization of dampers is an important problem in energy dissipation design. Its purpose is to use the least number of dampers to make the structural system achieve the corresponding damping objectives or even a better damping effect. Therefore, the selection of optimization objectives becomes particularly important. At present, the common objective control functions are mainly the maximum interfloor displacement angle, floor lateral displacement, absolute acceleration, and their weighted combination of the structure. According to the characteristics of viscoelastic dampers, there are five kinds of damper optimization design methods with different objective control functions: Taking interlayer displacement as control function; taking control force as control function; taking interlayer displacement and floor lateral displacement as control function; taking interlayer displacement and top floor displacement as control function; and taking vibration mode as control function. According to the relevant characteristics of concrete shear wall, in this design, interlayer displacement and top floor displacement are selected as the control function in the design scheme of the damper. According to the given different damping, the optimal damping is the optimal configuration when the optimal control effect is obtained; through genetic algorithm, the optimal damping is sought to reduce the total damping when the seismic performance of the structure is basically the same. Based on the theory of structural control, the optimal position with the control force as the objective is studied from the two criteria of “safety” and “comfort”. It is concluded that the optimal position is at the maximum displacement of the first mode when the variance of the control force and the variance of the structural response are the minimum.
According to the measured anti-vibration coefficient of shear wall, the damping coefficient of damper is set and applied to the reinforcement of shear wall. In this design, the Maxwell model is used to set the damping coefficient of damping wall [16], which is a more accurate mechanical calculation model expressed by the continuity of pure damping element and damper’s own stiffness. In this model, the damper has a strong dependence on the frequency. In this model, if we define the damper’s own stiffness as a spring element, and its damping model can be made up of a pure damping element and a spring element in series, then the damping coefficient can be obtained through the data changes before and after the deformation of the pure damping element and the spring element. If the displacements of damping element [17] and spring element are
The integration of the above two formulas is as follows:
In the above formula,
If the above two formulas are combined, they are:
Through the calculation of the above formula, the energy storage coefficient and energy dissipation coefficient of the shear wall after the damper is installed can be obtained. The formula can be expressed as follows [18]:
Considering the damper–damping relationship, there are:
Combining the above with the damper energy dissipation coefficient
The damping parameters of the damper used in the shear wall are controlled by the above formula and applied to the concrete shear wall.
2.3 Strengthening of the concrete shear wall
Compared with the traditional structural strengthening technology, this design uses the buckling brace reinforcement technology to install the buckling brace in the wall. The technology cannot damage the use function of the original structure, does not affect the size of the structure space, and is easy to maintain. Compared with the traditional reinforcement technology, the repair work after a major earthquake is more simple and recyclable. Buckling restrained brace is a new seismic method developed in recent decades. The essence of the anti-seismic technology of buckling brace is to set the buckling brace between the structural members. When an earthquake occurs, the buckling brace members yield before the main structure, which plays the role of energy dissipation and shock absorption, and can effectively reduce the damage of the main structure caused by the earthquake. As a result, the technology of buckling proof brace has become the main direction of building reinforcement. In this project, it is difficult to ensure the safety of the structure under a strong earthquake. The structure with buckling proof support has a great energy consumption capacity due to the buckling proof support. According to the domestic and foreign engineering examples, the cost of a buckling proof support technology can be reduced by about 5–10% compared with the traditional reinforcement technology [19]. As it shows good economy, the project has adopted the buckling support technology for reinforcement. The setting of a buckling brace used in this design is as follows (Figure 5).

Design drawing of a buckling proof supporting apparatus.
In order to make the reinforcement part play a better role and put into use more quickly, the selection of reinforcement materials is also very important. In order to reduce the size and material use, high-strength steel can be used. Considering the bonding of the combination surface of reinforcement and the integrity of the reinforcement components, when selecting materials to make concrete, the raw materials with high strength, small shrinkage, and good bonding with the original components are used. In addition to adding dampers and buckling brace devices, the shear wall is strengthened by sticking steel. The load-carrying capacity of the members is enhanced by sticking the 2–6 mm thick steel sheet on the surface of the concrete structure with a certain adhesive strength [20]. The construction process of this reinforcement method is simple and generally used to strengthen the flexural and tensile members. The structural adhesive used has strict shear and tensile strength, which can combine the strength of steel plate and concrete as a whole to resist the load. The shear wall structure after sticking steel is as follows (Figure 6).

Results of shear wall reinforcement with steel. (a) Design results of sticking steel method. (b) Wall structure after pasting steel.
The glued steel plate and the coated structural adhesive are exposed to the air. If the anti-corrosion and maintenance measures are not carried out in time, the bearing capacity of the steel plate will be greatly reduced, and the structural adhesive will lose its adhesion. It is necessary to set the protective measures as general application of waterproof materials and apply 15–20 mm M15 cement mortar to complete the reinforcement process [21,22]. Combining the above settings with the energy dissipation structure, the design of a shear wall reinforcement method based on the energy dissipation structure is completed.
3 Simulation experiment
In order to verify the effect of the method in this paper, the simulation experiment is conducted to obtain the results of the comparison between the original method and the design method in this paper. Many laws in the field of engineering are often dug out from some specific and special phenomena: first, from the phenomenon, through the corresponding logical deduction and theoretical analysis, to form a certain theoretical basis, then often use the finite element and other numerical simulation methods to verify the relevant laws, while further verification often needs to be carried out through the design of relevant tests, and then get more practical results. The design of this experiment is to further verify and study the influence of regularity of the design method in this paper.
3.1 Experimental preparation
Considering that the viscous damper used in this paper is a velocity-dependent damper, and its normal working frequency is usually between 1 and 3 HZ, it is not allowed to use any general simulation experimental equipment or conduct any static test. It is better to use the dynamic loading test with a dynamic control system. Therefore, the simulation seismic vibration table is selected to add the seismic wave and sine wave to the concrete experimental sample. For the load test, the basic parameters of the vibration table are shown in the table below (Tables 1–3).
Comparison of several methods for the determination of anti-vibration coefficient of concrete shear wall
Method | Scope of use | Content determination | Advantage | Shortcoming |
---|---|---|---|---|
Rebound | Compressive strength and homogeneity | Determine the hardness value of the position surface | The method is simple and easy to operate | The measuring position can only be on the surface of the test piece with low accuracy |
Ultrasonic-rebound | Compressive strength | Determine the hardness value of the position surface and the propagation speed of the sound wave in the concrete | The method is simple, easy to operate, and has high precision | Complex operation |
Core | Compressive strength, internal defects | Pressure resistance of core sample drilling | High precision | Damage to walls, repair required |
Pull-out | Compressive strength | Pull-out force | High precision | The equipment is bulky, causing damage to the wall, which needs to be repaired |
Parameters of experimental simulation platform
Item number | Project | Basic parameters |
---|---|---|
1 | Platform size | 5 m × 5 m |
2 | Maximum load capacity | 20 T |
3 | Direction of vibration | Two-way three degrees of freedom |
4 | Vibration waveform | Various regular waves, random waves, and simulated seismic waves |
5 | Peak acceleration | 0.2 g |
6 | Peak velocity | 1,000 mm/s |
7 | Displacement peak value | 150 mm |
8 | Maximum frequency | 0.2 Hz |
9 | Minimum frequency | 150 Hz |
Setting of concrete strength of an experimental specimen
Strength grade | C30 | C35 | C40 | C45 | C50 |
---|---|---|---|---|---|
Water–binder ratio | 0.65 | 0.60 | 0.55 | 0.51 | 0.45 |
Cement | 170 | 185 | 190 | 220 | 270 |
Mineral powder | 66 | 68 | 72 | 80 | 100 |
Powdered carbon ash | 28 | 32 | 34 | 35 | 40 |
Water | 180 | 175 | 170 | 165 | 165 |
Sand | 891 | 863 | 820 | 745 | 637 |
Stone | 1,100 | 1,115 | 1,120 | 1,134 | 1,160 |
Water reducing agent | 1.2 | 1.35 | 1.55 | 2.15 | 1.75 |
By using the above platform as the basic platform of this simulation experiment, through setting the relevant experimental instruments to connect with the platform, we need to complete the component work of the complete experimental platform. In this experiment, the effect of earthquake on the shear wall of a concrete structure is simulated by an electronic tensile instrument, and the instruments used in the experiment are as follows (Figure 7).

Electronic universal testing machine.
By using the above-mentioned instruments, the simulation experiments are carried out on the experimental specimens after the original reinforcement method and the design reinforcement method in this paper, and the seismic effects of the experimental specimens after the original method and the design method in this paper are compared.
3.2 Experimental specimen design
For the purpose of this experiment, the corresponding concrete shear wall model is made. The size and reinforcement of the test piece are determined according to the requirements of the “code for design of concrete structure reinforcement” and the “code for design of concrete structure,” combined with the conditions of test equipment in the simulation laboratory. The model test piece is composed of a base beam, wall, and loading beam. The height from the top of loading beam to the bottom of foundation beam is 1,500 mm. The height of loading beam is 200 mm, the height of base beam is 400 mm, the height of wall is 900 mm, the section length of wall limb is 800 mm, the thickness of unreinforced wall is 70 mm, and the total thickness of reinforced wall is 140 mm. The specific section size and reinforcement parameters of a shear wall model are as follows (Figure 8).

Experimental sample design results.
According to the above parameters as the design basis of the experimental samples, in order to ensure the uniformity of the experimental process, the concrete and steel bars used in the experiment are set to complete the design process of the shear wall on the basis of a certain proportion. The production processes are: steel processing, strain gauge pasting, steel binding, skeleton production, formwork installation, concrete pouring, specimen maintenance, reinforcement treatment, and reinforcement specimen maintenance. Each construction procedure shall be carried out in strict accordance with the code for construction of concrete structures (GB50666-2011), so as to ensure the quality of test pieces. The concrete proportions are as follows.
Due to the limited experimental conditions, in the process of the experiment, C35 concrete strength material is used as the basic part of the experimental sample, and the proportion set above is used to complete the production of the experimental sample. In this experiment, the number of simulated earthquake intensity experiments is set to 30, and the intensity of each earthquake increases by 5% compared with the previous experiment. The displacements of the experimental specimen after using the design method and the original structure method are compared.
The parameters of seismic simulation are designed as follows: the shear wall load is 2.5 kn/m2, the seismic grade of shear wall is grade 8, the peak value of basic seismic acceleration is 0.2 g, and the characteristic period is 0.45 s.
3.3 Analysis of experimental results
According to the above test settings, the displacement data of the strengthened test pieces are obtained from the structural laboratory, and the comparison results between the proposed method and the reference [5] method are shown in Table 4.
Displacement data of specimens strengthened by the proposed method and the traditional method
Number of experiments | Displacement data of reference [5] method/mm | Whether there is damage (Y/N) | The design method in this paper deals with the post displacement data/mm | Whether there is damage (Y/N) |
---|---|---|---|---|
1 | 3.2 | N | 2 | N |
2 | 4 | N | 1.1 | N |
3 | 2.3 | N | 1.3 | N |
4 | 3.5 | N | 1.4 | N |
5 | 2.6 | N | 1.1 | N |
6 | 2.7 | N | 1.7 | N |
7 | 3.6 | N | 1.9 | N |
8 | 2 | N | 1.7 | N |
9 | 3.2 | N | 1.3 | N |
10 | 2.3 | N | 1.3 | N |
11 | 3.4 | N | 1.2 | N |
12 | 2.7 | N | 1.1 | N |
13 | 2.5 | N | 1.1 | N |
14 | 2.9 | N | 1.5 | N |
15 | 4 | N | 1 | N |
16 | 3.9 | N | 1.5 | N |
17 | 3.2 | N | 1.7 | N |
18 | 4 | N | 1.1 | N |
19 | 2.3 | N | 1.2 | N |
20 | — | T | 1.9 | N |
21 | — | T | 1.2 | N |
22 | — | T | 1 | N |
23 | — | T | 2 | N |
24 | — | T | 1 | N |
25 | — | T | 2 | N |
26 | — | T | 1.1 | N |
27 | — | T | 1.3 | N |
28 | — | T | 1.4 | N |
29 | — | T | — | T |
30 | — | T | — | T |
According to the above test data, the reinforcement effect of the proposed method is obviously better than that of the reference [5]. In the above table, the displacement data of the specimen strengthened by the two methods will be reflected in detail. The data show that the floor shear force of the structure with damping is significantly smaller than that before use; when the damper is set in the middle, the displacement value is significantly smaller than the displacement distance of the reference [5] method. The displacement difference between the reference [5] method and the proposed method is obvious. When the seismic simulation level is the same, the displacement distance of the designed method is shorter than that of the reference [5]. At the same time, in the test process of reference [5], the crack appeared earlier, the crack developed faster, the width was larger, and the penetration was earlier. But because the energy dissipation structure can effectively restrain the development of the original wall concrete inclined cracks and avoid the premature fracture of the concrete inclined cracks, the development trend of the cracks in the test pieces designed in this paper is obviously slowed down, and the number and width of the concrete damage are reduced, which shows that the reinforcement method of energy dissipation structure shear wall can improve the seismic performance of the shear wall to a certain extent. This paper slows down the development speed of time cracks after reinforcement according to the design method and reduces the number and width of main cracks. The results show that the damper reinforcement can restrain the development of cracks, and the ductility of the wall is larger than that of the single reinforcement. Most of the cracks in shear wall specimens start from the two sides of the wall and develop into inclined cracks, which are basically concentrated in the middle and lower part of the wall, and the concrete is crushed at the bottom. According to the development process and failure characteristics of the cracks in the test pieces, it is suggested to take corresponding structural measures for the middle and lower part of the wall in the process of reinforcement. In conclusion, this design method is superior to the reference [5] design method.
4 Conclusions
In order to improve the safety of concrete buildings, this paper studies the important problems of energy dissipation and damping structure in the application of concrete shear wall reinforcement through theoretical analysis, numerical simulation, shaking table test of earthquake simulation, and engineering examples. The following conclusions are proved by theory and experiment. This method shows high accuracy in the analysis of concrete shear wall reinforcement. First, the influence of shear wall on building safety is analyzed in detail and then the reinforcement method of shear wall is designed. The experimental results show that, compared with the traditional method, the energy dissipation structure can effectively inhibit the development of the original wall concrete diagonal cracks and avoid the premature fracture of the concrete diagonal cracks. In future research, the design method will be improved to ensure an advanced and reasonable method.
References
[1] Ashraf T, Ranaiefar M, Khatri S, Kavosi J, Gardea F, Glaz B, et al. Carbon nanotubes within polymer matrix can synergistically enhance mechanical energy dissipation. Nanotechnology. 2018;29(11):115704.10.1088/1361-6528/aaa7e6Search in Google Scholar PubMed
[2] Krymsky GF. Energy dissipation in a medium with turbulent viscosity and the hill vortex. Doklady Phys. 2019;64(6):269–70.10.1134/S1028335819060065Search in Google Scholar
[3] Rashahmadi S, Meguid SA. Modeling size-dependent thermoelastic energy dissipation of graphene nanoresonators using nonlocal elasticity theory. Acta Mech. 2019;230(3):771–85.10.1007/s00707-018-2281-5Search in Google Scholar
[4] Bauer A, Wegt S, Bopp M, Jakirlic S, Tropea C, Krafft AJ, et al. Comparison of wall shear stress estimates obtained by laser Doppler velocimetry, magnetic resonance imaging and numerical simulations. Exp Fluids. 2019;60(7):1–16.10.1007/s00348-019-2758-6Search in Google Scholar
[5] Frommer F, Hanke M, Jansen S. A note on the uniqueness result for the inverse Henderson problem. J Math Phys. 2019;60(9):093303.10.1063/1.5112137Search in Google Scholar
[6] Aguilar G, Villamizar S, Ramirez. JA. Evaluation of shear reinforcement design limits in high-strength concrete beams. Aci Struct J. 2018;115(2):401–14.10.14359/51701132Search in Google Scholar
[7] Baek J-W, Park H-G, Choi K-K, Seo M, Chung L. Minimum shear reinforcement of slender walls with grade 500 MPa (72.5 ksi) reinforcing bars. Aci Struct J. 2018;115(3):225–31.10.14359/51701281Search in Google Scholar
[8] Bellizzi S, Chung K-W, Sampaio R. Response regimes of a linear oscillator with a nonlinear energy sink involving an active damper with delay. Nonlinear Dyn. 2019;97(2):1667–84.10.1007/s11071-019-05089-0Search in Google Scholar
[9] Vikash P, Prasad P, Dhrubaditya M. Clustering and energy spectra in two-dimensional dusty gas turbulence. Phys Rev E. 2019;100(1):013114.10.1103/PhysRevE.100.013114Search in Google Scholar PubMed
[10] Sessa S, Marmo F, Vaiana N, Rosati L. Probabilistic assessment of axial force–biaxial bending capacity domains of reinforced concrete sections. Meccanica. 2019;54(9):1451–69.10.1007/s11012-019-00979-4Search in Google Scholar
[11] Claudia L, Burdick Jason A. Engineering stem and stromal cell therapies for musculoskeletal tissue repair. Cell Stem Cell. 2018;22(3):325–39.10.1016/j.stem.2018.01.014Search in Google Scholar PubMed PubMed Central
[12] Baleanu D, Fernandez A, Akgül A. On a fractional operator combining proportional and classical differintegrals. Mathematics. 2020;8(3):360.10.3390/math8030360Search in Google Scholar
[13] Patra A, Saha Ray S. Analysis for fin efficiency with temperature-dependent thermal conductivity of fractional order energy balance equation using HPST method. Alex Eng J. 2016;55(1):77–85.10.1016/j.aej.2016.01.009Search in Google Scholar
[14] Takahisa M, Kentarou M, Ryota K, Otsuki K, Yuhao J, Fujisawa R, et al. Arousal from tonic immobility by vibration stimulus. Behav Genetics. 2019;49(5):478–83.10.1007/s10519-019-09962-xSearch in Google Scholar PubMed
[15] Pakoksung K, Suppasri A, Imamura F, Athanasius C, Omang A, Muhari A. Simulation of the submarine landslide tsunami on 28 september 2018 in Palu Bay, Sulawesi Island, Indonesia, using a two-layer model. Pure Appl Geophys. 2019;176(8):3323–50.10.1007/s00024-019-02235-ySearch in Google Scholar
[16] Han YC. Case study of slope deterioration characteristics: simbal landslide, Salt Range, Pakistan. Environ Earth Sci. 2019;78(10):1–9.10.1007/s12665-019-8272-6Search in Google Scholar
[17] Belyaev Aleksey V. Long ligands reinforce biological adhesion under shear flow. Phys Rev E. 2018;97(4-1):042407.10.1103/PhysRevE.97.042407Search in Google Scholar PubMed
[18] Al Kaissi A, Chehida FB, Grill F, Ganger R, Kircher SG. Turning the backbone into an ankylosed concrete-like structure: case report. Medicine. 2018;97(15):e0278.10.1097/MD.0000000000010278Search in Google Scholar PubMed PubMed Central
[19] Akyildiz FT, Vajravelu K. Galerkin-Chebyshev pseudo spectral method and a split step new approach for a class of two dimensional semi-linear parabolic equations of second order. Appl Math Nonlinear Sci. 2018;3:255–64.10.21042/AMNS.2018.1.00019Search in Google Scholar
[20] Devaki P, Sreenadh S, Vajravelu K, Prasad KV, Vaidya H. Wall properties and slip consequences on peristaltic transport of a casson liquid in a flexible channel with heat transfer. Appl Math Nonlinear Sci. 2018;3:277–90.10.21042/AMNS.2018.1.00021Search in Google Scholar
[21] Khalique CM, Mhlanga IE. Travelling waves and conservation laws of a (2 + 1)-dimensional coupling system with Korteweg-de Vries equation. Appl Math Nonlinear Sci. 2018;3:241–54.10.21042/AMNS.2018.1.00018Search in Google Scholar
[22] Lokesha V, Shruti R, Deepika T. Reckoning of the dissimilar topological indices of human liver. Appl Math Nonlinear Sci. 2018;3:265–76.10.21042/AMNS.2018.1.00020Search in Google Scholar
© 2020 Shujuan Yang, published by De Gruyter
This work is licensed under the Creative Commons Attribution 4.0 International License.
Articles in the same Issue
- Regular Articles
- Model of electric charge distribution in the trap of a close-contact TENG system
- Dynamics of Online Collective Attention as Hawkes Self-exciting Process
- Enhanced Entanglement in Hybrid Cavity Mediated by a Two-way Coupled Quantum Dot
- The nonlinear integro-differential Ito dynamical equation via three modified mathematical methods and its analytical solutions
- Diagnostic model of low visibility events based on C4.5 algorithm
- Electronic temperature characteristics of laser-induced Fe plasma in fruits
- Comparative study of heat transfer enhancement on liquid-vapor separation plate condenser
- Characterization of the effects of a plasma injector driven by AC dielectric barrier discharge on ethylene-air diffusion flame structure
- Impact of double-diffusive convection and motile gyrotactic microorganisms on magnetohydrodynamics bioconvection tangent hyperbolic nanofluid
- Dependence of the crossover zone on the regularization method in the two-flavor Nambu–Jona-Lasinio model
- Novel numerical analysis for nonlinear advection–reaction–diffusion systems
- Heuristic decision of planned shop visit products based on similar reasoning method: From the perspective of organizational quality-specific immune
- Two-dimensional flow field distribution characteristics of flocking drainage pipes in tunnel
- Dynamic triaxial constitutive model for rock subjected to initial stress
- Automatic target recognition method for multitemporal remote sensing image
- Gaussons: optical solitons with log-law nonlinearity by Laplace–Adomian decomposition method
- Adaptive magnetic suspension anti-rolling device based on frequency modulation
- Dynamic response characteristics of 93W alloy with a spherical structure
- The heuristic model of energy propagation in free space, based on the detection of a current induced in a conductor inside a continuously covered conducting enclosure by an external radio frequency source
- Microchannel filter for air purification
- An explicit representation for the axisymmetric solutions of the free Maxwell equations
- Floquet analysis of linear dynamic RLC circuits
- Subpixel matching method for remote sensing image of ground features based on geographic information
- K-band luminosity–density relation at fixed parameters or for different galaxy families
- Effect of forward expansion angle on film cooling characteristics of shaped holes
- Analysis of the overvoltage cooperative control strategy for the small hydropower distribution network
- Stable walking of biped robot based on center of mass trajectory control
- Modeling and simulation of dynamic recrystallization behavior for Q890 steel plate based on plane strain compression tests
- Edge effect of multi-degree-of-freedom oscillatory actuator driven by vector control
- The effect of guide vane type on performance of multistage energy recovery hydraulic turbine (MERHT)
- Development of a generic framework for lumped parameter modeling
- Optimal control for generating excited state expansion in ring potential
- The phase inversion mechanism of the pH-sensitive reversible invert emulsion from w/o to o/w
- 3D bending simulation and mechanical properties of the OLED bending area
- Resonance overvoltage control algorithms in long cable frequency conversion drive based on discrete mathematics
- The measure of irregularities of nanosheets
- The predicted load balancing algorithm based on the dynamic exponential smoothing
- Influence of different seismic motion input modes on the performance of isolated structures with different seismic measures
- A comparative study of cohesive zone models for predicting delamination fracture behaviors of arterial wall
- Analysis on dynamic feature of cross arm light weighting for photovoltaic panel cleaning device in power station based on power correlation
- Some probability effects in the classical context
- Thermosoluted Marangoni convective flow towards a permeable Riga surface
- Simultaneous measurement of ionizing radiation and heart rate using a smartphone camera
- On the relations between some well-known methods and the projective Riccati equations
- Application of energy dissipation and damping structure in the reinforcement of shear wall in concrete engineering
- On-line detection algorithm of ore grade change in grinding grading system
- Testing algorithm for heat transfer performance of nanofluid-filled heat pipe based on neural network
- New optical solitons of conformable resonant nonlinear Schrödinger’s equation
- Numerical investigations of a new singular second-order nonlinear coupled functional Lane–Emden model
- Circularly symmetric algorithm for UWB RF signal receiving channel based on noise cancellation
- CH4 dissociation on the Pd/Cu(111) surface alloy: A DFT study
- On some novel exact solutions to the time fractional (2 + 1) dimensional Konopelchenko–Dubrovsky system arising in physical science
- An optimal system of group-invariant solutions and conserved quantities of a nonlinear fifth-order integrable equation
- Mining reasonable distance of horizontal concave slope based on variable scale chaotic algorithms
- Mathematical models for information classification and recognition of multi-target optical remote sensing images
- Hopkinson rod test results and constitutive description of TRIP780 steel resistance spot welding material
- Computational exploration for radiative flow of Sutterby nanofluid with variable temperature-dependent thermal conductivity and diffusion coefficient
- Analytical solution of one-dimensional Pennes’ bioheat equation
- MHD squeezed Darcy–Forchheimer nanofluid flow between two h–distance apart horizontal plates
- Analysis of irregularity measures of zigzag, rhombic, and honeycomb benzenoid systems
- A clustering algorithm based on nonuniform partition for WSNs
- An extension of Gronwall inequality in the theory of bodies with voids
- Rheological properties of oil–water Pickering emulsion stabilized by Fe3O4 solid nanoparticles
- Review Article
- Sine Topp-Leone-G family of distributions: Theory and applications
- Review of research, development and application of photovoltaic/thermal water systems
- Special Issue on Fundamental Physics of Thermal Transports and Energy Conversions
- Numerical analysis of sulfur dioxide absorption in water droplets
- Special Issue on Transport phenomena and thermal analysis in micro/nano-scale structure surfaces - Part I
- Random pore structure and REV scale flow analysis of engine particulate filter based on LBM
- Prediction of capillary suction in porous media based on micro-CT technology and B–C model
- Energy equilibrium analysis in the effervescent atomization
- Experimental investigation on steam/nitrogen condensation characteristics inside horizontal enhanced condensation channels
- Experimental analysis and ANN prediction on performances of finned oval-tube heat exchanger under different air inlet angles with limited experimental data
- Investigation on thermal-hydraulic performance prediction of a new parallel-flow shell and tube heat exchanger with different surrogate models
- Comparative study of the thermal performance of four different parallel flow shell and tube heat exchangers with different performance indicators
- Optimization of SCR inflow uniformity based on CFD simulation
- Kinetics and thermodynamics of SO2 adsorption on metal-loaded multiwalled carbon nanotubes
- Effect of the inner-surface baffles on the tangential acoustic mode in the cylindrical combustor
- Special Issue on Future challenges of advanced computational modeling on nonlinear physical phenomena - Part I
- Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications
- Some new extensions for fractional integral operator having exponential in the kernel and their applications in physical systems
- Exact optical solitons of the perturbed nonlinear Schrödinger–Hirota equation with Kerr law nonlinearity in nonlinear fiber optics
- Analytical mathematical schemes: Circular rod grounded via transverse Poisson’s effect and extensive wave propagation on the surface of water
- Closed-form wave structures of the space-time fractional Hirota–Satsuma coupled KdV equation with nonlinear physical phenomena
- Some misinterpretations and lack of understanding in differential operators with no singular kernels
- Stable solutions to the nonlinear RLC transmission line equation and the Sinh–Poisson equation arising in mathematical physics
- Calculation of focal values for first-order non-autonomous equation with algebraic and trigonometric coefficients
- Influence of interfacial electrokinetic on MHD radiative nanofluid flow in a permeable microchannel with Brownian motion and thermophoresis effects
- Standard routine techniques of modeling of tick-borne encephalitis
- Fractional residual power series method for the analytical and approximate studies of fractional physical phenomena
- Exact solutions of space–time fractional KdV–MKdV equation and Konopelchenko–Dubrovsky equation
- Approximate analytical fractional view of convection–diffusion equations
- Heat and mass transport investigation in radiative and chemically reacting fluid over a differentially heated surface and internal heating
- On solitary wave solutions of a peptide group system with higher order saturable nonlinearity
- Extension of optimal homotopy asymptotic method with use of Daftardar–Jeffery polynomials to Hirota–Satsuma coupled system of Korteweg–de Vries equations
- Unsteady nano-bioconvective channel flow with effect of nth order chemical reaction
- On the flow of MHD generalized maxwell fluid via porous rectangular duct
- Study on the applications of two analytical methods for the construction of traveling wave solutions of the modified equal width equation
- Numerical solution of two-term time-fractional PDE models arising in mathematical physics using local meshless method
- A powerful numerical technique for treating twelfth-order boundary value problems
- Fundamental solutions for the long–short-wave interaction system
- Role of fractal-fractional operators in modeling of rubella epidemic with optimized orders
- Exact solutions of the Laplace fractional boundary value problems via natural decomposition method
- Special Issue on 19th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering
- Joint use of eddy current imaging and fuzzy similarities to assess the integrity of steel plates
- Uncertainty quantification in the design of wireless power transfer systems
- Influence of unequal stator tooth width on the performance of outer-rotor permanent magnet machines
- New elements within finite element modeling of magnetostriction phenomenon in BLDC motor
- Evaluation of localized heat transfer coefficient for induction heating apparatus by thermal fluid analysis based on the HSMAC method
- Experimental set up for magnetomechanical measurements with a closed flux path sample
- Influence of the earth connections of the PWM drive on the voltage constraints endured by the motor insulation
- High temperature machine: Characterization of materials for the electrical insulation
- Architecture choices for high-temperature synchronous machines
- Analytical study of air-gap surface force – application to electrical machines
- High-power density induction machines with increased windings temperature
- Influence of modern magnetic and insulation materials on dimensions and losses of large induction machines
- New emotional model environment for navigation in a virtual reality
- Performance comparison of axial-flux switched reluctance machines with non-oriented and grain-oriented electrical steel rotors
- Erratum
- Erratum to “Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications”
Articles in the same Issue
- Regular Articles
- Model of electric charge distribution in the trap of a close-contact TENG system
- Dynamics of Online Collective Attention as Hawkes Self-exciting Process
- Enhanced Entanglement in Hybrid Cavity Mediated by a Two-way Coupled Quantum Dot
- The nonlinear integro-differential Ito dynamical equation via three modified mathematical methods and its analytical solutions
- Diagnostic model of low visibility events based on C4.5 algorithm
- Electronic temperature characteristics of laser-induced Fe plasma in fruits
- Comparative study of heat transfer enhancement on liquid-vapor separation plate condenser
- Characterization of the effects of a plasma injector driven by AC dielectric barrier discharge on ethylene-air diffusion flame structure
- Impact of double-diffusive convection and motile gyrotactic microorganisms on magnetohydrodynamics bioconvection tangent hyperbolic nanofluid
- Dependence of the crossover zone on the regularization method in the two-flavor Nambu–Jona-Lasinio model
- Novel numerical analysis for nonlinear advection–reaction–diffusion systems
- Heuristic decision of planned shop visit products based on similar reasoning method: From the perspective of organizational quality-specific immune
- Two-dimensional flow field distribution characteristics of flocking drainage pipes in tunnel
- Dynamic triaxial constitutive model for rock subjected to initial stress
- Automatic target recognition method for multitemporal remote sensing image
- Gaussons: optical solitons with log-law nonlinearity by Laplace–Adomian decomposition method
- Adaptive magnetic suspension anti-rolling device based on frequency modulation
- Dynamic response characteristics of 93W alloy with a spherical structure
- The heuristic model of energy propagation in free space, based on the detection of a current induced in a conductor inside a continuously covered conducting enclosure by an external radio frequency source
- Microchannel filter for air purification
- An explicit representation for the axisymmetric solutions of the free Maxwell equations
- Floquet analysis of linear dynamic RLC circuits
- Subpixel matching method for remote sensing image of ground features based on geographic information
- K-band luminosity–density relation at fixed parameters or for different galaxy families
- Effect of forward expansion angle on film cooling characteristics of shaped holes
- Analysis of the overvoltage cooperative control strategy for the small hydropower distribution network
- Stable walking of biped robot based on center of mass trajectory control
- Modeling and simulation of dynamic recrystallization behavior for Q890 steel plate based on plane strain compression tests
- Edge effect of multi-degree-of-freedom oscillatory actuator driven by vector control
- The effect of guide vane type on performance of multistage energy recovery hydraulic turbine (MERHT)
- Development of a generic framework for lumped parameter modeling
- Optimal control for generating excited state expansion in ring potential
- The phase inversion mechanism of the pH-sensitive reversible invert emulsion from w/o to o/w
- 3D bending simulation and mechanical properties of the OLED bending area
- Resonance overvoltage control algorithms in long cable frequency conversion drive based on discrete mathematics
- The measure of irregularities of nanosheets
- The predicted load balancing algorithm based on the dynamic exponential smoothing
- Influence of different seismic motion input modes on the performance of isolated structures with different seismic measures
- A comparative study of cohesive zone models for predicting delamination fracture behaviors of arterial wall
- Analysis on dynamic feature of cross arm light weighting for photovoltaic panel cleaning device in power station based on power correlation
- Some probability effects in the classical context
- Thermosoluted Marangoni convective flow towards a permeable Riga surface
- Simultaneous measurement of ionizing radiation and heart rate using a smartphone camera
- On the relations between some well-known methods and the projective Riccati equations
- Application of energy dissipation and damping structure in the reinforcement of shear wall in concrete engineering
- On-line detection algorithm of ore grade change in grinding grading system
- Testing algorithm for heat transfer performance of nanofluid-filled heat pipe based on neural network
- New optical solitons of conformable resonant nonlinear Schrödinger’s equation
- Numerical investigations of a new singular second-order nonlinear coupled functional Lane–Emden model
- Circularly symmetric algorithm for UWB RF signal receiving channel based on noise cancellation
- CH4 dissociation on the Pd/Cu(111) surface alloy: A DFT study
- On some novel exact solutions to the time fractional (2 + 1) dimensional Konopelchenko–Dubrovsky system arising in physical science
- An optimal system of group-invariant solutions and conserved quantities of a nonlinear fifth-order integrable equation
- Mining reasonable distance of horizontal concave slope based on variable scale chaotic algorithms
- Mathematical models for information classification and recognition of multi-target optical remote sensing images
- Hopkinson rod test results and constitutive description of TRIP780 steel resistance spot welding material
- Computational exploration for radiative flow of Sutterby nanofluid with variable temperature-dependent thermal conductivity and diffusion coefficient
- Analytical solution of one-dimensional Pennes’ bioheat equation
- MHD squeezed Darcy–Forchheimer nanofluid flow between two h–distance apart horizontal plates
- Analysis of irregularity measures of zigzag, rhombic, and honeycomb benzenoid systems
- A clustering algorithm based on nonuniform partition for WSNs
- An extension of Gronwall inequality in the theory of bodies with voids
- Rheological properties of oil–water Pickering emulsion stabilized by Fe3O4 solid nanoparticles
- Review Article
- Sine Topp-Leone-G family of distributions: Theory and applications
- Review of research, development and application of photovoltaic/thermal water systems
- Special Issue on Fundamental Physics of Thermal Transports and Energy Conversions
- Numerical analysis of sulfur dioxide absorption in water droplets
- Special Issue on Transport phenomena and thermal analysis in micro/nano-scale structure surfaces - Part I
- Random pore structure and REV scale flow analysis of engine particulate filter based on LBM
- Prediction of capillary suction in porous media based on micro-CT technology and B–C model
- Energy equilibrium analysis in the effervescent atomization
- Experimental investigation on steam/nitrogen condensation characteristics inside horizontal enhanced condensation channels
- Experimental analysis and ANN prediction on performances of finned oval-tube heat exchanger under different air inlet angles with limited experimental data
- Investigation on thermal-hydraulic performance prediction of a new parallel-flow shell and tube heat exchanger with different surrogate models
- Comparative study of the thermal performance of four different parallel flow shell and tube heat exchangers with different performance indicators
- Optimization of SCR inflow uniformity based on CFD simulation
- Kinetics and thermodynamics of SO2 adsorption on metal-loaded multiwalled carbon nanotubes
- Effect of the inner-surface baffles on the tangential acoustic mode in the cylindrical combustor
- Special Issue on Future challenges of advanced computational modeling on nonlinear physical phenomena - Part I
- Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications
- Some new extensions for fractional integral operator having exponential in the kernel and their applications in physical systems
- Exact optical solitons of the perturbed nonlinear Schrödinger–Hirota equation with Kerr law nonlinearity in nonlinear fiber optics
- Analytical mathematical schemes: Circular rod grounded via transverse Poisson’s effect and extensive wave propagation on the surface of water
- Closed-form wave structures of the space-time fractional Hirota–Satsuma coupled KdV equation with nonlinear physical phenomena
- Some misinterpretations and lack of understanding in differential operators with no singular kernels
- Stable solutions to the nonlinear RLC transmission line equation and the Sinh–Poisson equation arising in mathematical physics
- Calculation of focal values for first-order non-autonomous equation with algebraic and trigonometric coefficients
- Influence of interfacial electrokinetic on MHD radiative nanofluid flow in a permeable microchannel with Brownian motion and thermophoresis effects
- Standard routine techniques of modeling of tick-borne encephalitis
- Fractional residual power series method for the analytical and approximate studies of fractional physical phenomena
- Exact solutions of space–time fractional KdV–MKdV equation and Konopelchenko–Dubrovsky equation
- Approximate analytical fractional view of convection–diffusion equations
- Heat and mass transport investigation in radiative and chemically reacting fluid over a differentially heated surface and internal heating
- On solitary wave solutions of a peptide group system with higher order saturable nonlinearity
- Extension of optimal homotopy asymptotic method with use of Daftardar–Jeffery polynomials to Hirota–Satsuma coupled system of Korteweg–de Vries equations
- Unsteady nano-bioconvective channel flow with effect of nth order chemical reaction
- On the flow of MHD generalized maxwell fluid via porous rectangular duct
- Study on the applications of two analytical methods for the construction of traveling wave solutions of the modified equal width equation
- Numerical solution of two-term time-fractional PDE models arising in mathematical physics using local meshless method
- A powerful numerical technique for treating twelfth-order boundary value problems
- Fundamental solutions for the long–short-wave interaction system
- Role of fractal-fractional operators in modeling of rubella epidemic with optimized orders
- Exact solutions of the Laplace fractional boundary value problems via natural decomposition method
- Special Issue on 19th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering
- Joint use of eddy current imaging and fuzzy similarities to assess the integrity of steel plates
- Uncertainty quantification in the design of wireless power transfer systems
- Influence of unequal stator tooth width on the performance of outer-rotor permanent magnet machines
- New elements within finite element modeling of magnetostriction phenomenon in BLDC motor
- Evaluation of localized heat transfer coefficient for induction heating apparatus by thermal fluid analysis based on the HSMAC method
- Experimental set up for magnetomechanical measurements with a closed flux path sample
- Influence of the earth connections of the PWM drive on the voltage constraints endured by the motor insulation
- High temperature machine: Characterization of materials for the electrical insulation
- Architecture choices for high-temperature synchronous machines
- Analytical study of air-gap surface force – application to electrical machines
- High-power density induction machines with increased windings temperature
- Influence of modern magnetic and insulation materials on dimensions and losses of large induction machines
- New emotional model environment for navigation in a virtual reality
- Performance comparison of axial-flux switched reluctance machines with non-oriented and grain-oriented electrical steel rotors
- Erratum
- Erratum to “Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications”