Authors:
Al-Saudi Sarah Kareem Mohammed Faculty of Materials and Chemical Engineering, Institute of Energy, Ceramic and Polymer Technology, University of Miskolc, Miskolc-Egyetemvaros, Hungary
Department of Building and Construction Technologies Engineering, Al-Esraa University College, Baghdad, Iraq

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Róbert Géber Faculty of Materials and Chemical Engineering, Institute of Energy, Ceramic and Polymer Technology, University of Miskolc, Miskolc-Egyetemvaros, Hungary

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Abstract

This article aims to achieve the hardening of geopolymer binder-based metakaolin under the same setting time and hardening temperature as traditional cement. It studied the hardening of the geopolymer binder-based metakaolin at two temperatures of 60 °C and room temperature using different liquid-to-solid ratios of 0.8, 0.95, and 1.1. The bulk density, compressive strength, sitting times, thermal conductivity, and microstructure were measured for geopolymer binders. Based on the specified range for cement characteristics, the geopolymer binder was solidified at room temperature, utilizing a liquid-to-solid ratio of 0.8 to achieve optimal results stratified according to the cement's ideal characteristics. It had a bulk density of 1.264 g cm−3, compressive strength of 19.12 MPa, initial setting time of 288 min, final setting time of 358 min, and thermal conductivity of 0.49 W m−1 K.

Abstract

This article aims to achieve the hardening of geopolymer binder-based metakaolin under the same setting time and hardening temperature as traditional cement. It studied the hardening of the geopolymer binder-based metakaolin at two temperatures of 60 °C and room temperature using different liquid-to-solid ratios of 0.8, 0.95, and 1.1. The bulk density, compressive strength, sitting times, thermal conductivity, and microstructure were measured for geopolymer binders. Based on the specified range for cement characteristics, the geopolymer binder was solidified at room temperature, utilizing a liquid-to-solid ratio of 0.8 to achieve optimal results stratified according to the cement's ideal characteristics. It had a bulk density of 1.264 g cm−3, compressive strength of 19.12 MPa, initial setting time of 288 min, final setting time of 358 min, and thermal conductivity of 0.49 W m−1 K.

1 Introduction

Geopolymer is well known as an alternative to conventional Portland cement, representing a development shift in construction. There are many advantages to opting for geopolymer over cement, foremost among them being the reduction in CO2 emissions, alongside reduced energy used, and it had lower thermal conductivity. The geopolymer binder needs curing by heat to harden, which hinders use as a cement replacement [1, 2].

Geopolymer binder has a quality performance comparable to conventional cement due to its strength, fire resistance due to low thermal conductivity, and acid and alkali resistance, in addition, it produces less than 20% of the carbon emissions of conventional Portland cement [3]. Geopolymer is formed by activating materials rich in aluminosilicate like fly ash, kaolin, metakaolin, slag, mine, etc., obtained from natural minerals or solid waste materials [1, 4]. The highly alkaline conditions are used to induce the formation of polymeric aluminosilicate compounds from geological materials by using alkali metal silicate solutions [4–6].

Geopolymers are utilized in various applications due to their versatile properties. They are prominent in the production of fire-resistant materials and innovative ceramics. They are effective alternatives to asbestos, offering safe and durable building materials. Geopolymers also play a critical role in stabilizing hazardous waste, providing a secure method for waste containment. Additionally, they are used as adsorbent materials in water treatment processes, enhancing the removal of contaminants and improving water quality [5].

Metakaolin will be expected as a major resource for the geopolymer binder due to its main contents of SiO2 and Al2O3, and excellent chemical stability compared with other waste materials. The obtained by heating kaolin at temperatures higher than 650 °C. Consequently, the mass of the kaolin was reduced by approximately 14 wt% due to the removal of strongly attached hydroxyl ions and the disintegration of the kaolin structure, resulting in the contraction and dissolution of the organized arrangement inside the alumina and silica layers [6]. Metakaolin, outstanding in its amorphous structure and unique characteristics, emerges as a compelling alternative to cement in geopolymer production, especially when compared with other aluminum silicate sources. Its inherent pozzolanic and latent hydraulic reactivity, a significant surface area, minimal impurities, and a substantial amorphous composition resulted in solidification without requiring heat curing [7].

Multiple factors affect the geopolymer characteristics: raw materials type, alkali activator molarity, SiO2/Al2O3 ratio, liquid-to-solid ratio, curing conditions (temperature, and time), etc. All these factors significantly contribute to influencing the properties of the geopolymer binder. It affects density, strength, porosity percent, sitting time, thermal conductivity, and microstructure, depending on these properties geopolymer binder could be used in many fields for example decorative stone, thermal insulation, refractory materials, foundry applications, concrete, aircraft ways, etc. [8, 9].

N A Jaya et al. [10] investigated the impact of various Liquid-to-Solid (L/S) ratios specifically 1.66, 1.42, 1.25, 1.11, and 1 on the properties of metakaolin-based geopolymers. The study used a NaOH/Na2SiO3 ratio of 1 and used a 10 M NaOH solution. After aging the samples for 28 days, it was found that the optimal compressive strength of 32 MPa was achieved with a L/S ratio of 0.8. Adelino Lopes et al. [11] recommended, preventing a reduction in the strength of metakaolin-based geopolymers, it is recommended to use curing temperatures below 30 °C. Samples cured at 50 °C show a decrease of over 35% in flexural strength and more than 60% in compressive strength compared to those cured at room temperature.

In this work, two factors effects were studied the liquid-to-solid ratio and curing temperature. The objective was to prepare a metakaolin-based geopolymer binder solidifying at room temperature within an acceptable setting time.

2 Materials and methods

2.1 Raw material

The solid raw material for preparing the geopolymer binder was kaolin and the materials to prepare the activator solution were water glass, sodium hydroxide flakes, and distilled water. Table 1 shows the water glass properties and Table 2 sodium hydroxide properties, identified by the manufacturer company.

Table 1.

Water glass properties

NameSilicate sodium
FormulaNa2SiO3
CaseLiquid
Density1.37 g cm−3
Silicate modulus3.80
Chemical compositionH2O: 61.06 wt%
SiO2: 30.95 wt%
Na2O: 8.00 wt%
Table 2.

Properties sodium hydroxide flakes

NameSodium hydroxide
FormulaNaOH
CaseSolid (flakes)
Purity∼98%

2.2 Characterization techniques of the kaolin and metakaolin

The transformation phases of kaolin into metakaolin were analyzed through X-ray diffraction using the Rigaku Miniflex II diffractometer model. The oxide composition of metakaolin was determined using X-ray fluorescence with the Rigaku SuperMini 200 spectrometry.

Placeholder granulometry 715 measured partial size in a range of 1–192 µm.

2.3 Geopolymer binder preparation

Metakaolin was prepared by calcinating the kaolin at 750 °C for 3 h. The metakaolin was milled to fine powder by using a ball mill model Retsch PM 400, milling conditions speed of 180 rpm and milling time of 20 min. Five silica balls were used to mill with different sizes (the diameter of three balls was 150 cm and for the other two balls was 30 cm). The sodium hydroxide solution was made to a concentration of 10 mol L−1 by dissolving 800 g of sodium hydroxide flakes in 2 L of distilled water. It was mixing an equal weight percentage of water glass and sodium hydroxide solution to prepare the activator solution [12]. The geopolymer binder samples were prepared by using a silicon mold cubic with a length of 5 cm, the samples were cured at two different temperatures: 60 °C and room temperature, and formulated with different liquid-to-solid ratios of 0.8, 0.95, and 1.1. The geopolymer binder mix proportion design is shown in Table 3 for a cubic length of 5 cm.

Table 3.

Composition of geopolymer binder with a NaOH/Na2SiO3 ratio of 1 and NaOH with (10 mol L−1)

Samples CodsL/SLiquid (g)Solid (g)
Na2SiO3NaOHMetakaolin
GP 0.81.15050125.0
GP 0.90.95050111.1
GP 1.10.8505090.9

2.4 Characterization techniques of the geopolymer binder

The geopolymer binder's bulk density and compressive strength were assessed using cubic samples measuring 5 cm long after a 28-day curing process at 60 °C for 24 h and at ambient room temperature. Bulk density was determined for an average of five samples according to ASTM C642-06:2006 [13] by dividing the mass of the sample by its volume. The compressive strength of the samples was evaluated using an automated Smart Power and Control System specifically designed for standard failure testing, the Zwick/Roell Z100. Three cubic samples were subjected to testing at a speed of 2 mm min−1, following the ASTM C109/C109M-02:2002 [14] standard. Compressive strength was calculated by dividing the maximum force applied by the cross-sectional area.

The C-Therm TCi thermal conductivity analyzer instrument has been used to measure the thermal conductivity of the geopolymer binder. The sample cubic shape with a side length of 2.5 cm conductive materials was applied to the sample's surface before it was placed on the sensor. The test was performed at room temperature.

The sitting times of the geopolymer binder were measured with the used Vicat apparatus according to standard EN 196-3:2005 [15]. The Vicat mold was filled with a geopolymer binder, and the filled mold with a base plate was put in the container, adjusting the distance zero between the end of the needle and the base, the test was made at room temperature 23 °C. A thin metal needle with a diameter of 1 mm was used to measure the initial time. It checked the needle penetration every 15 min. The onset of the initial setting time was determined by observing the penetration of the thin metal needle into the mixture until it reached a depth of 5 mm. To measure the final setting time, invert the mold for the other face and use the hollow circular needle with a diameter of 5 mm. The determination of the final setting time was by observing the penetration of the hollow needle of 0.5 mm. Figure 1 shows the Vicat apparatus for measuring geopolymer binder sitting time.

Fig. 1.
Fig. 1.

Vicat apparatus for the measurement of geopolymer binder test (Source: Authors' photo)

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

Scanning Electron Microscope (SEM) was employed to examine the microstructure and analyze the predominant elemental composition of the geopolymer binder. The Thermo Helios G4-PFIB CXe Dual scanning electron microscope, equipped with a Bruker microprobe and operated at a voltage of 20 kV, was utilized for this purpose. Before SEM imaging, the fractured samples underwent a coating process with a layer of gold to enhance conductivity.

3 Results and discussion

3.1 Metakaolin characteristics

The effect of the calcination process on the phase transformation of kaolin as a crystal phase to metakaolin as an amorphous phase is shown in Fig. 2. Following calcination at 750 °C for 3 h, the kaolin initially contained 16 wt% of amorphous phases, which then increased to 74 wt%, resulting in the formation of metakaolin as it is shown in Table 4 detected by X-ray diffraction results. The findings of the ray fluorescence study, which was used to determine the composition of metakaolin, are presented in Table 5. Depicts the particle size distribution of metakaolin particles in Fig. 3, with an average size of 5.4 µm.

Fig. 2.
Fig. 2.

The X-ray pattern for the kaolin and transformation into metakaolin through the calcination process

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

Table 4.

X-ray results show the quantity of kaolin and metakaolin's crystalline and amorphous phases

PhasesKaolin (wt%)Metakaolin (wt%)
Quartz22.6826.00
Kaolinite61.320.00
Amorphous16.0074.00
SUM100.00100.00
Table 5.

Metakaolin composition

Oxide composition(wt%)Oxide composition(wt%)
SiO258.30CaO0.180
Al2O339.40Fe2O30.470
Na2O0.06P2O30.013
MgO0.33Other0.987
K2O0.26SUM100
Fig. 3.
Fig. 3.

Metakaolin particle size distribution

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

3.2 Geopolymer binder characteristics

The bulk density of the geopolymer binders in samples that were cured at two different temperatures and had different liquid-to-solid ratios were measured. The bulk density range of the binders cured at 60 °C for 24 h was 1.172–1.195 g cm−3, and that of the binders cured at room temperature was 1.213–1.264 g cm−3, as it is shown in Fig. 4. As the curing temperature increases, the binder density decreases due to increased moisture loss early during polymerization. It is necessary to prevent water loss before it is completely cured [16]. Note that the bulk density of the binders reduces with the liquid-to-solid ratio. The higher density was 1.264 g cm−3 for the sample with a liquid-to-solid 0.8 ratio and was cured at room temperature. When the ratio of liquid to solid in geopolymers is higher, holes appear, particles are not packed tightly enough, the volume shrinks more, and the porosity increases. All these factors lead to a notable reduction in the binder's density [17].

Fig. 4.
Fig. 4.

Bulk density of geopolymer binders with different liquid-to-solid rates cured at two different temperatures

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

The compressive strength of the geopolymer binders cured for 28 days is presented in Fig. 5. The selected curing temperature of the geopolymer depended on raw materials for the fly ash-based geopolymer needs a curing temperature of more than 60 °C to get higher compressive strength [18]. In this work, the metakaolin-based geopolymer gave maximum compressive strength for samples cured at room temperature by adjusting the raw materials ratio and kaolin calcination temperature depending on previous works [12] The compressive strength range of the binders cured at 60 °C for 24 h (one day) and 27 days at room temperature was 16.52–17.91 MPa, and that of the binders cured at room temperature for 28 days was 17.01–19.12 MPa. The compressive strength of the binders was influenced by the ratios of liquid to solid components. The highest strength recorded was 19.12 MPa, observed in samples with a liquid-to-solid ratio of 0.8, cured at room temperature. Mainly, increasing the solid content in geopolymer binders leads to improving the mixture by good packing, enhanced chemical reaction, and reduced porosity, all of which factor in improving compressive strength. Depending on previous work, it was found to reduce compressive strength and poor workability when the liquid-to-solid ratio was less than 0.4 because the activation solution amount would be insufficient for the completed polymerization process [19].

Fig. 5.
Fig. 5.

Compressive strength of geopolymer binders with different liquid-to-solid rates cured at two different temperatures

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

The setting times both initial and final were measured for geopolymer binder cured at room temperature with different liquid-to-solid ratios as it is shown in Fig. 6. The initial setting denotes the duration required for the binder to transition from a liquid to a solid state following the mixing of the powder with an activator solution. While the final setting time indicates the period needed for the binder to attain hardening. It was found setting time for geopolymer binder decreases as the liquid-solid ratio decreases. The lower setting time was recorded at 288 min for the initial setting time and 358 min for the final setting for the geopolymer binder with a 0.8 liquid-to-solid ratio due to the Increased mixture fluidity leading to delayed formation of geopolymer gel [20]. The standard setting times of cement: the initial setting time should be more than 45 min and the final setting should be less than 390 min.

Fig. 6.
Fig. 6.

Setting time of geopolymer binders with different liquid-to-solid rates cured at room temperature

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

Regarding this matter, the sample with a liquid-to-solid ratio of 0.8 underwent solidification within the specified standard setting time limit. This is one of the metakaolin-based geopolymers advantages, it solidification at room temperature more rapidly than fly ash-based geopolymers [21]. The ultimate final setting time of fly ash-derived geopolymer solidifying at room temperature is approximately 1800 min [22].

One of the geopolymer binders advantages is that it has lower thermal conductivity than cement due to the absence of calcium hydroxide, which is mainly a contributor to the high thermal conductivity value of cementitious materials [23]. Figure 7 presented the thermal conductivity values of geopolymer binders, which were in the range of 0.28–0.49 W m−1 K for samples cured at room temperature with different liquid-to-solid ratios [12]. As the ratio of liquid to solid in a geopolymer binder increases, the thermal conductivity of the material reduces because of the decreased bulk density of the mixture. Denser materials generally have a greater thermal conductivity rating because their atoms and molecules are more closely packed, allowing for active heat transfer.

Fig. 7.
Fig. 7.

Thermal conductivity of geopolymer binders with different liquid-to-solid rates cured at room temperature

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

Figure 8 illustrates the microstructural composition of the geopolymer binder made using two liquid-to-solid ratios: 1.1 and 0.8 cured at room temperature the microstructure of the two samples displayed metakaolin unreacted and some microcracks in the gel matrix. In a sample with a lower liquid-to-solid ratio of 0.8, the resultant gel exhibited a comparatively denser and more uniformly structured composition, characterized by reduced pore size. Conversely, in samples with a ratio of 1.1, geopolymer specimens displayed heightened occurrences of cracks and larger pores. Higher liquid-to-solid ratios in geopolymer binder formulations typically result in increased porosity. This phenomenon occurs because a greater amount of water is present, which facilitates the formation of voids within the binder matrix [17]. As a result, the overall porosity of the geopolymer tends to rise, potentially impacting properties such as strength, durability, and permeability.

Fig. 8.
Fig. 8.

Electron microscopic images of geopolymer binders with different liquid to solid rates at magnifications 500X harder at room temperature (GP: Geopolymer gel, MC: Micro crack, MK: metakaolin)

Citation: Pollack Periodica 20, 1; 10.1556/606.2024.01141

4 Conclusions

This article studied the effects of curing temperature and liquid-to-solid ratio on metakaolin-based geopolymer binders. The curing temperature affects the compressive strength and bulk density of the geopolymer binder; the samples cured at room temperature have higher values. The solid and liquid ratio effect increases the bulk density, compressive strength, and thermal conductivity while reducing the liquid-to-solid ratio. As the liquid-to-solid ratio rises, the hardening times increase because of the augmented fluid content, necessitating a longer duration for complete hardening. The sample with the lower value of liquid-to-solid ratio 0.8 cured at room temperature achieved a maximum compressive strength of 19.12 MPa with lower setting times, an initial setting time of 288 min, and a final setting time of 358 min respectively.

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  • [1]

    G. L. Thankam, T. R. Neelakantan, and S. C. Gnanaraj, “Effect on the properties of fresh and hardened concrete made using fly ash geopolymer sand,” Int. Rev. Appl. Sci. Eng., vol. 12, no. 2, pp. 176182, 2021.

    • Search Google Scholar
    • Export Citation
  • [2]

    M. Osfouri and A. Simon, “Study on the thermal conductivity and density of foam glass,” Pollack Period., vol. 18, no. 1, pp. 126131, 2023.

    • Search Google Scholar
    • Export Citation
  • [3]

    P. S. Deb, P. Nath, and P. K. Sarker, “The effects of ground granulated blast-furnace slag blending with fly ash and activator content on the workability and strength properties of geopolymer concrete cured at ambient temperature,” Mater. Des., vol. 62, pp. 3239, 2014.

    • Search Google Scholar
    • Export Citation
  • [4]

    A. S. S. K. Mohammed, A. Simon, and R. Géber, “Preparation and characterization of foam glass from soda lime silicate glass waste by using different dosages of limestone,” Multidiszciplináris tudományok, vol. 12, no. 4, pp. 189197, 2022.

    • Search Google Scholar
    • Export Citation
  • [5]

    J. Liu and C. Lv, “Durability of cellulosic-fiber-reinforced geopolymers: A review,” Molecules, vol. 27, no. 3, pp. 123, 2022.

  • [6]

    A. S. S. K. Mohammed, E. Kurovics, J. E. F. M. Ibrahim, M. Tihtih, A. Simon, and R. Géber, “Preparation of an aluminum titania/mullite composite from the raw materials alumina, titania and silica fume,” Revue des Composites et des Materiaux Avances, vol. 32, no. 5, pp. 223228, 2022.

    • Search Google Scholar
    • Export Citation
  • [7]

    G. F. Huseien, J. Mirza, M. Ismail, S. K. Ghoshal, and A. A. Hussein, “Geopolymer mortars as sustainable repair material: A comprehensive review,” Renew. Sustain. Energy Rev., vol. 80, pp. 5474, 2017.

    • Search Google Scholar
    • Export Citation
  • [8]

    S. Mabroum, S. Moukannaa, A. El Machi, Y. Taha, M. Benzaazoua, and R. Hakkou, “Mine wastes based geopolymers: A critical review,” Clean. Eng. Technol., vol. 1, 2020, Art no. 100014.

    • Search Google Scholar
    • Export Citation
  • [9]

    J. E. F. M. Ibrahim, M. Tihtih, E. Kurovics, E. I. Şahin, L. A. Gömze, and I. Kocserha, “Glass-ceramic foams produced from zeolite-poor rock (Tokaj),” Pollack Period, vol. 18, no. 1, pp. 119125, 2023.

    • Search Google Scholar
    • Export Citation
  • [10]

    N. A. Jaya, Y. M. Liew, C. Y. Heah, and M. M. A. B. Abdullah, “Effect of solid-to-liquid ratios on metakaolin geopolymers,” in 4th Electronic and Green Materials International Conference, Bandung, Indonesia, July 27–28, 2018, pp. 020099-1020099-5.

    • Search Google Scholar
    • Export Citation
  • [11]

    A. Lopes, S. Lopes, and I. Pinto, “Influence of curing temperature on the strength of a metakaolin-based geopolymer,” Materials, vol. 16, no. 23, 2023, Art no. 7460.

    • Search Google Scholar
    • Export Citation
  • [12]

    A. S. S. K. Mohammed, R. Géber, A. Simon, E. Kurovics, and A. Hamza, “Comparative study of metakaolin-based geopolymer characteristics utilizing different dosages of water glass in the activator solution,” Results Eng., vol. 20, 2023, Art no. 101469.

    • Search Google Scholar
    • Export Citation
  • [13]

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    L. Jamaludin, A. Rafiza, M. Mohd, V. Petrica, V. Andrei, Z. Shayfull, and A. Romisuhani, “Solid-to-liquid ratio influenced on adhesion strength of metakaolin geopolymer coating paste added photocatalyst materials,” Coatings, vol. 13, no. 2, 2023, Art no. 236.

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    A. A. Adam and X. X. X. Horianto, “The effect of temperature and duration of curing on the strength of fly ash based geopolymer mortar,” Proced. Eng., vol. 95, pp. 410414, 2014.

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Senior editors

Editor(s)-in-Chief: Iványi, Amália

Editor(s)-in-Chief: Iványi, Péter

 

Scientific Secretary

Miklós M. Iványi

Editorial Board

  • Bálint Bachmann (Institute of Architecture, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Jeno Balogh (Department of Civil Engineering Technology, Metropolitan State University of Denver, Denver, Colorado, USA)
  • Radu Bancila (Department of Geotechnical Engineering and Terrestrial Communications Ways, Faculty of Civil Engineering and Architecture, “Politehnica” University Timisoara, Romania)
  • Charalambos C. Baniotopolous (Department of Civil Engineering, Chair of Sustainable Energy Systems, Director of Resilience Centre, School of Engineering, University of Birmingham, U.K.)
  • Oszkar Biro (Graz University of Technology, Institute of Fundamentals and Theory in Electrical Engineering, Austria)
  • Ágnes Borsos (Institute of Architecture, Department of Interior, Applied and Creative Design, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Matteo Bruggi (Dipartimento di Ingegneria Civile e Ambientale, Politecnico di Milano, Italy)
  • Petra Bujňáková (Department of Structures and Bridges, Faculty of Civil Engineering, University of Žilina, Slovakia)
  • Anikó Borbála Csébfalvi (Department of Civil Engineering, Institute of Smart Technology and Engineering, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Mirjana S. Devetaković (Faculty of Architecture, University of Belgrade, Serbia)
  • Szabolcs Fischer (Department of Transport Infrastructure and Water Resources Engineering, Faculty of Architerture, Civil Engineering and Transport Sciences Széchenyi István University, Győr, Hungary)
  • Radomir Folic (Department of Civil Engineering, Faculty of Technical Sciences, University of Novi Sad Serbia)
  • Jana Frankovská (Department of Geotechnics, Faculty of Civil Engineering, Slovak University of Technology in Bratislava, Slovakia)
  • János Gyergyák (Department of Architecture and Urban Planning, Institute of Architecture, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Kay Hameyer (Chair in Electromagnetic Energy Conversion, Institute of Electrical Machines, Faculty of Electrical Engineering and Information Technology, RWTH Aachen University, Germany)
  • Elena Helerea (Dept. of Electrical Engineering and Applied Physics, Faculty of Electrical Engineering and Computer Science, Transilvania University of Brasov, Romania)
  • Ákos Hutter (Department of Architecture and Urban Planning, Institute of Architecture, Faculty of Engineering and Information Technolgy, University of Pécs, Hungary)
  • Károly Jármai (Institute of Energy and Chemical Machinery, Faculty of Mechanical Engineering and Informatics, University of Miskolc, Hungary)
  • Teuta Jashari-Kajtazi (Department of Architecture, Faculty of Civil Engineering and Architecture, University of Prishtina, Kosovo)
  • Róbert Kersner (Department of Technical Informatics, Institute of Information and Electrical Technology, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Rita Kiss  (Biomechanical Cooperation Center, Faculty of Mechanical Engineering, Budapest University of Technology and Economics, Budapest, Hungary)
  • István Kistelegdi  (Department of Building Structures and Energy Design, Institute of Architecture, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Stanislav Kmeť (President of University Science Park TECHNICOM, Technical University of Kosice, Slovakia)
  • Imre Kocsis  (Department of Basic Engineering Research, Faculty of Engineering, University of Debrecen, Hungary)
  • László T. Kóczy (Department of Information Sciences, Faculty of Mechanical Engineering, Informatics and Electrical Engineering, University of Győr, Hungary)
  • Dražan Kozak (Faculty of Mechanical Engineering, Josip Juraj Strossmayer University of Osijek, Croatia)
  • György L. Kovács (Department of Technical Informatics, Institute of Information and Electrical Technology, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Balázs Géza Kövesdi (Department of Structural Engineering, Faculty of Civil Engineering, Budapest University of Engineering and Economics, Budapest, Hungary)
  • Tomáš Krejčí (Department of Mechanics, Faculty of Civil Engineering, Czech Technical University in Prague, Czech Republic)
  • Jaroslav Kruis (Department of Mechanics, Faculty of Civil Engineering, Czech Technical University in Prague, Czech Republic)
  • Miklós Kuczmann (Department of Automations, Faculty of Mechanical Engineering, Informatics and Electrical Engineering, Széchenyi István University, Győr, Hungary)
  • Tibor Kukai (Department of Engineering Studies, Institute of Smart Technology and Engineering, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Maria Jesus Lamela-Rey (Departamento de Construcción e Ingeniería de Fabricación, University of Oviedo, Spain)
  • János Lógó  (Department of Structural Mechanics, Faculty of Civil Engineering, Budapest University of Technology and Economics, Hungary)
  • Carmen Mihaela Lungoci (Faculty of Electrical Engineering and Computer Science, Universitatea Transilvania Brasov, Romania)
  • Frédéric Magoulés (Department of Mathematics and Informatics for Complex Systems, Centrale Supélec, Université Paris Saclay, France)
  • Gabriella Medvegy (Department of Interior, Applied and Creative Design, Institute of Architecture, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Tamás Molnár (Department of Visual Studies, Institute of Architecture, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Ferenc Orbán (Department of Mechanical Engineering, Institute of Smart Technology and Engineering, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Zoltán Orbán (Department of Civil Engineering, Institute of Smart Technology and Engineering, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Dmitrii Rachinskii (Department of Mathematical Sciences, The University of Texas at Dallas, Texas, USA)
  • Chro Radha (Chro Ali Hamaradha) (Sulaimani Polytechnic University, Technical College of Engineering, Department of City Planning, Kurdistan Region, Iraq)
  • Maurizio Repetto (Department of Energy “Galileo Ferraris”, Politecnico di Torino, Italy)
  • Zoltán Sári (Department of Technical Informatics, Institute of Information and Electrical Technology, Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Grzegorz Sierpiński (Department of Transport Systems and Traffic Engineering, Faculty of Transport, Silesian University of Technology, Katowice, Poland)
  • Zoltán Siménfalvi (Institute of Energy and Chemical Machinery, Faculty of Mechanical Engineering and Informatics, University of Miskolc, Hungary)
  • Andrej Šoltész (Department of Hydrology, Faculty of Civil Engineering, Slovak University of Technology in Bratislava, Slovakia)
  • Zsolt Szabó (Faculty of Information Technology and Bionics, Pázmány Péter Catholic University, Hungary)
  • Mykola Sysyn (Chair of Planning and Design of Railway Infrastructure, Institute of Railway Systems and Public Transport, Technical University of Dresden, Germany)
  • András Timár (Faculty of Engineering and Information Technology, University of Pécs, Hungary)
  • Barry H. V. Topping (Heriot-Watt University, UK, Faculty of Engineering and Information Technology, University of Pécs, Hungary)

POLLACK PERIODICA
Pollack Mihály Faculty of Engineering
Institute: University of Pécs
Address: Boszorkány utca 2. H–7624 Pécs, Hungary
Phone/Fax: (36 72) 503 650

E-mail: peter.ivanyi@mik.pte.hu 

or amalia.ivanyi@mik.pte.hu

Indexing and Abstracting Services:

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2024  
Scopus  
CiteScore  
CiteScore rank  
SNIP  
Scimago  
SJR index 0.385
SJR Q rank Q3

2023  
Scopus  
CiteScore 1.5
CiteScore rank Q3 (Civil and Structural Engineering)
SNIP 0.849
Scimago  
SJR index 0.288
SJR Q rank Q3

Pollack Periodica
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Pollack Periodica
Language English
Size A4
Year of
Foundation
2006
Volumes
per Year
1
Issues
per Year
3
Founder Faculty of Engineering and Information Technology, University of Pécs
Founder's
Address
H–7624 Pécs, Hungary, Boszorkány utca 2.
Publisher Akadémiai Kiadó
Publisher's
Address
H-1117 Budapest, Hungary 1516 Budapest, PO Box 245.
Responsible
Publisher
Chief Executive Officer, Akadémiai Kiadó
ISSN 1788-1994 (Print)
ISSN 1788-3911 (Online)

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