Pub Date : 2025-07-29DOI: 10.1007/s12647-025-00842-w
Shihoko Kajiwara, Naomi Akiyama, Takahiro Tamaki
Respiratory rate is a critical parameter for activating rapid response systems. Given the limitations of existing respiratory rate measurement methods, we aimed to develop a simple, affordable, portable, non-contact, and automatic measurement device using commercially available optical components. We further verified its measurement accuracy through experiments involving a simulator and a volunteer. The proposed system consisted of a webcam with 10 infrared light-emitting diodes, a webcam arm stand, and a laptop. The system employed the law of light attenuation to assess changes in the distance between the camera and the body surface and then extracted depth information from two-dimensional images. In the simulator experiments, the Bland–Altman analysis revealed a bias of 0.167 between simulator settings and automatic system measurements, and 0.200 between simulator settings and visual measurements by a nurse. In the volunteer experiment, the bias between automatic system measurements and visual measurements by a nurse was 0.033. The results were satisfactory. The proposed method exhibits sufficient measurement accuracy for practical use in an individual with a stable respiratory state. Collectively, our findings suggest that the device could reduce observational burden on nurses and significantly improve recording rate of respiratory parameters.
{"title":"Development of a Non-contact Respiratory Rate Measurement Method Considering Introduction of Rapid Response Systems","authors":"Shihoko Kajiwara, Naomi Akiyama, Takahiro Tamaki","doi":"10.1007/s12647-025-00842-w","DOIUrl":"10.1007/s12647-025-00842-w","url":null,"abstract":"<div><p>Respiratory rate is a critical parameter for activating rapid response systems. Given the limitations of existing respiratory rate measurement methods, we aimed to develop a simple, affordable, portable, non-contact, and automatic measurement device using commercially available optical components. We further verified its measurement accuracy through experiments involving a simulator and a volunteer. The proposed system consisted of a webcam with 10 infrared light-emitting diodes, a webcam arm stand, and a laptop. The system employed the law of light attenuation to assess changes in the distance between the camera and the body surface and then extracted depth information from two-dimensional images. In the simulator experiments, the Bland–Altman analysis revealed a bias of 0.167 between simulator settings and automatic system measurements, and 0.200 between simulator settings and visual measurements by a nurse. In the volunteer experiment, the bias between automatic system measurements and visual measurements by a nurse was 0.033. The results were satisfactory. The proposed method exhibits sufficient measurement accuracy for practical use in an individual with a stable respiratory state. Collectively, our findings suggest that the device could reduce observational burden on nurses and significantly improve recording rate of respiratory parameters.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"619 - 627"},"PeriodicalIF":1.3,"publicationDate":"2025-07-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s12647-025-00842-w.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242699","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-26DOI: 10.1007/s12647-025-00832-y
Oleh Velychko, Valentyn Isaiev, Viktoriia Shvedova, Igor Pototskiy
This article discusses the relationship between three characteristics of the quality of a measurement result, namely traceability, uncertainty, and stability. The presented annual stability investigation is based on the assumption of high long-term stability of the planar multi-junction voltage thermal converter, with which the AC/DC transfer standard under study is compared. To evaluate the qualitative aspect of the reproduction of the AC voltage unit for further dissemination, the relationship between the uncertainty of measurements and the difference between two estimates, separated in time by 1 year, was analyzed. To predict the random displacement of the reproducible volt unit, the presence of long-term drift of the hypothetical average AC/DC voltage transfer difference was also analyzed. To guarantee the quality of the performed assessment, three criteria of mathematical statistics were applied in the analysis of the presence of displacement trends.
{"title":"AC/DC Transfer Features of Dissemination of Voltage Unit Including Long-Term Stability","authors":"Oleh Velychko, Valentyn Isaiev, Viktoriia Shvedova, Igor Pototskiy","doi":"10.1007/s12647-025-00832-y","DOIUrl":"10.1007/s12647-025-00832-y","url":null,"abstract":"<div><p>This article discusses the relationship between three characteristics of the quality of a measurement result, namely traceability, uncertainty, and stability. The presented annual stability investigation is based on the assumption of high long-term stability of the planar multi-junction voltage thermal converter, with which the AC/DC transfer standard under study is compared. To evaluate the qualitative aspect of the reproduction of the AC voltage unit for further dissemination, the relationship between the uncertainty of measurements and the difference between two estimates, separated in time by 1 year, was analyzed. To predict the random displacement of the reproducible volt unit, the presence of long-term drift of the hypothetical average AC/DC voltage transfer difference was also analyzed. To guarantee the quality of the performed assessment, three criteria of mathematical statistics were applied in the analysis of the presence of displacement trends.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"775 - 792"},"PeriodicalIF":1.3,"publicationDate":"2025-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242772","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-26DOI: 10.1007/s12647-025-00840-y
Dinesh K. Aswal, Anirudh Chandra
India's ambitious initiative, “Viksit Bharat” (Developed India) by 2047, aims to transform the nation into a technologically advanced, economically robust, and socially inclusive society. Education stands as a central pillar of this vision. To ensure that quality education is accessible, equitable, and affordable for all, the National Education Policy (NEP) was introduced by the government in 2020, serving as a critical policy framework within the broader “Viksit Bharat” vision. While the NEP provides a comprehensive roadmap for India’s educational transformation, a unified approach to ensure systemic quality and stakeholder integration is lacking. To fill this gap, this paper introduces the Aswal Model—a quality infrastructure-based framework originally developed for science and innovation—as a conceptual tool to analyse and amplify the NEP’s impact. Rooted in the Quadruple Helix model of academia, industry, government, and civil society, the Aswal Model emphasizes the foundational role of metrology and quality infrastructure systems (QIS) in mediating stakeholder interactions. Using thematic analysis and policy documents, the study demonstrates how QI elements such as standardization, accreditation, and conformity assessment align with NEP’s elements, including core focus areas—Early Childhood Care and Education, Higher Education, and Vocational Education. By embedding QI principles into India’s education policy, the paper offers a novel interdisciplinary pathway for strengthening educational governance and knowledge generation. The findings contribute to both policy and metrology discourse by extending the application of quality infrastructure frameworks to education, providing actionable insights for regulators, technocrats, and institutional leaders.
{"title":"Leveraging the Aswal Model to Understand and Amplify the Impact of India’s National Education Policy","authors":"Dinesh K. Aswal, Anirudh Chandra","doi":"10.1007/s12647-025-00840-y","DOIUrl":"10.1007/s12647-025-00840-y","url":null,"abstract":"<div><p>India's ambitious initiative, “Viksit Bharat” (Developed India) by 2047, aims to transform the nation into a technologically advanced, economically robust, and socially inclusive society. Education stands as a central pillar of this vision. To ensure that quality education is accessible, equitable, and affordable for all, the National Education Policy (NEP) was introduced by the government in 2020, serving as a critical policy framework within the broader “Viksit Bharat” vision. While the NEP provides a comprehensive roadmap for India’s educational transformation, a unified approach to ensure systemic quality and stakeholder integration is lacking. To fill this gap, this paper introduces the Aswal Model—a quality infrastructure-based framework originally developed for science and innovation—as a conceptual tool to analyse and amplify the NEP’s impact. Rooted in the Quadruple Helix model of academia, industry, government, and civil society, the Aswal Model emphasizes the foundational role of metrology and quality infrastructure systems (QIS) in mediating stakeholder interactions. Using thematic analysis and policy documents, the study demonstrates how QI elements such as standardization, accreditation, and conformity assessment align with NEP’s elements, including core focus areas—Early Childhood Care and Education, Higher Education, and Vocational Education. By embedding QI principles into India’s education policy, the paper offers a novel interdisciplinary pathway for strengthening educational governance and knowledge generation. The findings contribute to both policy and metrology discourse by extending the application of quality infrastructure frameworks to education, providing actionable insights for regulators, technocrats, and institutional leaders.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"793 - 807"},"PeriodicalIF":1.3,"publicationDate":"2025-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://link.springer.com/content/pdf/10.1007/s12647-025-00840-y.pdf","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242623","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
This work presents the development of a methodology and software interface for the measurement of liquid dielectric constant based on the equivalent capacitance model. This work also presents the design and development of a novel coaxial probe with a 3D-printed transmission environment. The proposed coaxial probe is capable of working in the broadband frequency range from 500 MHz to 8.5 GHz. This probe, along with the developed software, leads to an indigenous solution for measuring the real-time electromagnetic parameters (i.e., permittivity, conductivity, and loss tangent) of liquids in a broad band frequency range. The complete setup is tested with the measurements of dielectric values of liquid and then compared and reported with the outcome of a commercially available software package and the actual target data. The measured results are comparable with the values obtained from commercial software as well as with the target data. Further, the measurement uncertainty was estimated to find out the tolerance limit, which is as per the IEC/IEEE 62209–1528:2020 standard (below ± 5%). This work is performed for the measurement and evaluation of dielectric properties in the frequency range of mobile communication, which includes 2G, 3G, 4G, and VoLTE.
{"title":"Characterization of Liquid Dielectric Solution with 3D Printed Broadband Coaxial Transmission Line","authors":"Prachi Tyagi, Aijaz Ahmed, Asheesh Kumar Sharma, Satya Kesh Dubey","doi":"10.1007/s12647-025-00839-5","DOIUrl":"10.1007/s12647-025-00839-5","url":null,"abstract":"<div><p>This work presents the development of a methodology and software interface for the measurement of liquid dielectric constant based on the equivalent capacitance model. This work also presents the design and development of a novel coaxial probe with a 3D-printed transmission environment. The proposed coaxial probe is capable of working in the broadband frequency range from 500 MHz to 8.5 GHz. This probe, along with the developed software, leads to an indigenous solution for measuring the real-time electromagnetic parameters (i.e., permittivity, conductivity, and loss tangent) of liquids in a broad band frequency range. The complete setup is tested with the measurements of dielectric values of liquid and then compared and reported with the outcome of a commercially available software package and the actual target data. The measured results are comparable with the values obtained from commercial software as well as with the target data. Further, the measurement uncertainty was estimated to find out the tolerance limit, which is as per the IEC/IEEE 62209–1528:2020 standard (below ± 5%). This work is performed for the measurement and evaluation of dielectric properties in the frequency range of mobile communication, which includes 2G, 3G, 4G, and VoLTE.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"763 - 773"},"PeriodicalIF":1.3,"publicationDate":"2025-07-24","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242743","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-19DOI: 10.1007/s12647-025-00836-8
Kaweri Gambhir, Parag Sharma, A. G. Vedeshwar, Ranjana Mehrotra
Nonlinear optical phenomena and techniques challenge existing in-line metrology. In order to validate a wide range of classical and nonclassical photonic outcomes, it is now crucial to broaden the scope of metrological aspects which were initially confined to fundamental SI units. The conventional method to determine third-order nonlinear optical coefficients is Z-scan spectroscopy. Carbon Disulfide (CS2) is the most extensively used reference material for various nonlinear optical setups including Z-scan spectroscopy. However, variation in the incident laser beam’s pulse duration drastically alters the nonlinear optical response of CS2. Therefore, till date all the available literature quotes relative nonlinear optical coefficients of CS2 and a consensus over the absolute nonlinearity of the reference material itself is missing. In order to overcome this limitation, the present article employs the Law of Propagation of Uncertainties (LPU/GUM) to establish a generic model to assess the uncertainties involved in the nonlinear absorption coefficient and nonlinear refractive index in the standard CS2 solution using transmission mode Z-scan spectroscopy. This would not only help in expanding the bounds of nonlinear optical metrology but also permit assessment, comparison, and commercialization of the results obtained from different third-order nonlinear optical measurements.
非线性光学现象和技术对现有的在线计量提出了挑战。为了验证广泛的经典和非经典光子结果,现在至关重要的是扩大最初局限于基本SI单位的计量方面的范围。确定三阶非线性光学系数的传统方法是z扫描光谱法。二硫化碳(CS2)是各种非线性光学装置(包括z扫描光谱)最广泛使用的参考物质。然而,入射激光束脉冲持续时间的变化极大地改变了CS2的非线性光学响应。因此,迄今为止,所有可用的文献都引用了CS2的相对非线性光学系数,而对参考物质本身的绝对非线性缺乏共识。为了克服这一局限,本文采用不确定性传播定律(Law of Propagation of uncertainty, LPU/GUM)建立了一个通用模型,利用透射模式z扫描光谱法评估标准CS2溶液中非线性吸收系数和非线性折射率所涉及的不确定性。这不仅有助于扩大非线性光学测量的范围,而且还允许评估、比较和商业化从不同的三阶非线性光学测量中获得的结果。
{"title":"Uncertainty Analysis in Z-Scan Spectroscopy: A Systematic Approach for Budget Estimation","authors":"Kaweri Gambhir, Parag Sharma, A. G. Vedeshwar, Ranjana Mehrotra","doi":"10.1007/s12647-025-00836-8","DOIUrl":"10.1007/s12647-025-00836-8","url":null,"abstract":"<div><p>Nonlinear optical phenomena and techniques challenge existing in-line metrology. In order to validate a wide range of classical and nonclassical photonic outcomes, it is now crucial to broaden the scope of metrological aspects which were initially confined to fundamental SI units. The conventional method to determine third-order nonlinear optical coefficients is Z-scan spectroscopy. Carbon Disulfide (CS<sub>2</sub>) is the most extensively used reference material for various nonlinear optical setups including Z-scan spectroscopy. However, variation in the incident laser beam’s pulse duration drastically alters the nonlinear optical response of CS<sub>2</sub>. Therefore, till date all the available literature quotes relative nonlinear optical coefficients of CS<sub>2</sub> and a consensus over the absolute nonlinearity of the reference material itself is missing. In order to overcome this limitation, the present article employs the Law of Propagation of Uncertainties (LPU/GUM) to establish a generic model to assess the uncertainties involved in the nonlinear absorption coefficient and nonlinear refractive index in the standard CS<sub>2</sub> solution using transmission mode <i>Z</i>-scan spectroscopy. This would not only help in expanding the bounds of nonlinear optical metrology but also permit assessment, comparison, and commercialization of the results obtained from different third-order nonlinear optical measurements.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"751 - 761"},"PeriodicalIF":1.3,"publicationDate":"2025-07-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242750","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-18DOI: 10.1007/s12647-025-00834-w
S. D. Suherlan, N. D. AlDawood, I. S. AlSubaie, I. A. AlFaleh, R. O. AlNefaie, K. M. Ahmed
This study presents a verification method for Infrared Forehead Thermometer (IRFT) readings developed at the National Measurement and Calibration Center (NMCC) of the Saudi Standards, Metrology, and Quality Organization (SASO). Six IRFTs from two different models were tested at 38 °C, a temperature threshold for fever according to the World Health Organization (WHO). The IRFT readings were compared against reference radiance temperatures generated by a standard blackbody radiator commonly used for Infrared Ear Thermometer (IRET) calibration. The blackbody was maintained in a temperature-controlled water bath near 38 °C, with its true temperature monitored using a contact standard thermometer (Pt-100). The blackbody’s effective emissivity was calculated as 0.999874, closely matching the default emissivity setting (~ 1.0) of most IRFTs. Instead of using a radiation thermometer, radiance temperatures were calculated from the blackbody’s true temperature measurements using the Sakuma-Hattori Planck III function. When compared to reference radiance temperatures, the laboratory errors in IRFT readings ranged from − 0.20 to 0.09 °C. These values comply with the maximum permissible laboratory error (MPLE) of ± 0.3 °C specified in ASTM E1965-98:2016 for skin IR thermometers. However, when measurement uncertainty (± 0.16 °C) was considered, one IRFT (− 0.20 °C error) failed verification. This was likely due to dust or smudges on the inner lens, which are difficult to clean externally. Further studies are needed to compare and validate these findings using methodologies from other national laboratories.
{"title":"Verification of Infrared Forehead Thermometer Readings Using a Blackbody Radiator at NMCC-SASO","authors":"S. D. Suherlan, N. D. AlDawood, I. S. AlSubaie, I. A. AlFaleh, R. O. AlNefaie, K. M. Ahmed","doi":"10.1007/s12647-025-00834-w","DOIUrl":"10.1007/s12647-025-00834-w","url":null,"abstract":"<div><p>This study presents a verification method for Infrared Forehead Thermometer (IRFT) readings developed at the National Measurement and Calibration Center (NMCC) of the Saudi Standards, Metrology, and Quality Organization (SASO). Six IRFTs from two different models were tested at 38 °C, a temperature threshold for fever according to the World Health Organization (WHO). The IRFT readings were compared against reference radiance temperatures generated by a standard blackbody radiator commonly used for Infrared Ear Thermometer (IRET) calibration. The blackbody was maintained in a temperature-controlled water bath near 38 °C, with its true temperature monitored using a contact standard thermometer (Pt-100). The blackbody’s effective emissivity was calculated as 0.999874, closely matching the default emissivity setting (~ 1.0) of most IRFTs. Instead of using a radiation thermometer, radiance temperatures were calculated from the blackbody’s true temperature measurements using the Sakuma-Hattori Planck III function. When compared to reference radiance temperatures, the laboratory errors in IRFT readings ranged from − 0.20 to 0.09 °C. These values comply with the maximum permissible laboratory error (MPLE) of ± 0.3 °C specified in ASTM E1965-98:2016 for skin IR thermometers. However, when measurement uncertainty (± 0.16 °C) was considered, one IRFT (− 0.20 °C error) failed verification. This was likely due to dust or smudges on the inner lens, which are difficult to clean externally. Further studies are needed to compare and validate these findings using methodologies from other national laboratories.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"909 - 918"},"PeriodicalIF":1.3,"publicationDate":"2025-07-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242621","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Early and accurate fault diagnosis in rotating machinery is essential to prevent unplanned breakdowns, costly downtime, and safety risks. Conventional fault detection methods are usually based on contact sensors or sophisticated signal processing, which may be intricate, expensive, or unreliable in harsh industrial environments. To overcome these drawbacks, this work introduces an Extended-Adaptive Neuro-Fuzzy Inference System (E-ANFIS) approach for fault diagnosis in rotating machine components by utilizing infrared thermography data from the machine. The method is validated by developing a real-time experimental setup consisting of a motor-driven rotating system with key components, including a bearing, bearing housing, rotating shaft, and belt-pulley mechanism. This test uses a FLIR ONE PRO LT iOS Pro-Grade infrared thermography camera to take thermal images of these components when they work in different operating conditions. The system is configured to run for 16 continuous hours, first under healthy conditions, where recorded temperature includes (47^circ text{C }) for a healthy bearing, (49.5^circ text{C }) for a scratched bearing, (51^circ text{C}) for a healthy V-belt, and (45^circ{rm C}) for an aligned shaft. Therafter, the system is then tested under fault conditions, where a broken ball bearing reaches (65.5^circ text{C }), a cracked outer ring (63^circ text{C }) , a loose V-belt (68.5^circ text{C }) , and a misaligned shaft (67^circ text{C }). The method is validated by using five performance parameters, namely accuracy, sensitivity, precision, Jaccard Similarity Index (JSI), and Dice Similarity Index (DSI). The proposed E-ANFIS model achieves an accuracy of 96.19, 94.29 sensitivity, 99.91% JSI, and 97.02% DSI, proving its effectiveness as a non-contact, real-time defect detection method. Additionally, the proposed method is compared with four existing defect detection methods, namely, Conventional ANFIS, Linear Transformation, and Improved Hyper Smoothing based Local Binary Pattern (LTIHLBP), Fuzzy-integrated Local Binary Pattern (Fuzzy-ILBP), and Modified Local Binary Pattern (MANN) method. Although, the accuracy parameter from E-ANFIS is 96.19%, which is lower in comparison to LTIHLBP, Fuzzy-ILBP, and MANN approaches. However, E-ANFIS outperforms all above methods in terms of sensitivity, precision, JSI, and DSI.
在旋转机械中,早期和准确的故障诊断对于防止意外故障,昂贵的停机时间和安全风险至关重要。传统的故障检测方法通常基于接触式传感器或复杂的信号处理,在恶劣的工业环境中,这些方法可能复杂、昂贵或不可靠。为了克服这些缺点,本工作引入了一种扩展自适应神经模糊推理系统(E-ANFIS)方法,利用机器的红外热成像数据对旋转机械部件进行故障诊断。通过建立一个由电机驱动的旋转系统组成的实时实验装置,验证了该方法的有效性,该系统包括轴承、轴承壳、转轴和皮带轮机构等关键部件。本测试使用FLIR ONE PRO LT iOS PRO级红外热像仪拍摄这些组件在不同操作条件下工作时的热图像。系统配置为连续运行16小时,首先在健康条件下,记录的温度包括:健康轴承(47^circ text{C }),划伤轴承(49.5^circ text{C }),健康v带(51^circ text{C}),对齐轴(45^circ{rm C})。然后,在故障条件下对系统进行测试,其中球轴承损坏(65.5^circ text{C }),外圈破裂(63^circ text{C }), v形带松动(68.5^circ text{C }),轴不对准(67^circ text{C })。通过准确性、灵敏度、精密度、Jaccard Similarity Index (JSI)和Dice Similarity Index (DSI) 5个性能参数对方法进行了验证。所提出的E-ANFIS模型准确率为96.19,灵敏度为94.29,99.91% JSI, and 97.02% DSI, proving its effectiveness as a non-contact, real-time defect detection method. Additionally, the proposed method is compared with four existing defect detection methods, namely, Conventional ANFIS, Linear Transformation, and Improved Hyper Smoothing based Local Binary Pattern (LTIHLBP), Fuzzy-integrated Local Binary Pattern (Fuzzy-ILBP), and Modified Local Binary Pattern (MANN) method. Although, the accuracy parameter from E-ANFIS is 96.19%, which is lower in comparison to LTIHLBP, Fuzzy-ILBP, and MANN approaches. However, E-ANFIS outperforms all above methods in terms of sensitivity, precision, JSI, and DSI.
{"title":"The Fault Diagnosis of Different Rotating Machine Elements by Using Infrared Thermography Images and Extended Adaptive Neuro-Fuzzy Inference System: An Experimental Evaluation","authors":"Ekta Yadav, Viveak Kumar Chawla, Surjit Angra, Sanjay Yadav","doi":"10.1007/s12647-025-00838-6","DOIUrl":"10.1007/s12647-025-00838-6","url":null,"abstract":"<div><p>Early and accurate fault diagnosis in rotating machinery is essential to prevent unplanned breakdowns, costly downtime, and safety risks. Conventional fault detection methods are usually based on contact sensors or sophisticated signal processing, which may be intricate, expensive, or unreliable in harsh industrial environments. To overcome these drawbacks, this work introduces an Extended-Adaptive Neuro-Fuzzy Inference System (E-ANFIS) approach for fault diagnosis in rotating machine components by utilizing infrared thermography data from the machine. The method is validated by developing a real-time experimental setup consisting of a motor-driven rotating system with key components, including a bearing, bearing housing, rotating shaft, and belt-pulley mechanism. This test uses a FLIR ONE PRO LT iOS Pro-Grade infrared thermography camera to take thermal images of these components when they work in different operating conditions. The system is configured to run for 16 continuous hours, first under healthy conditions, where recorded temperature includes <span>(47^circ text{C })</span> for a healthy bearing, <span>(49.5^circ text{C })</span> for a scratched bearing, <span>(51^circ text{C})</span> for a healthy V-belt, and <span>(45^circ{rm C})</span> for an aligned shaft. Therafter, the system is then tested under fault conditions, where a broken ball bearing reaches <span>(65.5^circ text{C })</span>, a cracked outer ring <span>(63^circ text{C })</span> , a loose V-belt <span>(68.5^circ text{C })</span> , and a misaligned shaft <span>(67^circ text{C })</span>. The method is validated by using five performance parameters, namely accuracy, sensitivity, precision, Jaccard Similarity Index (JSI), and Dice Similarity Index (DSI). The proposed E-ANFIS model achieves an accuracy of 96.19, 94.29 sensitivity, 99.91% JSI, and 97.02% DSI, proving its effectiveness as a non-contact, real-time defect detection method. Additionally, the proposed method is compared with four existing defect detection methods, namely, Conventional ANFIS, Linear Transformation, and Improved Hyper Smoothing based Local Binary Pattern (LTIHLBP), Fuzzy-integrated Local Binary Pattern (Fuzzy-ILBP), and Modified Local Binary Pattern (MANN) method. Although, the accuracy parameter from E-ANFIS is 96.19%, which is lower in comparison to LTIHLBP, Fuzzy-ILBP, and MANN approaches. However, E-ANFIS outperforms all above methods in terms of sensitivity, precision, JSI, and DSI.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"731 - 749"},"PeriodicalIF":1.3,"publicationDate":"2025-07-17","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242751","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-16DOI: 10.1007/s12647-025-00841-x
Hongtao Liu, Mingming Wei, Yandong Wang, Xi Gong, Shuai Ma, Ning Chen
Accurate wind speed measurement is of great significance for meteorological forecasting, industrial and agricultural production, and other fields, Metrological comparison serves as a crucial approach to ensure the consistency of wind speed instrument calibration. To evaluate the value-transfer ability of portable three-cup anemometers, the Hubei Meteorological Information and Technical Support Center took the lead in organizing a metrological comparison in 2024, involving 10 laboratories from 8 provinces and cities in the Yangtze River Economic Belt. This comparison adopted a petal-style transfer method, taking the YQY-QXM type portable three—cup anemometer as the transfer standard. Calibration experiments were carried out at multiple wind speed points ranging from 2 to 25 m/s in accordance with the JJG431-2014 protocol. The consistency of the results was evaluated using normalized deviation (En value). Experimental data demonstrated that the absolute value of En for all laboratories was less than 1, achieving a 100% satisfaction rate. The results indicated that the overall calibration capabilities of the laboratories met the requirements, and the value transfer was reliable. This comparison verified the comprehensive capabilities of the participating laboratories and provided an important basis for enhancing the standardization of wind speed measurement.
{"title":"Analysis of Measurement Comparison Results of Portable Three-Cup Anemometers","authors":"Hongtao Liu, Mingming Wei, Yandong Wang, Xi Gong, Shuai Ma, Ning Chen","doi":"10.1007/s12647-025-00841-x","DOIUrl":"10.1007/s12647-025-00841-x","url":null,"abstract":"<div><p>Accurate wind speed measurement is of great significance for meteorological forecasting, industrial and agricultural production, and other fields, Metrological comparison serves as a crucial approach to ensure the consistency of wind speed instrument calibration. To evaluate the value-transfer ability of portable three-cup anemometers, the Hubei Meteorological Information and Technical Support Center took the lead in organizing a metrological comparison in 2024, involving 10 laboratories from 8 provinces and cities in the Yangtze River Economic Belt. This comparison adopted a petal-style transfer method, taking the YQY-QXM type portable three—cup anemometer as the transfer standard. Calibration experiments were carried out at multiple wind speed points ranging from 2 to 25 m/s in accordance with the JJG431-2014 protocol. The consistency of the results was evaluated using normalized deviation (<i>E</i>n value). Experimental data demonstrated that the absolute value of <i>E</i>n for all laboratories was less than 1, achieving a 100% satisfaction rate. The results indicated that the overall calibration capabilities of the laboratories met the requirements, and the value transfer was reliable. This comparison verified the comprehensive capabilities of the participating laboratories and provided an important basis for enhancing the standardization of wind speed measurement.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 4","pages":"929 - 936"},"PeriodicalIF":1.3,"publicationDate":"2025-07-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145646348","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2025-07-08DOI: 10.1007/s12647-025-00833-x
Anup Kumar, Rajveer Singh Yaduvanshi
In this paper, a metrological analysis of GPS ceramic antenna using polarization conversion with anti-jamming features have been presented. Additionally, a novel polarization conversion technique using a metasurface is introduced to enhance the gain of a rectangular dielectric resonator antenna (RDRA). Two split-ring resonators (SRRs) interconnect provided anti-jamming capability. The structure consists of an RDRA made from a high DK ceramic material, which is excited by coaxial feeding. The proposed model has been fabricated and tested using a Vector Network Analyzer (VNA). The anti-jamming service features in the L1 band at 1.5742 GHz. Furthermore, a (SRR) cell integrated with a Z-shaped strip line is used to convert right-hand circular polarization (RHCP) to left-hand circular polarization (LHCP) as a novel feature. The gain enhancement is another novel feature, which is obtained due to polarization conversion. This study also emphasizes the significance of metrology in ensuring accurate measurement of key antenna parameters, including (S_{11}), gain, axial ratio and impedance. The ceramic DRA also contributes to the measurement and detection of environmental signals.
{"title":"A Metrological Analysis of GPS Ceramic Antenna Using Polarization Conversion with Anti-Jamming Features","authors":"Anup Kumar, Rajveer Singh Yaduvanshi","doi":"10.1007/s12647-025-00833-x","DOIUrl":"10.1007/s12647-025-00833-x","url":null,"abstract":"<div><p>In this paper, a metrological analysis of GPS ceramic antenna using polarization conversion with anti-jamming features have been presented. Additionally, a novel polarization conversion technique using a metasurface is introduced to enhance the gain of a rectangular dielectric resonator antenna (RDRA). Two split-ring resonators (SRRs) interconnect provided anti-jamming capability. The structure consists of an RDRA made from a high DK ceramic material, which is excited by coaxial feeding. The proposed model has been fabricated and tested using a Vector Network Analyzer (VNA). The anti-jamming service features in the L1 band at 1.5742 GHz. Furthermore, a (SRR) cell integrated with a Z-shaped strip line is used to convert right-hand circular polarization (RHCP) to left-hand circular polarization (LHCP) as a novel feature. The gain enhancement is another novel feature, which is obtained due to polarization conversion. This study also emphasizes the significance of metrology in ensuring accurate measurement of key antenna parameters, including <span>(S_{11})</span>, gain, axial ratio and impedance. The ceramic DRA also contributes to the measurement and detection of environmental signals.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 3","pages":"717 - 729"},"PeriodicalIF":1.3,"publicationDate":"2025-07-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145242749","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
The change of seawater temperature significantly affects the solubility of gas in it. With the increase of water temperature, the gas in sea water gradually precipitates to form bubbles, which may attach to the surface of the sensitive unit of the conductivity sensor, affecting the accuracy of the measurement results of the sensor. The effect of bubble on the measurement of conductivity sensor is discussed through a series of rising and cooling experiments in sea tank, and the effect is reduced by cooling method or specific debubling operation. The experimental results show that the bubble attachment will cause the measurement value of the conductivity sensor to be lower than the standard value, and the difference will gradually increase with the accumulation of bubbles on the surface of the sensitive unit. The offset of the electromagnetic induction conductivity sensor in the cooling measurement process of this study reached a maximum of − 0.0252mS/cm, and the offset in the heating measurement process reached a maximum of − 1.0761mS/cm. These offsets seriously affect the accuracy of the measurement data. The error of the electrode type conductivity sensor during the cooling measurement process was controlled within the range of ± 0.005mS/cm, and even during the heating measurement process, the maximum error was only − 0.0133mS/cm. In addition, the research shows that the electrode conductivity sensor performs better than the induction conductivity sensor in terms of anti-bubble interference. Therefore, the influence of bubbles on the measurement results of the conductivity sensor should be fully considered when Conductivity Temperature Depth (CTD) profiler measurement is carried out, and the operation of excluding bubbles and cooling measurement should be adopted to ensure the accuracy and reliability of the obtained data.
{"title":"Study on the Influence of Bubbles on the Measurement Results of CTD Conductivity Sensor","authors":"Qindan Liu, Yue Yin, Mengyang Liu, Aihua Xu, Yuzhen Guo, Lijun Zhang, Hua Zhang, Jiangyong Hu","doi":"10.1007/s12647-025-00837-7","DOIUrl":"10.1007/s12647-025-00837-7","url":null,"abstract":"<div><p>The change of seawater temperature significantly affects the solubility of gas in it. With the increase of water temperature, the gas in sea water gradually precipitates to form bubbles, which may attach to the surface of the sensitive unit of the conductivity sensor, affecting the accuracy of the measurement results of the sensor. The effect of bubble on the measurement of conductivity sensor is discussed through a series of rising and cooling experiments in sea tank, and the effect is reduced by cooling method or specific debubling operation. The experimental results show that the bubble attachment will cause the measurement value of the conductivity sensor to be lower than the standard value, and the difference will gradually increase with the accumulation of bubbles on the surface of the sensitive unit. The offset of the electromagnetic induction conductivity sensor in the cooling measurement process of this study reached a maximum of − 0.0252mS/cm, and the offset in the heating measurement process reached a maximum of − 1.0761mS/cm. These offsets seriously affect the accuracy of the measurement data. The error of the electrode type conductivity sensor during the cooling measurement process was controlled within the range of ± 0.005mS/cm, and even during the heating measurement process, the maximum error was only − 0.0133mS/cm. In addition, the research shows that the electrode conductivity sensor performs better than the induction conductivity sensor in terms of anti-bubble interference. Therefore, the influence of bubbles on the measurement results of the conductivity sensor should be fully considered when Conductivity Temperature Depth (CTD) profiler measurement is carried out, and the operation of excluding bubbles and cooling measurement should be adopted to ensure the accuracy and reliability of the obtained data.</p></div>","PeriodicalId":689,"journal":{"name":"MAPAN","volume":"40 4","pages":"1145 - 1153"},"PeriodicalIF":1.3,"publicationDate":"2025-07-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"145646271","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}