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Cutolo A, Bernini R, Berruti GM, Breglio G, Bruno FA, Buontempo S, Catalano E, Consales M, Coscetta A, Cusano A, Cutolo MA, Di Palma P, Esposito F, Fienga F, Giordano M, Iele A, Iadicicco A, Irace A, Janneh M, Laudati A, Leone M, Maresca L, Marrazzo VR, Minardo A, Pisco M, Quero G, Riccio M, Srivastava A, Vaiano P, Zeni L, Campopiano S. Innovative Photonic Sensors for Safety and Security, Part II: Aerospace and Submarine Applications. SENSORS (BASEL, SWITZERLAND) 2023; 23:2417. [PMID: 36904622 PMCID: PMC10007474 DOI: 10.3390/s23052417] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 01/13/2023] [Revised: 02/08/2023] [Accepted: 02/15/2023] [Indexed: 06/18/2023]
Abstract
The employability of photonics technology in the modern era's highly demanding and sophisticated domain of aerospace and submarines has been an appealing challenge for the scientific communities. In this paper, we review our main results achieved so far on the use of optical fiber sensors for safety and security in innovative aerospace and submarine applications. In particular, recent results of in-field applications of optical fiber sensors in aircraft monitoring, from a weight and balance analysis to vehicle Structural Health Monitoring (SHM) and Landing Gear (LG) monitoring, are presented and discussed. Moreover, underwater fiber-optic hydrophones are presented from the design to marine application.
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Affiliation(s)
- Antonello Cutolo
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
| | - Romeo Bernini
- Istituto per il Rilevamento Elettromagnetico dell’Ambiente, Consiglio Nazionale delle Ricerche, Via Diocleziano 328, 81024 Napoli, Italy
| | - Gaia Maria Berruti
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Giovanni Breglio
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
- European Organization for Nuclear Research (CERN), CH-1211 Geneva, Switzerland
| | - Francesco Antonio Bruno
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Salvatore Buontempo
- European Organization for Nuclear Research (CERN), CH-1211 Geneva, Switzerland
- National Institute for Nuclear Physics (INFN), 80125 Napoli, Italy
| | - Ester Catalano
- Dipartimento di Ingegneria, Università della Campania Luigi Vanvitelli, Via Roma 29, 81031 Aversa, Italy
- Optosensing Ltd., Via Carlo de Marco 69, 80137 Napoli, Italy
| | - Marco Consales
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Agnese Coscetta
- Dipartimento di Ingegneria, Università della Campania Luigi Vanvitelli, Via Roma 29, 81031 Aversa, Italy
| | - Andrea Cusano
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Maria Alessandra Cutolo
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
| | - Pasquale Di Palma
- Dipartimento di Ingegneria, Università degli studi di Napoli Parthenope, Centro Direzionale Isola C4, 80143 Napoli, Italy
| | - Flavio Esposito
- Dipartimento di Ingegneria, Università degli studi di Napoli Parthenope, Centro Direzionale Isola C4, 80143 Napoli, Italy
| | - Francesco Fienga
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
- European Organization for Nuclear Research (CERN), CH-1211 Geneva, Switzerland
| | - Michele Giordano
- Istituto per i Polimeri, Compositi e Biomateriali Consiglio Nazionale delle Ricerche Via Enrico Fermi 1, 80055 Portici, Italy
| | - Antonio Iele
- CERICT SCARL, CNOS Center, Viale Traiano, Palazzo ex Poste, 82100 Benevento, Italy
| | - Agostino Iadicicco
- Dipartimento di Ingegneria, Università degli studi di Napoli Parthenope, Centro Direzionale Isola C4, 80143 Napoli, Italy
| | - Andrea Irace
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
| | - Mohammed Janneh
- CERICT SCARL, CNOS Center, Viale Traiano, Palazzo ex Poste, 82100 Benevento, Italy
| | | | - Marco Leone
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Luca Maresca
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
| | - Vincenzo Romano Marrazzo
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
- European Organization for Nuclear Research (CERN), CH-1211 Geneva, Switzerland
| | - Aldo Minardo
- Dipartimento di Ingegneria, Università della Campania Luigi Vanvitelli, Via Roma 29, 81031 Aversa, Italy
| | - Marco Pisco
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Giuseppe Quero
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Michele Riccio
- Dipartimento di Ingegneria Elettrica e delle Tecnologie dell’Informazione, Università degli studi di Napoli Federico II, Via Claudio 21, 80125 Napoli, Italy
| | - Anubhav Srivastava
- Dipartimento di Ingegneria, Università degli studi di Napoli Parthenope, Centro Direzionale Isola C4, 80143 Napoli, Italy
| | - Patrizio Vaiano
- Dipartimento di Ingegneria, Università degli Studi del Sannio, Corso Garibaldi, Palazzo Bosco Lucarelli, 82100 Benevento, Italy
| | - Luigi Zeni
- Dipartimento di Ingegneria, Università della Campania Luigi Vanvitelli, Via Roma 29, 81031 Aversa, Italy
- Optosensing Ltd., Via Carlo de Marco 69, 80137 Napoli, Italy
| | - Stefania Campopiano
- Dipartimento di Ingegneria, Università degli studi di Napoli Parthenope, Centro Direzionale Isola C4, 80143 Napoli, Italy
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Zhan J, Li H, Pan Q, Cheng Z, Li H, Fu B. Effect of Slag on the Strength and Shrinkage Properties of Metakaolin-Based Geopolymers. MATERIALS 2022; 15:ma15082944. [PMID: 35454637 PMCID: PMC9032675 DOI: 10.3390/ma15082944] [Citation(s) in RCA: 2] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 03/30/2022] [Revised: 04/13/2022] [Accepted: 04/14/2022] [Indexed: 12/04/2022]
Abstract
Metakaolin-based geopolymers possess excellent corrosion and high-temperature resistance, which are advantageous compared to ordinary Portland cement. The addition of slag in metakaolin-based geopolymers is a promising approach to improve their mechanical properties. Thus, this study investigated the effect of slag content on the strength and shrinkage properties of metakaolin-based geopolymers. Increasing the slag content and Na2O content was beneficial to the reaction of alkali-activated metakaolin-based geopolymers, thereby improving their compressive strength and density. After 56 days of aging, a maximum compressive strength of 86.1 MPa was achieved for a metakaolin-based geopolymer with a slag content of 50 mass%. When the Na2O content was 12%, the compressive strength of the metakaolin geopolymers with a slag content of 30% was 42.36% higher than those with a Na2O content of 8%. However, as the slag and alkali contents increased, the reaction rate of the metakaolin-based geopolymers increased, which significantly decreased the porosity, increased the shrinkage, and decreased the volumetric stability of the system. In this paper, in-depth study of the volume stability of alkali-activated metakaolin-based geopolymers plays an important role in further understanding, controlling, and utilizing the deformation behavior of geopolymers.
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Affiliation(s)
- Jianghuai Zhan
- College of Civil and Hydraulic Engineering, Ningxia University, Yinchuan 750021, China; (J.Z.); (H.L.)
| | - Hongbo Li
- College of Civil and Hydraulic Engineering, Ningxia University, Yinchuan 750021, China; (J.Z.); (H.L.)
| | - Qun Pan
- Chongqing Construction Science and Research Institute Co., Ltd., Chongqing 400060, China;
| | - Zhenyun Cheng
- School of Civil Engineering, North Minzu University, Yinchuan 750021, China;
| | - Huang Li
- China Construction Fifth Engineering Bureau Co., Ltd., Changsha 410011, China;
| | - Bo Fu
- School of Civil Engineering, North Minzu University, Yinchuan 750021, China;
- National Energy Group, Coal Chemical Industry Technology Research Institute, Ningxia Coal Industry Co., Ltd., Yinchuan 720021, China
- Correspondence:
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Use of a Piezoelectric Bender Element for the Determination of Initial and Final Setting Times of Metakaolin Geopolymer Pastes, with Applications to Laterite Soils. SENSORS 2022; 22:s22031267. [PMID: 35162012 PMCID: PMC8838400 DOI: 10.3390/s22031267] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 12/30/2021] [Revised: 01/27/2022] [Accepted: 02/01/2022] [Indexed: 11/17/2022]
Abstract
This study proposes the use of a non-destructive testing technique, based on piezoelectric bender element tests, to determine the initial and final setting times of metakaolin geopolymer pastes. (1) Background: Metakaolin geopolymer is a new eco-friendly building material that develops strength rapidly and is high in compressive strength. (2) Methods: The initial and the final setting times were investigated via bender element and Vicat needle tests. Metakaolin powder was prepared by treating kaolin at 0, 200, 800, 1000, and 1200 °C. All metakaolin powder samples were then mixed with geopolymer solution at different mixing ratios of 0.8:1.0, 1.0:1.0, 1.2:1.0, and 1.5:1.0. The geopolymer solution was prepared by adding 10 normal concentrations of sodium hydroxide (10 N NaOH) to sodium silicate (Na2SiO3) at various solution ratios of 1.0:1.0, 1.0:1.2, 1.0:1.5, 1.0:2.0, 1.2:1.0, 1.5:1.0 and 2.0:1.0. (3) Results: The optimum temperature for treating metakaolin is established at 1000 °C, with a mixing ratio between the metakaolin powder and the geopolymer solution of 1.0:1.0, as well as a solution ratio between NaOH and Na2SiO3 of 2.0:1.0. (4) Conclusions: The use of piezoelectric bender elements to determine the initial and final setting times of metakaolin geopolymer pastes is a useful method by which to detect geopolymerization by shear wave velocity in a real-time manner. Moreover, the penetration of the Vicat apparatus can confirm the setting times at specific intervals. The relationships between the shear wave velocity and the Vicat penetration appear to be linear, with an initial setting time of 168 m/s and a final setting time of 187 m/s. Finally, the optimum metakaolin geopolymer pastes are applied to improve laterite soils, as measured by CBR tests.
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