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Abstract

The bonding state of the asphalt layers in a road pavement structure significantly affects its fatigue life. These bondings, therefore, require detailed tests and optimization. In this paper, the analyses of the correlation between the results of laboratory static tests and the results of fatigue tests of asphalt mixture interlayer bondings were performed. The existence of the relationships between selected parameters was confirmed. In the future, the results of these analyses may allow for assessment of interlayer bondings' fatigue life based on the results of quick and relatively easy static tests.

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Authors and Affiliations

A. Szydło
K. Malicki
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Abstract

The paper presents the results of an extensive investigation of asphalt concrete specimens with geosynthetic interlayer. The subject of this research is evaluation of influence of geosynthetics interlayer applied to bituminous pavements on interlayer bonding of specimens. The results of the tests proves that when geosynthetic is used, the bonding of interlayer depends mainly on the type of bituminous mixture, the type of geosynthetic, and the type and amount of bitumen used for saturation and sticking of geosynthetic. The amount of bitumen used in order to saturate and fix the geosynthetic significantly changes the interlayer bonding of specimens.

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Authors and Affiliations

P. Zieliński
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Abstract

Brazing of two dissimilar structural materials; Zircaloy-4 and SS-316L was performed at 900oC under high vacuum conditions. The metallic glass ribbons (Zr55Cu30Al10Ni2Fe3-at. %) of 30 µm thickness, were used as an interlayer. The bonded region was characterized by scanning electron microscope (SEM), energy dispersive spectroscope (EDS) and microhardness testing. The metallurgical bond formation was due to compositional changes in the molten interlayer and later on its subsequent solidification. Assessment of the bonded zone (BZ) revealed three distinct regions (Region-I, Region-II and Region-III). Diffusion transformation was observed in Region-I and Region-III which were interface with base alloys SS-316L and Zircaloy-4 respectively. However, Region-II at the middle of the BZ was composed of isothermally and athermally solidified portions. The highest values of Microhardness were observed in Region-III which was due to the presence of hard phases. Moreover, a crack parallel to BZ was observed in Region-III and was attributed to differential contraction of base alloys during cooling. Maximum shear stress acting on the BZ was calculated and correlated to the brittle phase cracking.

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Authors and Affiliations

A. Munis
Maosheng Zheng
J.I. Akhter
M. Ahmad
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Abstract

This paper presents the results of an extensive investigation of asphalt concrete beams with geosynthetics interlayer. The subject of the research is an evaluation of infl uence of geosynthetics interlayer applied to bituminous samples on their fatigue life. The results of the tests evidences that when geosynthetics are used, the fatigue life depends mainly on the type of bituminous mixture, the type of geosynthetics, and the type and the amount of bitumen used for saturation and sticking. The amount of bitumen used to saturate and fix the geosynthetic signifi cantly changes the samples fatigue properties. Essential positive correlation between fatigue and parameters of interlayer bonding (shear strength, shear stiffness) occurs in both testing temperatures.

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Authors and Affiliations

P. Zieliński
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Abstract

In the presented work, the author describes a new diagnostic method of ballistic resistance of multi– layered shields. The proper ballistic energy absorbed by the shield is introduced in the form V2BL[R] according to Recht’s and Ipson’s method, and V2BL[Z] according to author’s method. The kinetic energy of the bullet mp · V2p/2 and the momentum of force I are transferred to the shield and the dynamometer of ballistic pendulum. They are used to determine the proper energy V2BL[Z] and ballistic thickness hBL of the shield. The procedure can be widened onto the absorption of the energy by individual layers of the shield, where: AHnan,bn – the effect of n – interlayer on proper energy absorbed by the shield. The effectiveness of the used methods is expressed by average effectiveness coefficient βs of proper energy absorbed by the shield V2BL as well as by average mass coefficients α2s . The ballistic shields can be composed of different grades of metal layers and interlayer areas with well-chosen ballistic proprieties.

The maximization of interlayer effectiveness Nn[R] and Nn[Z] as well as relative mass effectiveness Ms[R] and Ms[Z] leads to optimum conditions of selection of multi–layered shields structures.

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Authors and Affiliations

Zdzisław Zatorski
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Abstract

The structure and load characteristics of the roadway are simplified, and the experimental model of the roadway deformation and damage under compression-shear load is established. The experimental data acquisition system is built with a CCD camera. The digital speckle correlation method is used to calculate the image data of the experimental model. The correspondence between the evolution law of the deformation field, the interlayer displacement and deformation evolution are analysed, including the dynamic characteristic of the roadway surrounding the rock. Research results indicate: (1) The damage peak load of the weak layer structure shows a decreasing trend as the interlayer shear stress increases. As the initially applied shear stress increases, the value of interlayer sliding displacement increases, and the dynamic characteristics become more apparent. (2) In the sub-instability phase of the loading curve, when the surrounding rock slides along the layers under compression-shear load, the stress is re-distributed and transmitted to the deep part of the surrounding rock. Then the surrounding rock of the roadway forms the characteristic of alternating change, between tension to compression. (3) According to the state of dynamic and static mechanics, the deformation evolution of the roadway before the peak load belongs to the static process. Zonal fracturing is part of the transition phase from the static process to the slow dynamic process, and the rockburst damage is a high-speed dynamic process. (4) Under the compression-shear load, due to the weak layer structure of the coal and rock mass, the local fracture, damage, instability and sliding of the surrounding rock of the roadway are the mechanical causes of rockburst. (5) Even if the coal and rock mass does not have the condition of impact tendency, under stress load of the horizontal direction, distribution of large shear stress is formed between layers, and the dynamic damage of the rockburst may occur.
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Bibliography

[1] H. Lippman, The Mechanics of “Protruding” in Coal Mine: Discussion on The Violent Deformation on Both Sides of The Channel in Coal Seam [J], Advances in Mechanics 19 (2), 100-113+59 (1989). DOI: https://doi.org/10.6052/1000-0992-1989-1-j1989-011
[2] H.T. Li, J. Liu, S.K. Zhao, L.S. Cai, Q.X. Qi, L.H. Kong, Experimental Study on The Development Mechanism of Coal Bump Considering The Clamping Effect of Roof and Floor [J], Journal of China Coal Society 43 (11), 2951-2958 (2018). DOI: CNKI:SUN:MTXB.0.2018-11-001
[3] M.V. Kurlenya, V.N. Oparin, V.I. Vostrikov, Effect of Anomalously Low Friction in Block Media [J], Journal of Applied Mechanics & Technical Physics 40 (6), 1116-1120 (1999). DOI: https://doi.org/10.1007/BF02469182
[4] L .M. Dou, H. He, J. He, Z.Y. Wang, New Method of Rock Burst Risk Assessment Using Relative Stress Concentration Factor Superposition [J], Journal of China Coal Society 43 (2), 327-332 (2018). DOI: CNKI:SUN:MTXB.0.2018-02-004
[5] L .P. Li, W.J. Li, Y.S. Pan, Influence of Impact Disturbance on Anomalously Low Friction Rock Bursts [J], Chinese Journal of Rock Mechanics and Engineering, 38 (1), 111-120 (2019). DOI: https://doi.org/10.13722/j.cnki.jrme.2018.0922
[6] L .Y. Pan, H.Z. Yang, Dilatancy Theory for Identification of Premonitory Information of Rock Burst [J], Chinese Journal of Rock Mechanics and Engineering 23 (1), 4528-4530 (2004). DOI: https://doi.org/10.3321/j.issn:1000-6915.2004.z1.056
[7] Q.X. Qi, T.Q. Liu, Y.W. Shi, J.L. Lv, Mechanism of Friction Sliding Instability of Rock Burst [J], Ground Pressure and Strata Control 1, 174-177+200 (1995). DOI: CNKI:SUN:KSYL.0.1995-Z1-042
[8] Q.X. Qi, Y.W. Shi, T.Q. Liu, Mechanism of Instability Caused by Viscous Sliding in Rock Burst [J], Journal of China Coal Society 22 (2), 144-148 (1997). DOI: CNKI:SUN:MTXB.0.1997-02-006
[9] Q.X. Qi, Z.Z. Gao, S. Wang, The Theory of Rock Burst Led by Structure Damage of Bedded Coal-rock Mass [J], Coal Mining Technology (2), 14-17+64 (1998). DOI: CNKI:SUN:MKKC.0.1998-02-004
[10] E.I. Shemyakin, G.L. Fisenko, M.V. Kurlenya, V.N. Oparin, Y.S. Kuznetsov, Zonal Disintegration of Rocks around Underground Work, Part I:Data of In-situ Observations [J], Journal of Mining Science 22 (3), 157-168 (1986). DOI: https://doi.org/10.1007/BF02500863368
[11] E.I. Shemyakin, G.L. Fisenko, M.V. Kurlenya, V.N. Oparin, V.N. Reva, F.P. Glushikhin, M.A. Rozenbaum, E.A. Tropp, Y.S. Kuznetsov, Zonal Disintegration of Rocks around Underground Work, Part II: Rock Fracture Simulated in Equivalent Materials [J], Journal of Mining Science 22 (4), 223-232 (1986). DOI: https://doi.org/10.1007/BF02500845
[12] E.I. Shemyakin, G.L. Fisenko, M.V. Kurlenya, V.N. Oparin, Y.S. Kuznetsov, Zonal Disintegration of Rocks around Underground Workings, Part III: Theoretical Concepts [J], Journal of Mining Science 23 (1), 1-6 (1987). DOI: https://doi.org/10.1007/BF02534034
[13] E.I. Shemyakin, M.V. Kurlenya, V.N. Oparin, V.N. Reva, F.P. Glushikhin, E.A. Tropp, Zonal Disintegration of Rocks around Underground Workings, Part IV: Practical Applications [J], Journal of Mining Science 25 (4), 297- 302 (1989). DOI: https://doi.org/10.1007/BF02528546
[14] W.Q. Guo, S.P. Ma, Y.J. Kang, Q.W. Ma, Virtual Extensometer Based on Digital Speckle Correlation Method and Its Application to Deformation Field Evolution of Rock Specimen [J], Rock and Soil Mechanics 32 (10), 3196- 3200 (2011). DOI: https://doi.org/10.16285/j.rsm.2011.10.030
[15] X.T. Zhang, Q.Y. Zhang, W. Xiang, Q. Gao, S.B. Yuan, C. Wang, Model Test Study of Zonal Disintegration in Deep Layered Jointed Rock Mass [J], Rock and Soil Mechanics 35 (8), 2247-2254 (2014). DOI: CNKI:SUN:YTLX.0.2014-08-018
[16] Y. Xu, P. Yuan, Model Test of Zonal Disintegration in Deep Rock under Blasting Load [J], Chinese Journal of Rock Mechanics and Engineering 34 (S2), 3844-3851 (2015). DOI: CNKI:SUN:YSLX.0.2015-S2-027
[17] Y.M. Song, Z.X. Zhao, L.L. Deng, J.N. Wu, Deformation Field and Acoustic Emission Characteristics of Marble during Sub-instability Stage [J], Journal of Liaoning Technical University 37 (3), 541-546 (2018). DOI: CNKI:SUN:FXKY.0.2018-03-016
[18] Y.S. Pan, K.X. Wang, Pendulum-type Waves Theory on The Mechanism of Anomalously Low Friction between Rock Masses [J], Seismology and Geology 36 (3), 833-844 (2014). DOI: https://doi.org/10.3969/j.issn.0253-4967.2014.03.022
[19] Y.S. Pan, Y.H. Xiao, Z.H. Li, K.X. Wang, Study of Roadway Support Theory of Rock Burst in Coal Mine and Its Application [J], Journal of China Coal Society 39 (2), 222-228 (2014). DOI: https://doi.org/10.13225/j.cnki.jccs.2013.2015
[20] Z.L. Fang, Study on The Ground Pressure and Control Method for Openings in Soft and Broken Rocks in Jin Chuon Mine No. 2 [J]. Journal of Beijing Iron and Steel Institute (1), 1-20 (1984). DOI: CNKI:SUN:BJKD.0.1984-01-000
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Authors and Affiliations

Yimin Song
1
He Ren
1
Hailiang Xu
1
Dong An
1

  1. North China University of Technology, School of Civil Engineering, China
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Abstract

This study aimed to investigate the effect of different coating processes on interlayer coating using ProCAST software and identify the preferred coating process so as to prepare an EH40/2205 composite plate with a coating interlayer of Ni-5 Fe-15 Co (wt.%) displaying good performance. The preparation and characterization tests were conducted to analyze the interlayer coating, the diffusion of elements at the bonding interface and the mechanical properties of the hot-rolled composite plate. The results showed that the coating rate increased linearly with an increase in the initial coating temperature, pressure difference and the width ratio of the suction layer. The interlayer coating was complete under the guidance of optimized process parameters, and the test results and simulations confirmed each other. The coated interlayer successfully blocked the diffusion of elements between the bonding surfaces. The tensile strength of the rolled composite plate was 580 MPa, which met the needs of the project. The tensile shear fracture occurred at EH40, which proved that the plate was well bonded.
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Authors and Affiliations

K.K. Feng
1
ORCID: ORCID
Y.L. Yi
1
ORCID: ORCID
Y. Qin
1
ORCID: ORCID
H.R. Jin
2 3
ORCID: ORCID

  1. Yanshan University, School of Mechanical Engineering, Qinhuangdao, China
  2. Yanshan University, Key Laboratory of Advanced Forging & Stamping Technology and Science of Ministry of National Education, Qinhuangdao, China
  3. Yanshan University, Parallel Robot and Mechatronic System Laboratory of Hebei Province, Qinhuangdao, China
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Abstract

Ultrasound-promoted transient liquid phase bonding (U-TLP) is a high quality, high efficiency, and low-cost method for fast bonding of difficult-wetting materials in the atmospheric environment. In this paper, U-TLP was used to bond SiC particles reinforced aluminium-based metal matrix composite which particle volume fraction was 70%. The pure zinc foil was used as the intermediate layer. The effects of ultrasonic on microstructure evolution and mechanical properties of joints during the transient liquefaction stage were investigated. The mechanism of ultrasonic effects in the transient liquefaction stage of U-TLP was also inducted. The results showed that high volume fraction SiCp/Al MMCs were bonded well at low temperature in the air environment. Ultrasonic vibration can remove the oxide film on the surface of aluminum matrix composites, enhance the wettability of SiC particles with weld metal, promote atomic diffusion and homogenization of SiC particles, and improve the welding quality and efficiency. Reasonable increase of ultrasonic vibration time could effectively improve the joint strength.
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Authors and Affiliations

Changzhuang Zhou
1
ORCID: ORCID
Lin Ma
1 2
ORCID: ORCID
Chao Zhu
1
ORCID: ORCID
Qinghe Cui
1
ORCID: ORCID
Jindi Liang
1
ORCID: ORCID
Yujian Song
1
ORCID: ORCID

  1. Shenyang Aerospace University, School of Materials Science and Engineering, Shenyang 110136, China
  2. The University of Queensland, Australia
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Abstract

One of the common defects of flexible road pavement is the loss of bonding between two layers of asphalt concrete: the base course and the binder course. The occurrence of this phenomenon has a major impact on the observed state of deflection and deformation of the pavement. This effect affects the results of non-destructive tests which are used to calculate material parameters and then are used in the diagnostics of the pavement condition or design of structural strengthening. This paper discusses the influence of the various level of bonding on the result of backcalculation and the obtained elastic moduli. For the obtained values of moduli, calculations of key deformations and pavement durability were performed. Improper assumptions about the interaction between the layers affects the observed results. Additionally paper discusses the effect of pavement displacement discontinuity on the observed deflection basin and compares the results with those for a model with continuity. Numerical calculations were carried out using Simulia Abaqus software, the computational model was verified using analytical solution.
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Authors and Affiliations

Paweł Tutka
1
ORCID: ORCID
Roman Nagórski
1
ORCID: ORCID
Magdalena Złotowska
1
ORCID: ORCID

  1. Warsaw University of Technology, Faculty of Civil Engineering, Al. Armii Ludowej 16, 00-637 Warsaw, Poland
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Abstract

In order to investigate the influence of vertical ground motion on seismic responses of story-isolation structures mounted on triple friction pendulum (TFP) bearings, the finite element model of a six-story building with various types of interlayer isolation TFP bearings under far field or near fault ground motions is established and analysed. A discrepancy rate function of peak interlayer shear, acceleration and displacement results is adopted to discuss the influence of the vertical seismic motions on isolation structural responses. Furthermore, the isolation form, the isolation period and the friction coefficient of bearings are changed to study their effect on the vertical seismic component’s influence. The results show that the influence of the vertical seismic component is considerable on the isolation layer especially under near-fault ground motions, so it should not be overlooked during the structural design; The change of isolation forms will greatly affect the influence of the vertical seismic component especially in the isolation layer and isolation systems with isolation devices set on higher stories or with less isolation layers will have less vertical seismic effect on story acceleration; The increase of the isolation period will globally result in the decrease of the influence of vertical seismic components, though in some cases it shows some sort of fluctuation before the final decrease; The increase of the friction coefficient will lead to the global decrease in the influence of the vertical seismic component in single-layer isolation structures, while it does not obviously affect those in the multi-layer isolation systems.
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Bibliography


[1] K. Ryan, C. Earl. “Analysis and Design of Inter-story Isolation Systems with Nonlinear Devices,” Journal of Earthquake Engineering 14(7): pp. 1044–1062, 2010. https://doi.org/10.1080/13632461003668020
[2] D.C.Charmpis, P.Komodromos, M.C.Phocas. “Optimized earthquake response of multi‐storey buildings with seismic isolation at various elevations,” Earthquake Engineering & Structural Dynamics 41(15): pp. 2289–2310, 2012. https://doi.org/10.1002/eqe.2187
[3] H. Fakhri, G.G. Amiri. “Nonlinear Response-History Analysis of Triple Friction Pendulum Bearings (TFPB), Installed Between Stories,” 15th World Conference on Earthquake Engineering, Lisbon, 2012.
[4] A. Reggio, M.D. Angelis. “Optimal energy‐based seismic design of non‐conventional Tuned Mass Damper (TMD) implemented via inter‐story isolation,” Earthquake Engineering & Structural Dynamics 44(10): pp. 1623–1642, 2015. https://doi.org/10.1002/eqe.2548
[5] M. Rabiei, F. Khoshnoudian. “Response of multistory friction pendulum base-isolated buildings including the vertical component of earthquakes,” Canadian Journal of Civil Engineering 38(10): pp. 1045–1059, 2011. https://doi.org/10.1139/l11-064
[6] K. Faramarz, R. Montazar. “Seismic Response of Double Concave Friction Pendulum Base-Isolated Structures Considering Vertical Component of Earthquake,” Advances in Structural Engineering 13(1): pp. 1–14, 2010. https://doi.org/10.1260/1369-4332.13.1.1
[7] V. Loghman, F. Khoshnoudian, M. Banazadeh. “Effect of vertical component of earthquake on seismic response of triple concave friction pendulum base-isolated structures,” Journal of Vibration & Control 21(11): pp. 2099–2113, 2013. https://doi.org/10.1177/1077546313503359
[8] D.M. Fenz, M.C. Constantinou. “Spherical sliding isolation bearings with adaptive behavior: Theory,” Earthquake Engineering and Structural Dynamics 37(2): pp. 163-183, 2008. https://doi.org/10.1002/eqe.751
[9] D.M. Fenz, M.C. Constantinou. “Spherical sliding isolation bearings with adaptive behavior: Experimental verification,” Earthquake Engineering & Structural Dynamics 37(2): pp. 185–205, 2010. https://doi.org/10.1002/eqe.750
[10] N.D. Dao. “Seismic Response of a Full-scale 5-story Steel Frame Building Isolated by Triple Pendulum Bearings under Three-Dimensional Excitations,” Dissertations & Theses - Gradworks, University of Nevada, 2012.
[11] T.C. Becker, S.A. Mahin. “Approximating peak responses in seismically isolated buildings using generalized modal analysis,” Earthquake Engineering & Structural Dynamics 42(12): pp. 1807–1825, 2014. https://doi.org/10.1002/eqe.2299
[12] J. Sheller, M.C. Constantinou. “Response history analysis of structures with seismic isolation and energy dissipation systems: verification examples for program SAP2000,” Report No. MCEER 99-02, Multidisciplinary Center for Earthquake Engineering Research, New York, 1999.
[13] W.I. Liao, C.H. Loh, S. Wan. “Earthquake responses of RC moment frames subjected to near-fault ground motions,” Structural Design of Tall & Special Buildings 10(3): pp. 219–229, 2001. https://doi.org/10.1002/tal.178
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Authors and Affiliations

Zhao Fang
1
Ping Yan
2

  1. Nanjing Institute of Technology, School of Architecture Engineering, Hongjing Avenue 1, 211167 Nanjing, China
  2. Jiangsu Provincial Architectural D&R Institute LTD, Chuangyi Road 86, 211167 Nanjing, China
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Abstract

The aim of this paper is to compare some geometric parameters and deflections of a sandwich meta-structure with its classic, three-layer counterpart. Both structures are composed of the same materials and have the same external dimensions and mass, but their middle layers (cores) are different. The core of the sandwich meta-structure is a new spatial structure itself, consisting of there-layer bars. The core of the classic sandwich structure is a layer of the continuum. To make the comparison more general and convincing, three geometrical parameters, i.e., ratio of interfacial contact (Ric), interlayer bonding factor (Ibf) and coefficient of impact sensitivity (Cis), were introduced and applied. Deflections of the structures, simply supported at the edges and loaded in the mid-span by a static force, have been measured and are presented in the paper. Potential advantages of the new meta-structure are briefly outlined.

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Bibliography

[1] A. Valera-Medina, A. Giles, D. Pugh, S. Morris, M. Pohl, and A. Ortwein. Investigation of combustion of emulated biogas in a gas turbine test rig. Journal of Thermal Science, 27:331–340, 2018. doi: 10.1007/s11630-018-1024-1.
[2] K. Tanaka and I. Ushiyama. Thermodynamic performance analysis of gas turbine power plants with intercooler: 1st report, Theory of intercooling and performance of intercooling type gas turbine. Bulletin of JSME, 13(64):1210–1231, 1970. doi: 10.1299/jsme1958.13.1210.
[3] H.M. Kwon, T.S. Kim, J.L. Sohn, and D.W. Kang. Performance improvement of gas turbine combined cycle power plant by dual cooling of the inlet air and turbine coolant using an absorption chiller. Energy, 163:1050–1061, 2018. doi: 10.1016/j.energy.2018.08.191.
[4] A.T. Baheta and S.I.-U.-H. Gilani. The effect of ambient temperature on a gas turbine performance in part load operation. AIP Conference Proceedings, 1440:889–893, 2012. doi: 10.1063/1.4704300.
[5] F.R. Pance Arrieta and E.E. Silva Lora. Influence of ambient temperature on combined-cycle power-plant performance. Applied Energy, 80(3):261–272, 2005. doi: 10.1016/j.apenergy.2004.04.007.
[6] M. Ameri and P. Ahmadi. The study of ambient temperature effects on exergy losses of a heat recovery steam generator. In: Cen, K., Chi, Y., Wang, F. (eds) Challenges of Power Engineering and Environment. Springer, Berlin, Heidelberg, 2007. doi: 10.1007/978-3-540-76694-0_9.
[7] M.A.A. Alfellag: Parametric investigation of a modified gas turbine power plant. Thermal Science and Engineering Progress, 3:141–149, 2017. doi: 10.1016/j.tsep.2017.07.004.
[8] J.H. Horlock and W.A. Woods. Determination of the optimum performance of gas turbines. Proceedings of the Institution of Mechanical Engineers, Part C: Journal of Mechanical Engineering Science, 214:243–255, 2000. doi: 10.1243/0954406001522930.
[9] L. Battisti, R. Fedrizzi, and G. Cerri. Novel technology for gas turbine blade effusion cooling. In: Proceedings of the ASME Turbo Expo 2006: Power for Land, Sea, and Air. Volume 3: Heat Transfer, Parts A and B. pages 491–501. Barcelona, Spain. May 8–11, 2006. doi: 10.1115/GT2006-90516.
[10] F.J. Wang and J.S. Chiou. Integration of steam injection and inlet air cooling for a gas turbine generation system. Energy Conversion and Management, 45(1):15–26, 2004. doi: 10.1016/S0196-8904 (03)00125-0.
[11] Z. Wang. 1.23 Energy and air pollution. In I. Dincer (ed.): Comprehensive Energy Systems, pp. 909–949. Elsevier, 2018. doi: 10.1016/B978-0-12-809597-3.00127-9.
[12] Z. Khorshidi, N.H. Florin, M.T. Ho, and D.E. Wiley. Techno-economic evaluation of co-firing biomass gas with natural gas in existing NGCC plants with and without CO$_2$ capture. International Journal of Greenhouse Gas Control, 49:343–363, 2016. doi: 10.1016/j.ijggc.2016.03.007.
[13] K. Mohammadi, M. Saghafifar, and J.G. McGowan. Thermo-economic evaluation of modifications to a gas power plant with an air bottoming combined cycle. Energy Conversion and Management, 172:619–644, 2018. doi: 10.1016/j.enconman.2018.07.038.
[14] S. Mohtaram, J. Lin, W. Chen, and M.A. Nikbakht. Evaluating the effect of ammonia-water dilution pressure and its density on thermodynamic performance of combined cycles by the energy-exergy analysis approach. Mechanika, 23(2):18110, 2017. doi: 10.5755/j01.mech.23.2.18110.
[15] M. Maheshwari and O. Singh. Comparative evaluation of different combined cycle configurations having simple gas turbine, steam turbine and ammonia water turbine. Energy, 168:1217–1236, 2019. doi: 10.1016/j.energy.2018.12.008.
[16] A. Khaliq and S.C. Kaushik. Second-law based thermodynamic analysis of Brayton/Rankine combined power cycle with reheat. Applied Energy, 78(2):179–197, 2004. doi: 10.1016/j.apenergy.2003.08.002.
[17] M. Aliyu, A.B. AlQudaihi, S.A.M. Said, and M.A. Habib. Energy, exergy and parametric analysis of a combined cycle power plant. Thermal Science and Engineering Progress. 15:100450, 2020. doi: 10.1016/j.tsep.2019.100450.
[18] M.N. Khan, T.A. Alkanhal, J. Majdoubi, and I. Tlili. Performance enhancement of regenerative gas turbine: air bottoming combined cycle using bypass valve and heat exchanger—energy and exergy analysis. Journal of Thermal Analysis and Calorimetry. 144:821–834, 2021. doi: 10.1007/s10973-020-09550-w.
[19] F. Rueda Martínez, A. Rueda Martínez, A. Toleda Velazquez, P. Quinto Diez, G. Tolentino Eslava, and J. Abugaber Francis. Evaluation of the gas turbine inlet temperature with relation to the excess air. Energy and Power Engineering, 3(4):517–524, 2011. doi: 10.4236/epe.2011.34063.
[20] A.K. Mohapatra and R. Sanjay. Exergetic evaluation of gas-turbine based combined cycle system with vapor absorption inlet cooling. Applied Thermal Engineering, 136:431–443, 2018. doi: 10.1016/j.applthermaleng.2018.03.023.
[21] A.A. Alsairafi. Effects of ambient conditions on the thermodynamic performance of hybrid nuclear-combined cycle power plant. International Journal of Energy Research, 37(3):211–227, 2013. doi: 10.1002/er.1901.
[22] A.K. Tiwari, M.M. Hasan, and M. Islam. Effect of ambient temperature on the performance of a combined cycle power plant. Transactions of the Canadian Society for Mechanical Engineering, 37(4):1177–1188, 2013. doi: 10.1139/tcsme-2013-0099.
[23] T.K. Ibrahim, M.M. Rahman, and A.N. Abdalla. Gas turbine configuration for improving the performance of combined cycle power plant. Procedia Engineering, 15:4216–4223, 2011. doi: 10.1016/j.proeng.2011.08.791.
[24] M.N. Khan and I. Tlili. New advancement of high performance for a combined cycle power plant: Thermodynamic analysis. Case Studies in Thermal Engineering. 12:166–175, 2018. doi: 10.1016/j.csite.2018.04.001.
[25] S.Y. Ebaid and Q.Z. Al-hamdan. Thermodynamic analysis of different configurations of combined cycle power plants. Mechanical Engineering Research. 5(2):89–113, 2015. doi: 10.5539/mer.v5n2p89.
[26] R. Teflissi and A. Ataei. Effect of temperature and gas flow on the efficiency of an air bottoming cycle. Journal of Renewable and Sustainable Energy, 5(2):021409, 2013. doi: 10.1063/1.4798486.
[27] A.A. Bazmi, G. Zahedi, and H. Hashim. Design of decentralized biopower generation and distribution system for developing countries. Journal of Cleaner Production, 86:209–220, 2015. doi: 10.1016/j.jclepro.2014.08.084.
[28] A.I. Chatzimouratidis and P.A. Pilavachi. Decision support systems for power plants impact on the living standard. Energy Conversion and Management, 64:182–198, 2012. doi: 10.1016/j.enconman.2012.05.006.
[29] T.K. Ibrahim, F. Basrawi, O.I. Awad, A.N. Abdullah, G. Najafi, R. Mamat, and F.Y. Hagos. Thermal performance of gas turbine power plant based on exergy analysis. Applied Thermal Engineering, 115:977–985, 2017. doi: 10.1016/j.applthermaleng.2017.01.032.
[30] M. Ghazikhani, I. Khazaee, and E. Abdekhodaie. Exergy analysis of gas turbine with air bottoming cycle. Energy, 72:599–607, 2014. doi: 10.1016/j.energy.2014.05.085.
[31] M.N. Khan, I. Tlili, and W.A. Khan. thermodynamic optimization of new combined gas/steam power cycles with HRSG and heat exchanger. Arabian Journal for Science and Engineering, 42:4547–4558, 2017. doi: 10.1007/s13369-017-2549-4.
[32] N. Abdelhafidi, İ.H. Yılmaz, and N.E.I. Bachari. An innovative dynamic model for an integrated solar combined cycle power plant under off-design conditions. Energy Conversion and Management, 220:113066, 2020. doi: 10.1016/j.enconman.2020.113066.
[33] T.K. Ibrahim, M.K. Mohammed, O.I. Awad, M.M. Rahman, G. Najafi, F. Basrawi, A.N. Abd Alla, and R. Mamat. The optimum performance of the combined cycle power plant: A comprehensive review. Renewable and Sustainable Energy Reviews, 79:459–474, 2017. doi: 10.1016/j.rser.2017.05.060.
[34] M.N. Khan. Energy and exergy analyses of regenerative gas turbine air-bottoming combined cycle: optimum performance. Arabian Journal for Science and Engineering, 45:5895–5905, 2020. doi: 10.1007/s13369-020-04600-9.
[35] A.M. Alklaibi, M.N. Khan, and W.A. Khan. Thermodynamic analysis of gas turbine with air bottoming cycle. Energy, 107:603–611, 2016. doi: 10.1016/j.energy.2016.04.055.
[36] M. Ghazikhani, M. Passandideh-Fard, and M. Mousavi. Two new high-performance cycles for gas turbine with air bottoming. Energy, 36(1):294–304, 2011. doi: 10.1016/j.energy.2010.10.040.
[37] M.N. Khan and I. Tlili. Innovative thermodynamic parametric investigation of gas and steam bottoming cycles with heat exchanger and heat recovery steam generator: Energy and exergy analysis. Energy Reports, 4:497–506, 2018. doi: 10.1016/j.egyr.2018.07.007.
[38] M.N. Khan and I. Tlili. Performance enhancement of a combined cycle using heat exchanger bypass control: A thermodynamic investigation. Journal of Cleaner Production, 192:443–452, 2018. doi: 10.1016/j.jclepro.2018.04.272.
[39] M. Korobitsyn. Industrial applications of the air bottoming cycle. Energy Conversion and Management, 43(9-12):1311–1322, 2002. doi: 10.1016/S0196-8904(02)00017-1.
[40] T.K. Ibrahim and M.M. Rahman. optimum performance improvements of the combined cycle based on an intercooler–reheated gas turbine. Journal of Energy Resources Technology, 137(6):061601, 2015. doi: 10.1115/1.4030447.
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Authors and Affiliations

Stanisław Karczmarzyk

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Abstract

The article presents a new approach to testing the strength of asphalt interlayer bonding. Two loading methods were used: static load and cyclic load. Before carrying out static shear strength tests, the interlayer bonding was subjected to cyclic loads with a constant number of cycles but with different frequencies. A number of layered samples with and without geosynthetic interlayers were tested at the set temperature. The comparative analyses allowed to determine the functions approximating the impact of the cyclic load frequency on the static strength of bonding at selected interlayer contact conditions. It was also possible to indicate the frequency of cyclic load at which this parameter has the largest and smallest impact on the static strength of the asphalt interlayer bonding.

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Authors and Affiliations

Jarosław Górszczyk
Konrad Malicki

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