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32 pages, 943 KiB  
Review
Advancements in Sensor Fusion for Underwater SLAM: A Review on Enhanced Navigation and Environmental Perception
by Fomekong Fomekong Rachel Merveille, Baozhu Jia, Zhizun Xu and Bissih Fred
Sensors 2024, 24(23), 7490; https://doi.org/10.3390/s24237490 (registering DOI) - 24 Nov 2024
Abstract
Underwater simultaneous localization and mapping (SLAM) has significant challenges due to the complexities of underwater environments, marked by limited visibility, variable conditions, and restricted global positioning system (GPS) availability. This study provides a comprehensive analysis of sensor fusion techniques in underwater SLAM, highlighting [...] Read more.
Underwater simultaneous localization and mapping (SLAM) has significant challenges due to the complexities of underwater environments, marked by limited visibility, variable conditions, and restricted global positioning system (GPS) availability. This study provides a comprehensive analysis of sensor fusion techniques in underwater SLAM, highlighting the amalgamation of proprioceptive and exteroceptive sensors to improve UUV navigational accuracy and system resilience. Essential sensor applications, including inertial measurement units (IMUs), Doppler velocity logs (DVLs), cameras, sonar, and LiDAR (light detection and ranging), are examined for their contributions to navigation and perception. Fusion methodologies, such as Kalman filters, particle filters, and graph-based SLAM, are evaluated for their benefits, limitations, and computational demands. Additionally, innovative technologies like quantum sensors and AI-driven filtering techniques are examined for their potential to enhance SLAM precision and adaptability. Case studies demonstrate practical applications, analyzing the compromises between accuracy, computational requirements, and adaptability to environmental changes. This paper proceeds to emphasize future directions, stressing the need for advanced filtering and machine learning to address sensor drift, noise, and environmental unpredictability, hence improving autonomous underwater navigation through reliable sensor fusion. Full article
(This article belongs to the Section Navigation and Positioning)
16 pages, 3711 KiB  
Article
Optical Flow Sensor with Fluorescent-Conjugated Hyperelastic Pillar: A Biomimetic Approach
by Dongmin Seo, Seungmin Yoon, Jaemin Park, Sangwon Lee, Seungoh Han, Sung-Hoon Byun and Sangwoo Oh
Biomimetics 2024, 9(12), 721; https://doi.org/10.3390/biomimetics9120721 - 22 Nov 2024
Viewed by 281
Abstract
Although the Doppler velocity log is widely applied to measure underwater fluid flow, it requires high power and is inappropriate for measuring low flow velocity. This study proposes a fluid flow sensor that utilizes optical flow sensing. The proposed sensor mimics the neuromast [...] Read more.
Although the Doppler velocity log is widely applied to measure underwater fluid flow, it requires high power and is inappropriate for measuring low flow velocity. This study proposes a fluid flow sensor that utilizes optical flow sensing. The proposed sensor mimics the neuromast of a fish by attaching a phosphor to two pillar structures (A and B) produced using ethylene propylene diene monomer rubber. The optical signal emitted by the phosphor is measured using a camera. An experiment was conducted to apply an external force to the reactive part using a push–pull force gauge sensor to confirm the performance of the proposed sensor. The optical signal emitted by the phosphor was obtained using an image sensor, and a quantitative value was calculated using image analysis. A simulation environment was constructed to analyze the flow field and derive the relationship between the flow rate and velocity. The physical properties of the pillar were derived from hysteresis measurement results, and the error was minimized when pillar types A and B were utilized within the ranges of 0–0.1 N and 0–2 N, respectively. A difference in the elastic recovery characteristics was observed; this difference was linear based on the shape of the pillar, and improvement rates of 99.585% and 99.825% were achieved for types A and B, respectively. The proposed sensor can help obtain important information, such as precise flow velocity measurements in the near field, to precisely navigate underwater unmanned undersea vehicles and precisely control underwater robots after applying the technology to the surface of various underwater systems. Full article
(This article belongs to the Special Issue Biomimetics in Intelligent Sensor)
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Graphical abstract

Graphical abstract
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<p>Fluid flow measurement sensor based on optical sensing and mimicking the superficial neuromast in fish. A pillar-shaped structure is used to induce mechanical deformation in response to the fluid flow. Unlike how fish generate electrical signals through mechanical deformation of the neuromast, this sensor measures fluid flow by analyzing the fluorescent signal of the phosphor generated by the mechanical deformation (indicated by the green arrow) of the pillar.</p>
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<p>Designed form of pillar mechanically deformed by fluid flow in the boundary layer. Phosphor is used as a signal source. (<b>a</b>) The pillar is cylindrical with a hole of 1 mm in diameter. Two types of pillars, with outer diameters of 3 mm (type A) and 5 mm (type B), were manufactured and used in experiments. (<b>b</b>) Phosphor as a transparent bead made of glass and coated with red fluorescence on the surface of the hemisphere. The graph shows the excitation and emission wavelengths of phosphor. In this experiment, phosphor was excited with a wavelength of 470 <math display="inline"><semantics> <mrow> <mo>±</mo> </mrow> </semantics></math> 10 nm, and a bandpass filter was utilized with a wavelength of 607 <math display="inline"><semantics> <mrow> <mo>±</mo> </mrow> </semantics></math> 36 nm to selectively acquire the emitted fluorescence signal. (<b>c</b>) Attachment of phosphor to the pillar, showing the actual appearance of the type A pillar from the top, appearance after attaching the phosphor, and red fluorescence signal emitted from phosphor.</p>
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<p>Optical measurement system for measuring the fluorescence signal of phosphors and analysis method of images obtained from the system. (<b>a</b>) Optical measurement system and external force application system for experiment. A push–pull force gauge sensor allows for quantifying the applied external force and is attached to the XYZ stage for precise movement. The enlarged area in the orange box shows the setup of the phosphor-attached pillar and push–pull force gauge sensor. (<b>b</b>) Diagram of experimental setup. The USB camera selectively obtains the fluorescence signal emitted by the phosphor and converts it into an image. (<b>c</b>) Fluorescence image and its analysis. The brightness of the fluorescence image decreases with increasing external force on the pillar. For the analysis, some areas (yellow square box) are selected from the fluorescence image, and the intensity of the pixels in the corresponding area is averaged.</p>
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<p>Property value derivation and simulation setup environment for simulating hyperelastic substances. (<b>a</b>) Specimen model for tensile test. The dumbbell type three specimen follows the guidance of the KS standard test method, KS M 6518. (<b>b</b>) Stress intensity–strain ratio curve. As a result of the test, the hardness, strength, and elongation were 74, 15.2 MPa, and 270%, respectively. (<b>c</b>) Parameters of the Mooney–Rivlin model derived from the stress intensity–strain ratio curve employing the ninth model. (<b>d</b>) Shape of chamber in which the flow field was analyzed. Considering the symmetry of the target to be analyzed, the pillar was modeled as a half-symmetric structure.</p>
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<p>Flow field analysis of chamber using COMSOL Multiphysics and simulation of mechanical displacement of pillars in line with the applied flow velocity. (<b>a</b>) Simulation of flow field applied to chamber. (<b>b</b>) Simulation results of the flow field with pillars in the chamber. (<b>c</b>) Simulation results for converting applied flow rate into flow velocity, from which the linear function can be derived. It is possible to calculate the flow velocity on the pillar based on the flow rate setting in the chamber. (<b>d</b>) Simulation results of mechanical displacement of pillar in line with applied flow velocity. The pillar shape determines the pattern of the mechanical displacement. The image in the graph shows the mechanical deformation of the pillar when a flow velocity of 45 cm/s is applied to a type A pillar.</p>
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<p>Fluorescence signal analysis results of pillars in line with applied force. (<b>a</b>) Experimental results for type A pillars. (<b>b</b>) Experimental results for type B pillars. Each experiment was repeatedly performed with the same pillar three times. The fluorescence signal was measured while increasing the force applied to the pillar and decreasing the force. The conditions of the optical measurement system were adjusted to match the initial intensity of both types. The solid and dashed lines represent the signal changes for increases and decreases in the force, respectively.</p>
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<p>Quantitative analysis results of the applied force and resulting elastic recovery of pillars. (<b>a</b>) Experimental results for type A pillars. (<b>b</b>) Experimental results for type B pillars. Three pillars were manufactured, and each was utilized for three repeated experiments. The black square symbols represent the initial fluorescence intensity of the pillar, whereas the other symbols indicate the fluorescence intensity emitted after a constant force was applied to the pillar and then removed. The closer the measured fluorescence intensity is to the black square symbol, the greater is the elastic recovery property of the pillar.</p>
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<p>Method for correcting elastic recovery characteristics. (<b>a</b>) Intensities extracted from <a href="#biomimetics-09-00721-f007" class="html-fig">Figure 7</a>a. (<b>b</b>) Intensities extracted from <a href="#biomimetics-09-00721-f007" class="html-fig">Figure 7</a>b. Each intensity was extracted as the difference between the initial intensity and intensity after elastic recovery. (<b>c</b>) Corrected results for <a href="#biomimetics-09-00721-f006" class="html-fig">Figure 6</a>a. (<b>d</b>) Corrected results for <a href="#biomimetics-09-00721-f006" class="html-fig">Figure 6</a>b. After calibration, the overall area is reduced; however, the shape of the graph remains the same.</p>
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13 pages, 5059 KiB  
Article
Measurement of Ultra-High Speed by Optical Multistage Cascade Frequency Reduction Technology
by Heli Ma, Long Chen, Wei Gu, Cangli Liu, Longhuang Tang, Xing Jia, Tianjiong Tao, Shenggang Liu, Yongchao Chen, Xiang Wang, Jian Wu, Chengjun Li, Dameng Liu, Jidong Weng and Huan Liu
Appl. Sci. 2024, 14(23), 10771; https://doi.org/10.3390/app142310771 - 21 Nov 2024
Viewed by 431
Abstract
In order to reduce the frequency of high-frequency Doppler signal light, the electronic bandwidth of a data acquisition system is reduced. This paper mainly describes the principle and experimental verification results of optical multistage cascade frequency reduction technology. The bandwidth requirement of the [...] Read more.
In order to reduce the frequency of high-frequency Doppler signal light, the electronic bandwidth of a data acquisition system is reduced. This paper mainly describes the principle and experimental verification results of optical multistage cascade frequency reduction technology. The bandwidth requirement of the detector and the oscilloscope is reduced by the method of “relaying” the measured beat frequency signal between multiple electronic channels. Aiming to achieve the requirement of ultra-high speed measurement of 22 km/s, the requirement of the original signal frequency as high as 28 GHz electrical bandwidth is reduced to the acquisition and recording system with only 8 GHz bandwidth. A complete velocity profile of up to 11.47 km/s is measured on a three-stage light gas gun with velocity measurement accuracy of 1%. Full article
(This article belongs to the Special Issue Advanced Optical Measurement Techniques and Applications)
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Figure 1
<p>Schematic diagram of optical cascade frequency reduction optical path.</p>
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<p>Schematic diagram of the corresponding relationship between (<b>a</b>) velocity curve and (<b>b</b>) two-stage cascade frequency signal.</p>
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<p>Leakage optical power input to photoelectric conversion module under different gains.</p>
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<p>Frequency spectrum of mixed signal generated by leakage light and output light of (<b>a</b>) reference laser 1 and (<b>b</b>) reference laser 2.</p>
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<p>Interference signals in (<b>a</b>) virtual oscilloscope 1 and (<b>b</b>) virtual oscilloscope 2.</p>
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<p>(<b>a</b>) First-stage frequency conversion spectrum (tuned laser wavelength is 1550.176 nm); (<b>b</b>) first-stage frequency conversion spectrum (tuned laser wavelength is 1550.048 nm); (<b>c</b>) frequency spectrum of the second stage (tuned laser wavelength is 1550.048 nm).</p>
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<p>(<b>a</b>) First-stage two-dimensional frequency conversion spectrum; (<b>b</b>) two-dimensional frequency conversion spectrum of the second stage.</p>
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<p>Linear fitting results of optical beat frequency.</p>
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<p>Experimental principle and device of three-stage light gas gun.</p>
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<p>Spectrum diagram of two kinds of velocity measurement results: (<b>a</b>) DISAR, (<b>b</b>) first stage, and (<b>c</b>) second stage.</p>
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<p>Velocity profiles obtained from experiments.</p>
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16 pages, 11648 KiB  
Article
Analysis of Umbilical Artery Hemodynamics in Development of Intrauterine Growth Restriction Using Computational Fluid Dynamics with Doppler Ultrasound
by Xue Song, Jingying Wang, Ke Sun and Chunhian Lee
Bioengineering 2024, 11(11), 1169; https://doi.org/10.3390/bioengineering11111169 - 20 Nov 2024
Viewed by 289
Abstract
Intrauterine growth restriction (IUGR), the failure of the fetus to achieve his/her growth potential, is a common and complex problem in pregnancy. Clinically, IUGR is usually monitored using Doppler ultrasound of the umbilical artery (UA). The Doppler waveform is generally divided into three [...] Read more.
Intrauterine growth restriction (IUGR), the failure of the fetus to achieve his/her growth potential, is a common and complex problem in pregnancy. Clinically, IUGR is usually monitored using Doppler ultrasound of the umbilical artery (UA). The Doppler waveform is generally divided into three typical patterns in IUGR development, from normal blood flow (Normal), to the loss of end diastolic blood flow (LDBF), and even to the reversal of end diastolic blood flow (RDBF). Unfortunately, Doppler ultrasound hardly provides complete UA hemodynamics in detail, while the present in silico computational fluid dynamics (CFD) can provide this with the necessary ultrasound information. In this paper, CFD is employed to simulate the periodic UA blood flow for three typical states of IUGR, which shows comprehensive information on blood flow velocity, pressure, and wall shear stress (WSS). A new finding is the “hysteresis effect” between the UA blood flow velocity and pressure drop in which the former always changes after the latter by 0.1–0.2 times a cardiac cycle due to the unsteady flow. The degree of hysteresis is a promising indicator characterizing the evolution of IUGR. CFD successfully shows the hemodynamic details in different development situations of IUGR, and undoubtedly, its results would also help clinicians to further understand the relationship between the UA blood flow status and fetal growth restriction. Full article
(This article belongs to the Section Biosignal Processing)
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<p>The UA color and pulsed Doppler ultrasound spectrogram (<b>a</b>–<b>c</b>) and inlet velocity profile (<b>d</b>–<b>f</b>) for Normal (<b>a</b>,<b>d</b>), LDBF (<b>b</b>,<b>e</b>), and RDBF (<b>c</b>,<b>f</b>). The “PS” and “LD” moments represent the peak systolic and least diastolic, respectively. The flow time (<span class="html-italic">t</span>) is normalized by the time of one cardiac cycle (T). In Doppler ultrasound images, blue indicates blood flow traveling away from the transducer (negative Doppler shift), and red indicates blood flow traveling toward the transducer (positive Doppler shift).</p>
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<p>The UA model, showing only two spirals.</p>
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<p>Grids with long and short cross-sections: (<b>a</b>) long cross-section; (<b>b</b>) short cross-section.</p>
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<p>Time marching independence analysis. The flow time (<span class="html-italic">t</span>) is normalized by the time of one cardiac cycle (T).</p>
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<p>Non-Newtonian blood flow simulation validation (comparison with the theoretical solution proposed by Tevaboba et al. [<a href="#B46-bioengineering-11-01169" class="html-bibr">46</a>]).</p>
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<p>Streamlines of blood flow within the middle spiral of the UA at the peak systolic (PS (<b>b</b>–<b>d</b>)) and least diastolic (LD (<b>e</b>–<b>g</b>)) moments for Normal (<b>b</b>,<b>e</b>), LDBF (<b>c</b>,<b>f</b>), and RDBF (<b>d</b>,<b>g</b>) (in m/s): (<b>a</b>) The middle spiral of the UA is shown. The curves in the UA are the streamlines. The arrows represent the actual direction of flow.</p>
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<p>Blood flow velocity distribution in the middle cross-sections of the UA at the peak systolic (PS (<b>a</b>–<b>c</b>)) and least diastolic (LD (<b>d</b>–<b>f</b>)) moments for Normal (<b>a</b>,<b>d</b>), LDBF (<b>b</b>,<b>e</b>), and RDBF (<b>c</b>,<b>f</b>) (in m/s). The length of the arrows represents the size of the vortex diameter.</p>
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<p>Intensity of secondary flow in the middle cross-sections of the umbilical artery for Normal, LDBF, and RDBF during a whole cycle. The flow time (<span class="html-italic">t</span>) is normalized by the time of one cardiac cycle (T).</p>
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<p>The UA pressure at the peak systolic (PS (<b>a</b>–<b>c</b>)) and least diastolic (LD (<b>d</b>–<b>f</b>)) moments for Normal (<b>a</b>,<b>d</b>), LDBF (<b>b</b>,<b>e</b>), and RDBF (<b>c</b>,<b>f</b>) (in Pa). The arrows represent the actual direction of flow.</p>
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<p>The UA pressure distribution in the flow direction normalized by the UA diameter (<span class="html-italic">D</span>) for Normal, LDBF, and RDBF: (<b>a</b>) the peak systolic moment; (<b>b</b>) the least diastolic moment.</p>
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<p>Hysteresis effect between the blood flow velocity and pressure during one cardiac cycle: (<b>a</b>) Normal; (<b>b</b>) LDBF; and (<b>c</b>) RDBF. The flow time (<span class="html-italic">t</span>) is normalized by the time of one cardiac cycle (T). The shaded area represents the time periods during which positive flow is accompanied by a negative pressure drop, or the reverse flow is accompanied by a positive pressure drop.</p>
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<p>The WSS distribution on the UA wall at the peak systolic (PS (<b>a</b>–<b>c</b>)) and least diastolic (LD (<b>d</b>–<b>f</b>)) moments for Normal (<b>a</b>,<b>d</b>), LDBF (<b>b</b>,<b>e</b>), and RDBF (<b>c</b>,<b>f</b>) (in Pa). The arrows represent the actual direction of flow.</p>
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<p>The WSS circumferential distribution in the middle cross-sections of the UA at the peak systolic and least diastolic moments: (<b>a</b>) Normal; (<b>b</b>) LDBF; and (<b>c</b>) RDBF.</p>
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16 pages, 1219 KiB  
Article
The Usefulness of Carotid Artery Doppler Measurement as a Predictor of Early Death in Sepsis Patients Admitted to the Emergency Department
by Su-Il Kim, Yun-Deok Jang, Jae-Gu Ji, Yong-Seok Kim, In-Hye Kang, Seong-Ju Kim, Seong-Min Han and Min-Seok Choi
J. Clin. Med. 2024, 13(22), 6912; https://doi.org/10.3390/jcm13226912 - 16 Nov 2024
Viewed by 444
Abstract
Background: This study aims to verify whether the blood flow velocity and the diameter size, measured through intra-carotid artery Doppler measurements performed on sepsis patients visiting the emergency department, are useful as tools for predicting the risk of early death. Methods: As a [...] Read more.
Background: This study aims to verify whether the blood flow velocity and the diameter size, measured through intra-carotid artery Doppler measurements performed on sepsis patients visiting the emergency department, are useful as tools for predicting the risk of early death. Methods: As a prospective study, this research was performed on sepsis patients who visited a local emergency medical center from August 2021 to February 2023. The sepsis patients’ carotid artery was measured using Doppler imaging, and they were divided into patients measured for the size of systolic and diastolic mean blood flow velocity and diameter size: those measured for their qSOFA (quick sequential organ failure assessment) score and those measured using the SIRS (systemic inflammatory response syndrome) criteria. By measuring and comparing their mortality prediction accuracies, this study sought to verify the usefulness of blood flow velocity and the diameter size of the intra-carotid artery as tools to predict early death. Results: This study was conducted on 1026 patients, excluding 45 patients out of the total of 1071 patients. All sepsis patients were measured using systolic and diastolic blood flow velocity and diameter by Doppler imaging of the intra-carotid artery, assessed using qSOFA and evaluated using SIRS criteria. The results of the analysis performed to compare the mortality prediction accuracy were as follows. First, the hazard ratio (95% CI) of the intra-carotid artery was significant (p < 0.05), at 1.020 (1.004–1.036); the hazard ratio (95% CI) of qSOFA was significant (p < 0.05), at 3.871 (2.526–5.931); and the hazard ratio (95% CI) of SIRS showed no significant difference, at 1.002 (0.995–1.009). After 2 h of infusion treatment, the diameter size was 4.72 ± 1.23, showing a significant difference (p < 0.05). After 2 h of fluid treatment, the blood flow velocity was 101 m/s ± 21.12, which showed a significant difference (p < 0.05). Conclusions: Measuring the mean blood flow velocity in the intra-carotid arteries of sepsis patients who visit the emergency department is useful for predicting the risk of death at an early stage. And this study showed that Doppler measurement of the diameter size of the carotid artery significantly increased after performing fluid treatment after early recognition. Full article
(This article belongs to the Special Issue Emergency Ultrasound: State of the Art and Perspectives)
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<p>Algorithm of study flow. DOA: death on arrival; ED: emergency department; qSOFA: quick sequential organ failure; SIRS criteria: systemic inflammatory response syndrome criteria.</p>
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<p>Measurement device (ACUSON NX3 Elite. SIEMENS-Healthineers. Germany). (<b>A</b>) Arterial view: ultrasonography device used for the study. (<b>B</b>) Probe for measuring Doppler ultrasound.</p>
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<p>Measurement of ICA by placing a caliper on the level at which the gradient begins to rise at the end of diastole to the first peak of systole (early systolic peak).</p>
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<p>The receiver operating characteristic (ROC) curve of PSV in ICA. AUC (area under the curve) was 0.891 (95% confidence interval 0.826~0.956, <span class="html-italic">p</span> &lt; 0.001). PSV: Peak Systolic Velocity; ICA: intra-carotid artery.</p>
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35 pages, 8025 KiB  
Article
An ADCP Attitude Dynamic Errors Correction Method Based on Angular Velocity Tensor and Radius Vector Estimation
by Zhaowen Sun, Shuai Yao, Ning Gao and Ke Zhang
J. Mar. Sci. Eng. 2024, 12(11), 2018; https://doi.org/10.3390/jmse12112018 - 8 Nov 2024
Viewed by 367
Abstract
An acoustic Doppler current profiler (ADCP) installed on a platform produces rotational tangential velocity as a result of variations in the platform’s attitude, with both the tangential velocity and radial orientation varying between each pulse’s transmission and reception by the transducer. These factors [...] Read more.
An acoustic Doppler current profiler (ADCP) installed on a platform produces rotational tangential velocity as a result of variations in the platform’s attitude, with both the tangential velocity and radial orientation varying between each pulse’s transmission and reception by the transducer. These factors introduce errors into the measurements of vessel velocity and flow velocity. In this study, we address the errors induced by dynamic factors related to variations in attitude and propose an ADCP attitude dynamic error correction method based on angular velocity tensor and radius vector estimation. This method utilizes a low-sampling-rate inclinometer and compass data and estimates the angular velocity tensor based on a physical model of vessel motion combined with nonlinear least-squares estimation. The angular velocity tensor is then used to estimate the transducers’ radius vectors. Finally, the radius vectors are employed to correct the instantaneous tangential velocity within the measured velocities of the vessel and flow. To verify the effectiveness of the proposed method, field tests were conducted in a water pool. The results demonstrate that the proposed method surpasses the attitude static correction approach. In comparison with the ASC method, the average relative error in vessel velocity during free-swaying movement decreased by 20.94%, while the relative standard deviation of the error was reduced by 17.38%. Full article
(This article belongs to the Section Ocean Engineering)
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<p>The Earth coordinate system <math display="inline"><semantics> <mrow> <mi>O</mi> <mi>x</mi> <mi>y</mi> <mi>z</mi> </mrow> </semantics></math>, the vessel (body-fixed) coordinate system <math display="inline"><semantics> <mrow> <mi>G</mi> <msub> <mi>x</mi> <mi>b</mi> </msub> <msub> <mi>y</mi> <mi>b</mi> </msub> <msub> <mi>z</mi> <mi>b</mi> </msub> </mrow> </semantics></math>, and the transducer coordinate system <math display="inline"><semantics> <mrow> <mi>P</mi> <msub> <mi>x</mi> <mi>t</mi> </msub> <msub> <mi>y</mi> <mi>t</mi> </msub> <msub> <mi>z</mi> <mi>t</mi> </msub> </mrow> </semantics></math>.</p>
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<p>Schematic diagram of vessel swaying.</p>
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<p>Block diagram illustrating the principle of the proposed ADCP attitude dynamic error correction method, which is based on angular velocity tensor and radius vector estimation.</p>
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<p>Block diagram for the estimation of angular velocity tensor expression.</p>
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<p>Schematic diagram of the pool experiment.</p>
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<p>The RiverRay ADCP transducer.</p>
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<p>Pool experiment setup diagram: (<b>a</b>) approach for propelling the boat; (<b>b</b>) approach for generating roll motion in the boat.</p>
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<p>Fitting results of the roll, yaw, and pitch angles in the radius vector estimation measurement.</p>
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<p>Transducer radius vector diagram. (<b>a</b>) Three-dimensional view of the radius vectors. (<b>b</b>) Top-down view of the radius vectors.</p>
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<p>The estimated radius vectors are used to fit the BT (bottom-tracking) radial velocities in this measurement to validate the accuracy of the estimation.</p>
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<p>Fitting results of the roll, yaw, and pitch angles in Measurement 1.</p>
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<p>Measurement 1 vessel angular velocity magnitude and the ASC method vessel velocity.</p>
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<p>Vessel velocities in Measurement 1 obtained with the ASC method and the proposed method.</p>
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<p>Vessel velocity directions in Measurement 1 obtained with the ASC method and the proposed method.</p>
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<p>Fitting results of the roll, yaw, and pitch angles in Measurement 2.</p>
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<p>Measurement 2 vessel angular velocity magnitude and the ASC method vessel velocity.</p>
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<p>Vessel velocities in Measurement 2 obtained with the ASC method and the proposed method.</p>
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<p>Vessel velocity directions in Measurement 2 obtained with the ASC method and the proposed method.</p>
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25 pages, 9425 KiB  
Article
Characteristic Analysis of Vertical Tidal Profile Parameters at Tidal Current Energy Site
by Uk-Jae Lee, Dong-Hui Ko and Jin-Soon Park
J. Mar. Sci. Eng. 2024, 12(11), 1998; https://doi.org/10.3390/jmse12111998 - 6 Nov 2024
Viewed by 474
Abstract
Many mathematical models have been proposed to estimate vertical tidal current profiles. However, as previous studies have shown that tidal current energy sites have different characteristics in their vertical tidal current profiles, it is necessary to estimate the profiles from field-measured data for [...] Read more.
Many mathematical models have been proposed to estimate vertical tidal current profiles. However, as previous studies have shown that tidal current energy sites have different characteristics in their vertical tidal current profiles, it is necessary to estimate the profiles from field-measured data for practical purposes. In this study, we measured layered tidal currents over two months using an acoustic Doppler current profiler (ADCP) to analyze the characteristics of vertical tidal current profiles at the Jangjuk Strait, a candidate site for tidal current energy. As a result, the power law parameter α and bed roughness β were estimated as 4.51–12.41 and 0.38–0.42, respectively. Additionally, the maximum roughness length representing seabed roughness in the logarithmic profile was estimated as 0.221 m, and the estimated friction velocity was 0.038–0.194 m/s. Furthermore, a high correlation was observed between the depth-averaged tidal current velocity and friction velocities at all sites during flood and ebb tide conditions. A high correlation was also found between the bed roughness, roughness length, and power law exponent at relatively deeper sites. Tidal current energy sites display distinct characteristics compared to other sea areas. Therefore, it is essential to account for field conditions when conducting numerical modeling and design. Full article
(This article belongs to the Section Marine Energy)
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<p>Deployment locations of measurement instrumentation in Jangjuk Strait, Korea, and bathymetry results.</p>
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<p>Tidal level characteristics in Jangjuk Strait.</p>
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<p>Example of fitting results of vertical tidal profile using power law and logarithmic profile equation.</p>
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<p>Characteristics of all points at Jangjuk Strait. (<b>a</b>,<b>c</b>,<b>e</b>) Time series of tidal current velocity; (<b>b</b>,<b>d</b>,<b>f</b>) Tidal rose diagrams of direction.</p>
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<p>Power law parameter (<math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math>) and bed roughness (<math display="inline"><semantics> <mrow> <mi>β</mi> </mrow> </semantics></math>) during flood and ebb conditions at the three measurement points.</p>
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<p>Histogram and boxplot of the roughness length (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>z</mi> </mrow> <mrow> <mn>0</mn> </mrow> </msub> </mrow> </semantics></math>) during flood and ebb tides at the measurement points.</p>
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<p>Histogram and boxplot of the results of friction velocity (<math display="inline"><semantics> <mrow> <msub> <mrow> <mi>u</mi> </mrow> <mrow> <mi>*</mi> </mrow> </msub> </mrow> </semantics></math>) during flood and ebb tides at the measurement points.</p>
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<p>Profile parameter correlation matrix at the measurement points.</p>
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<p>Parameter estimation results according to flood/ebb condition and tidal current velocity range at all measurement points. (<b>a</b>) Power law parameter, <math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math>; (<b>b</b>) Friction velocity; (<b>c</b>) Roughness length. Yellow box depicts the flood condition at JSD-3 station, where the power law parameter <math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math> is estimated to be relatively low; gray color corresponds to <math display="inline"><semantics> <mrow> <mn>0.5</mn> <mo>≤</mo> <mi>U</mi> <mo>(</mo> <mi>z</mi> <mo>)</mo> <mo>&lt;</mo> <mn>1.0</mn> </mrow> </semantics></math>; red color corresponds to <math display="inline"><semantics> <mrow> <mn>1.0</mn> <mo>≤</mo> <mi>U</mi> <mo>(</mo> <mi>z</mi> <mo>)</mo> <mo>&lt;</mo> <mn>2.0</mn> </mrow> </semantics></math>; blue color corresponds to <math display="inline"><semantics> <mrow> <mn>2.0</mn> <mo>≤</mo> <mi>U</mi> <mo>(</mo> <mi>z</mi> <mo>)</mo> <mo>&lt;</mo> <mn>3.0</mn> </mrow> </semantics></math> (JSD-1&amp;2) or <math display="inline"><semantics> <mrow> <mi>U</mi> <mo>(</mo> <mi>z</mi> <mo>)</mo> <mo>≥</mo> <mn>2.0</mn> </mrow> </semantics></math> (JSD-3); cyan color corresponds to <math display="inline"><semantics> <mrow> <mi>U</mi> <mo>(</mo> <mi>z</mi> <mo>)</mo> <mo>≥</mo> <mn>3.0</mn> </mrow> </semantics></math>.</p>
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<p>Fitting results of tidal current profiles at all measurement points. Red and blue colors correspond to JSD-1, green and purple to JSD-2, magenta and turquoise to JSD-3; blue line denotes the JSD-1 depth, purple dashed line denotes the JSD-2 depth, and magenta dotted line denotes the JSD-3 depth.</p>
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9 pages, 1047 KiB  
Article
Cerebral Overperfusion Despite Reduced Cortical Metabolism Is Associated with Postoperative Delirium in Cardiac Surgery Patients: A Prospective Observational Study
by Marcus Thudium, Lara Braun, Annika Stroemer, Andreas Mayr, Jan Menzenbach, Thomas Saller, Martin Soehle, Evgeniya Kornilov and Tobias Hilbert
J. Clin. Med. 2024, 13(21), 6605; https://doi.org/10.3390/jcm13216605 - 3 Nov 2024
Viewed by 553
Abstract
Background: Decreased cerebral oximetry (rSO2) in cardiac surgery is associated with postoperative delirium (POD). However, interventions optimizing intraoperative rSO2 are inconclusive. Methods: In this prospective observational cohort study, the relationship between rSO2, middle cerebral artery blood [...] Read more.
Background: Decreased cerebral oximetry (rSO2) in cardiac surgery is associated with postoperative delirium (POD). However, interventions optimizing intraoperative rSO2 are inconclusive. Methods: In this prospective observational cohort study, the relationship between rSO2, middle cerebral artery blood flow velocity (MCAV), and processed EEG was assessed in cardiac surgery patients with and without POD. MCAV was continuously recorded by transcranial Doppler sonography (TCD), together with continuous rSO2 and bispectral index (BIS) monitoring. Cardiopulmonary bypass (CPB) flow rate was adjusted according to body surface area. The cohort was divided into the POD and control groups, according to the postoperative results of the confusion assessment method (CAM/CAM-ICU), the 4A’s test (4AT), and the Delirium Observation Scale (DOS). A mixed model analysis was performed for intraoperative raw data. The cerebral autoregulation index was calculated from TCD, rSO2, and arterial pressure values. Differences in impaired autoregulation were compared using the Mann–Whitney U test. Results: A total of 41 patients were included in this study. A total of 13 patients (36.11%) developed postoperative delirium. There were no significant differences in the baseline characteristics of patients with or without POD. Patients with POD had lower BIS values during CPB (adjusted mean difference −4.449 (95% CI [−7.978, −0.925])). RSO2 was not significantly reduced in POD, (adjusted mean difference: −5.320, 95% CI [−11.508, 0.874]). In contrast, MCAV was significantly increased in POD (10.655, 95% CI [0.491, 20.819]). The duration of cerebral autoregulation impairment did not differ significantly for TCD and cerebral oximetry-derived indices (p = 0.4528, p = 0.2715, respectively). Conclusions: Our results suggest that disturbed cerebral metabolism reflects a vulnerable brain which may be more susceptible to overperfusion during CPB, which can be seen in increased MCAV values. These phenomena occur irrespectively of cerebral autoregulation. Full article
(This article belongs to the Section Anesthesiology)
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<p>Study design and patient flowchart.</p>
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<p>General hemodynamic and cerebral parameters in patients with and without delirium. Pump flow: blood flow of cardiopulmonary bypass; BIS: bispectral index; CBFV: (middle) cerebral artery mean blood flow velocity; MAP: mean arterial pressure; POD: postoperative delirium; rSO<sub>2</sub>: regional cerebral oxygen saturation. Median (solid lines) and interquartile range (dashed lines); * <span class="html-italic">p</span> &lt; 0.05, n.s. = not significant (according to results from linear mixed effect models).</p>
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<p>Absolute time of cerebral autoregulation indices above 0.3, indicating impaired cerebral autoregulation. Indices are derived from moving linear correlations between MAP and cerebral parameters. CBFV: (middle) cerebral artery mean blood flow velocity; MAP: mean arterial pressure; POD: postoperative delirium; rSO<sub>2</sub>: regional cerebral oxygen saturation. Median (solid lines) and interquartile range (dashed lines); n.s. = not significant (according to results from Mann–Whitney U test).</p>
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22 pages, 6242 KiB  
Review
Noninvasive Tools to Predict Necrotizing Enterocolitis in Infants with Congenital Heart Diseases: A Narrative Review
by Laura Moschino, Silvia Guiducci, Miriam Duci, Leonardo Meggiolaro, Daniel Nardo, Luca Bonadies, Sabrina Salvadori, Giovanna Verlato and Eugenio Baraldi
Children 2024, 11(11), 1343; https://doi.org/10.3390/children11111343 - 31 Oct 2024
Viewed by 466
Abstract
Background: Necrotizing enterocolitis (NEC) is the most frightening gastrointestinal emergency in newborns. Despite being primarily a disease of premature infants, neonates with congenital heart disease (CHD) are at increased risk of development. Acute and chronic hemodynamic changes in this population may lead to [...] Read more.
Background: Necrotizing enterocolitis (NEC) is the most frightening gastrointestinal emergency in newborns. Despite being primarily a disease of premature infants, neonates with congenital heart disease (CHD) are at increased risk of development. Acute and chronic hemodynamic changes in this population may lead to mesenteric circulatory insufficiency. Objectives: In this narrative review, we describe monitoring tools, alone or in multimodal use, that may help in the early recognition of patients with CHD at major risk of NEC development. Methods: We focused on vital parameters, echocardiography, Doppler flowmetry, abdominal near-infrared spectroscopy (aNIRS), and abdominal ultrasound (aUS). Results: The number of studies on this topic is small and includes a wide range of patients’ ages and types of CHD. Peripheral oxygen saturation (SpO2) and certain echocardiographic indices (antegrade and retrograde velocity time integral, cardiac output, etc.) do not seem to differentiate infants with further onset of NEC from those not developing it. Hypotensive events, persistent diastolic flow reversal in the descending aorta, and low mesenteric oxygen saturation (rsSO2) measured by aNIRS appear to occur more frequently in infants who later develop NEC. aUS may be helpful in the diagnosis of cardiac NEC, potentially showing air contrast tracked to the right atrium in the presence of pneumatosis. Conclusions: This narrative review describes the current knowledge on bedside tools for the early prediction of cardiac NEC. Future research needs to further explore the use of easy-to-learn, reproducible instruments to assist patient status and monitor patient trends. Full article
(This article belongs to the Special Issue Infant and Early Childhood Nutrition)
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<p>Potential bedside, easy-to-perform, point-of-care tools that might be used to predict the risk of NEC onset in patients with CHDs and that have been explored in some studies enrolling neonates and infants with variable findings. Image by Freepik and Biorender. Abbreviations: aNIRS = abdominal near-infrared spectroscopy; aUS = abdominal ultrasound; CA = celiac artery; CO = cardiac output; FTOE = fraction of oxygen extraction; HR = heart rate; PI = pulsatility index; RI = resistive index; SCOR = splanchnic to cerebral oxygenation ratio; SMA = superior mesenteric artery; VTI = velocity-to-time integral.</p>
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<p>Anatomical and pathophysiological classification of CHDs. Cardiac anomalies are divided as follows: (1) CHD with increased pulmonary blood flow (septal defects without pulmonary obstruction and with L-t—R shunt; (2) CHD with decreased pulmonary flow (septal defects with pulmonary obstruction and with R-to-L shunt); (3) CHD with obstruction to blood progression and no septal defects (no shunt); (4) CHD so severe as to be incompatible with postnatal blood circulation (ductus-dependent CHD, parallel systemic and pulmonary circulations, anomalous connection/obstruction of the pulmonary veins). Adapted from Thiene G, Frescura C. Cardiovasc Pathol 2010 [<a href="#B36-children-11-01343" class="html-bibr">36</a>].</p>
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17 pages, 5119 KiB  
Article
Insights into Microscopic Characteristics of Gasoline and Ethanol Spray from a GDI Injector Under Injection Pressure up to 50 MPa
by Xiang Li, Xuewen Zhang, Tianya Zhang, Ce Ji, Peiyong Ni, Wanzhong Li, Yiqiang Pei, Zhijun Peng and Raouf Mobasheri
Sustainability 2024, 16(21), 9471; https://doi.org/10.3390/su16219471 - 31 Oct 2024
Viewed by 649
Abstract
Nowadays it has become particularly valuable to control the Particulate Matter (PM) emissions from the road transport sector, especially in vehicle powertrains with an Internal Combustion Engine (ICE). However, almost no publication has focused on a comparison of the microscopic characteristics of gasoline [...] Read more.
Nowadays it has become particularly valuable to control the Particulate Matter (PM) emissions from the road transport sector, especially in vehicle powertrains with an Internal Combustion Engine (ICE). However, almost no publication has focused on a comparison of the microscopic characteristics of gasoline and ethanol spray under injection pressure conditions of more than 30 MPa, except in the impingement process. By using a Phase Doppler Particles Analyser (PDPA) system, the microscopic characteristics of gasoline and ethanol spray from a Gasoline Direct Injection (GDI) injector under injection pressure (PI) up to 50 MPa was fully explored in this research. The experimental results demonstrate that under the same PI, the second peak of the probability (pd) curves of droplet normal velocity for gasoline is slightly higher than that of ethanol. Moreover, gasoline spray exceeds ethanol by about 5.4% regarding the average droplet tangential velocity at 50 mm of jet downstream. Compared to ethanol, the pd curve’s peak of droplet diameter at (0, 50) for gasoline is 1.3 percentage points higher on average, and the overall Sauter mean diameter of gasoline spray is slightly smaller. By increasing PI from 10 MPa to 50 MPa, pd of the regions of “100 ≤ Weber number (We) < 1000” and “We ≥ 1000” increases by about 23%, and the pd of large droplets over 20 μm shows a significant reduction. This research would provide novel insights into the deeper understanding of the comparison between gasoline and ethanol spray in microscopic characteristics under ultra-high PI. Additionally, this research would help provide a theoretical framework and practical strategies to reduce PM emissions from passenger vehicles, which would significantly contribute to the protection and sustainability of the environment. Full article
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<p>A schematic diagram of the experimental setup.</p>
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<p>The nozzle geometry and PDPA test points.</p>
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<p>The positive directions of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>N</mi> </mrow> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>T</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>p</mi> </mrow> <mrow> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math> of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>N</mi> </mrow> </msub> </mrow> </semantics></math> at (0, 50) under <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math> of 10 MPa and 50 MPa.</p>
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<p>The average <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>N</mi> </mrow> </msub> </mrow> </semantics></math> at (0, 50) as <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> progresses under different <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>The average <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>V</mi> </mrow> <mrow> <mi>T</mi> </mrow> </msub> </mrow> </semantics></math> at 50 mm of jet downstream under different <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>D</mi> </mrow> <mrow> <mi>S</mi> <mi>M</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> at (0, 50) as <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> progresses under different <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>p</mi> </mrow> <mrow> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math> of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>D</mi> </mrow> <mrow> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math> at (0, 50) under <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math> of 10 MPa and 20 MPa.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>p</mi> </mrow> <mrow> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math> of <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>D</mi> </mrow> <mrow> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math> at (0, 50) under <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math> of 30 MPa and 50 MPa.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>p</mi> </mrow> <mrow> <mi>d</mi> </mrow> </msub> </mrow> </semantics></math> of droplets at (0, 50) based on the classification of <math display="inline"><semantics> <mrow> <mi>W</mi> <mi>e</mi> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>D</mi> </mrow> <mrow> <mi>S</mi> <mi>M</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> at (−16, 50) as <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> progresses under different <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>D</mi> </mrow> <mrow> <mi>S</mi> <mi>M</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> at (16, 50) as <math display="inline"><semantics> <mrow> <mi>t</mi> </mrow> </semantics></math> progresses under different <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>D</mi> </mrow> <mrow> <mi>S</mi> <mi>M</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> at 50 mm of jet downstream under different <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p><math display="inline"><semantics> <mrow> <msub> <mrow> <mi>D</mi> </mrow> <mrow> <mi>S</mi> <mi>M</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> at (0, 50), (0, 60) and (0, 70) under different <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>P</mi> </mrow> <mrow> <mi>I</mi> </mrow> </msub> </mrow> </semantics></math>.</p>
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24 pages, 18779 KiB  
Article
An Improved Velocity-Aided Method for Smartphone Single-Frequency Code Positioning in Real-World Driving Scenarios
by Zhaowei Han, Xiaoming Wang, Jinglei Zhang, Shiji Xin, Qiuying Huang and Sizhe Shen
Remote Sens. 2024, 16(21), 3988; https://doi.org/10.3390/rs16213988 - 27 Oct 2024
Viewed by 721
Abstract
The availability of Global Navigation Satellite System (GNSS) raw observations in smartphones has driven research into low-cost GNSS solutions, especially in challenging urban environments, which have garnered significant attention from scholars in recent years. This study proposes an improved smartphone-based velocity-aided positioning method [...] Read more.
The availability of Global Navigation Satellite System (GNSS) raw observations in smartphones has driven research into low-cost GNSS solutions, especially in challenging urban environments, which have garnered significant attention from scholars in recent years. This study proposes an improved smartphone-based velocity-aided positioning method and conducts vehicle-mounted experiments in urban roads representing typical scenarios. The results show that when transitioning from low- to high-multipath environments, the number of visible satellites and carrier phase observations are highly sensitive to environmental factors, with frequent multipath effects. The introduction of robust pre-fit and post-fit residual algorithms has proven to be an effective quality control method. Additionally, using more refined observation models and appropriate parameter estimation algorithms led to a slight 6% improvement in velocity performance. The improved Kalman filter position estimation model (KFSPP-P) strategy, by incorporating velocity uncertainty into the state estimation process, overcomes the limitations of conventional velocity-aided smartphone positioning methods (KFSPP-V) in complex urban environments. In low-multipath environments, the accuracy of the KFSPP-P strategy is comparable to that of KFSPP-V, with an approximate 8% improvement in horizontal accuracy. However, in more challenging environments, such as tree-lined roads and urban environments, the KFSPP-P strategy shows significant improvements, particularly enhancing horizontal positioning accuracy by approximately 50%. These advancements demonstrate the potential of using smartphones to provide reliable positioning services in complex urban environments. Full article
(This article belongs to the Special Issue GNSS for Urban Transport Applications II)
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<p>Flowchart of the KFSPP-P processing procedure.</p>
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<p>Installation method of smartphones in the vehicle. From left to right are S21, CL8, and AD11. The dashcam is shown in the upper left corner.</p>
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<p>The experimental route trajectory is shown on the left, with blue, red, green, and yellow corresponding to open-sky road, suburban, tree-lined road, and urban environments, respectively. The right image depicts the actual environments corresponding to open-sky road (<b>A</b>), suburban (<b>B</b>), tree-lined road (<b>C</b>), and urban (<b>D</b>).</p>
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<p>The schematic diagram of the in-vehicle experimental setup. The lever arm of the smartphone to GNSS antenna is front = 2.78 m, right = 0.43 m, and up = 0.66 m; the lever arm of the smartphone to ISA100C is front = 3.48 m, right = 0.13 m, and up = 0.3 m.</p>
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<p>Number of satellites and PDOP values for the S21 on the test route. The color blocks located at the bottom of the image represent changes in environmental scenes: blue, red, green, and yellow correspond to open-sky road (A), suburban (B), tree-lined road (C), and urban (D), respectively.</p>
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<p>The number of code (red), Doppler (blue), and phase (green) observations recorded by the S21 smartphone along the experimental trajectory (<b>left</b>); the average number of each observation type in open-sky road (A), suburban (B), tree-lined road (C), and urban (D) environments (<b>right</b>).</p>
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<p>TDCMC statistics for GPS, Galileo, BDS, and GLONASS systems recorded by the S21 smartphone along the experimental trajectory, with different colors representing individual satellites.</p>
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<p>Distribution of post-fit residuals during Doppler-based velocity estimation using the S21, showing results without (<b>top</b>) and with (<b>bottom</b>) robust estimation algorithms applied, with different colors representing different satellites. Notably, the y-axis scale range is −4 to 4 m/s (<b>top</b>) and −0.4 to 0.4 m/s (<b>bottom</b>). The color blocks located at the bottom of the image represent changes in environmental scenes: blue, red, green, and yellow correspond to open-sky road (A), suburban (B), tree-lined road (C), and urban (D), respectively.</p>
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<p>Doppler velocity estimation errors for the S21, without (red) and with (blue) the robust estimation algorithm applied. The color blocks located at the bottom of the image represent changes in environmental scenes: blue, red, green, and yellow correspond to open-sky road (A), suburban (B), tree-lined road (C), and urban (D), respectively.</p>
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<p>Time series of velocity errors for the S21, CL8, and AD11 using LS-D, LS-T, LS-DT, KF-DT1, and KF-DT2 solutions. The red, blue, and green lines represent the velocity errors in the E, N, and U directions, respectively. Here, the velocity errors in the E and U directions are presented with y = 2.5 and y = −2.5 as the respective reference baselines for the vertical axis.</p>
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<p>Error plots for the S21, CL8, and AD11 in the E, N, and U directions using the SPP (red), KFSPP-V (blue), and KFSPP-P (green) solutions.</p>
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<p>Four typical environments, with real routes (<b>a</b>–<b>d</b>) corresponding to open-sky road (A—blue), suburban (B—red), tree-lined road (C—green), and urban (D—yellow).</p>
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<p>Positioning errors in the E, N, and U directions for the S21 smartphone across four routes (<b>a</b>–<b>d</b>). The red, blue, and green lines represent the SPP, KFSPP-V, and KFSPP-P solutions, respectively.</p>
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14 pages, 666 KiB  
Article
A Fuzzy-Logic-Based Approach for Eliminating Interference Lines in Micro Rain Radar (MRR-2)
by Kwonil Kim and GyuWon Lee
Remote Sens. 2024, 16(21), 3965; https://doi.org/10.3390/rs16213965 - 25 Oct 2024
Viewed by 505
Abstract
This research presents a novel fuzzy-logic-based algorithm aimed at detecting and removing interference lines from Micro Rain Radar (MRR-2) data. Interference lines, which are non-meteorological echoes with unknown origins, can severely obscure meteorological signals. Leveraging an understanding of interference line characteristics, such as [...] Read more.
This research presents a novel fuzzy-logic-based algorithm aimed at detecting and removing interference lines from Micro Rain Radar (MRR-2) data. Interference lines, which are non-meteorological echoes with unknown origins, can severely obscure meteorological signals. Leveraging an understanding of interference line characteristics, such as temporal continuity, we identified and utilized eight key variables to distinguish interference lines from meteorological signals. These variables include radar moments, Doppler spectrum peaks, and the spatial/temporal continuity of Doppler velocity. The algorithm was developed and validated using data from MRR installations at three sites (Seoul, Suwon, and Incheon) in South Korea, from June to September 2021–2023. While there is a slight tendency to eliminate some weak precipitation, results indicate that the algorithm effectively removes interference lines while preserving the majority of genuine precipitation signals, even in complex scenarios where both interference and precipitation signals are present. The developed software, written in Python 3 and available as open-source, outputs in NetCDF4 format, with customizable parameters for user flexibility. This tool offers a significant contribution to the field, facilitating the accurate interpretation of MRR-2 data contaminated by interference. Full article
(This article belongs to the Section Atmospheric Remote Sensing)
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<p>Time–height diagrams of MRR-2 data for the ICN site on 23 August 2021: (<b>a</b>) reflectivity, (<b>b</b>) Doppler velocity, and (<b>c</b>) spectrum width.</p>
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<p>A flow chart of the algorithm for detecting and removing interference lines in MRR-2 data.</p>
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<p>Histograms of precipitation samples and interference lines for each membership variable, with the constructed membership function depicted by the red line on the secondary y-axis.</p>
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<p>(<b>a</b>) Similar to <a href="#remotesensing-16-03965-f003" class="html-fig">Figure 3</a> but showing interference line and precipitation candidate samples obtained from (<b>b</b>) and the updated reflectivity membership function. Time–height diagrams for the ICN site MRR-2 on 26 August 2021: (<b>b</b>) Ze, (<b>c</b>) MF(Ze), and (<b>d</b>) updated MF(Ze).</p>
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<p>Time–height diagrams of reflectivity for the ICN and SWN sites. From top to bottom, each row corresponds to 9 August 2021 (ICN); 21 August 2021 (SWN); 28 August 2021 (ICN); and 13 July 2021 (ICN). Each column represents the data before (denoted as “Before”, corresponding to the data after the MK12 algorithm) and after applying the algorithm (denoted as “After”).</p>
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<p>CFADs of reflectivity for each major step of the algorithm. From top to bottom: CFADs after applying the MK12 algorithm, after performing interference lines’ removal (denoted as “Step 1”), after performing despeckling (denoted as “Step 2”), the difference between “Step 2” and “MK12” CFADs, and the difference between “Step 2” and “Step 1” CFADs. From left to right: ICN, SWN, and SEL sites, with all data except for the period used to construct the fuzzy logic algorithm.</p>
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<p>CFADS of (<b>a</b>,<b>b</b>) reflectivity, (<b>c</b>,<b>d</b>) Doppler velocity, and (<b>e</b>,<b>f</b>) spectrum width for ICN site. Similar to <a href="#remotesensing-16-03965-f005" class="html-fig">Figure 5</a>, each column represents the data before (denoted as “Before”, corresponding to the data after the MK12 algorithm) and after applying the algorithm (denoted as “After”).</p>
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9 pages, 1724 KiB  
Article
Time Interval Between Right Ventricular Early Diastolic Velocity by Tissue and Pulse Wave Doppler: An Index of Right Atrial Pressure in Pulmonary Hypertension Patients
by Costanza Natalia Julia Colombo, Francesco Corradi, Valentino Dammassa, Davide Colombo, Alessandro Fasolino, Mauro Acquaro, Susanna Price, Stefano Ghio and Guido Tavazzi
J. Clin. Med. 2024, 13(21), 6349; https://doi.org/10.3390/jcm13216349 - 23 Oct 2024
Viewed by 450
Abstract
Background: A reversal of time difference between the onset of early diastolic velocity (e’) during tissue Doppler imaging and the onset of mitral inflow (E) has been observed in cases of elevated left atrial pressure. Whether this interval (Te’-E) may be [...] Read more.
Background: A reversal of time difference between the onset of early diastolic velocity (e’) during tissue Doppler imaging and the onset of mitral inflow (E) has been observed in cases of elevated left atrial pressure. Whether this interval (Te’-E) may be useful to assess right atrial pressure has never been investigated, neither in healthy subjects nor in pulmonary hypertension patients. Methods: Right ventricular Te’-E was assessed in patients with pre-capillary pulmonary hypertension and compared with healthy volunteers who underwent comprehensive echocardiography examination. Te’-E is the difference between the interval from R wave at the superimposed electrocardiogram to the e’ wave during right ventricular tissue Doppler imaging and the interval from the R wave to transtricuspid E wave during pulsed wave Doppler imaging. Right atrial pressure was invasively measured in pulmonary hypertension patients. Results: Fifty-six patients were enrolled. Te’-E was prolonged in pulmonary hypertension subjects compared with healthy subjects (p < 0.001). Amongst the pulmonary hypertension patients, strong correlations were found between Te’-E and right atrial pressure (r = −0.885, p < 0.001), systolic pulmonary pressure (r = −0.85, p < 0.001) and the duration of tricuspid regurgitation (r = 0.72, p < 0.001). The area under the receiver operating characteristic curve of Te’-E in identifying right atrial pressure higher than 15 mm of mercury was 0.992 (sensitivity 100%, specificity 83%). Conclusions: In contrast to the left ventricle, there is a delay in the proto-diastolic filling in pulmonary hypertension patients, which correlates with the increase in systolic pulmonary arterial pressure, right atrial pressure, tricuspid regurgitation duration and restrictive diastolic pattern. Full article
(This article belongs to the Section Intensive Care)
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<p><b>Right ventricular R-e’ and R-E measurements.</b> (<b>A</b>) R-e’ wave time interval (red): time from R wave during superimposed ECG to the onset of e’ during RV tissue Doppler imaging; (<b>B</b>) R-E wave time interval (light blue): time from R wave during superimposed ECG to the onset of E during transtricuspid pulse wave Doppler imaging. T<sub>e’-E</sub> = [(R-e’ time interval) − (R-E time interval)]).</p>
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<p><b>Total isovolumic time echocardiographic measurement.</b> (<b>A</b>) RV total ejection time; (<b>B</b>) RV total filling time. Total isovolumic time is measured in seconds/minute.</p>
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<p>(<b>A</b>) Scatter plot showing correlation between T<sub>e’-E</sub> and RAP; (<b>B</b>) area under the receiver operating characteristic curve of the time interval between e’ and E in predicting right atrial pressure.</p>
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25 pages, 932 KiB  
Review
Positioning Systems for Unmanned Underwater Vehicles: A Comprehensive Review
by Christos Alexandris, Panagiotis Papageorgas and Dimitrios Piromalis
Appl. Sci. 2024, 14(21), 9671; https://doi.org/10.3390/app14219671 - 23 Oct 2024
Viewed by 1322
Abstract
Positioning systems are integral to Unmanned Underwater Vehicle (UUV) operation, enabling precise navigation and control in complex underwater environments. This paper comprehensively reviews the key technologies employed for UUV positioning, including acoustic systems, inertial navigation, Doppler velocity logs, and GPS when near the [...] Read more.
Positioning systems are integral to Unmanned Underwater Vehicle (UUV) operation, enabling precise navigation and control in complex underwater environments. This paper comprehensively reviews the key technologies employed for UUV positioning, including acoustic systems, inertial navigation, Doppler velocity logs, and GPS when near the surface. These systems are essential for seabed mapping, marine infrastructure inspection, and search and rescue operations. The review highlights recent technological advancements and examines the integration of these systems to enhance accuracy and operational efficiency. It also addresses ongoing challenges, such as communication constraints, environmental variability, and discrepancies between theoretical models and field applications. Future trends in positioning system development are discussed, with a focus on improving reliability and performance in diverse underwater conditions to support the expanding capabilities of UUVs across scientific, commercial, and rescue missions. Full article
(This article belongs to the Special Issue Application of Computer Science in Mobile Robots II)
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<p>Block diagram of an Unmanned Underwater Vehicle (UUV) control system.</p>
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9 pages, 253 KiB  
Article
A Study of the Relationship Between Objective Tests to Diagnose Erectile Dysfunction and Markers of Cardiovascular Disease
by Maurizio De Rocco Ponce, Claudia Fabiana Quintian Schwieters, Juliette Meziere, Josvany Rene Sanchez Curbelo, Guillem Abad Carratalá, Eden Troka, Lluis Bassas Arnau, Eduard Ruiz Castañé, Maria José Martinez Barcina and Osvaldo Rajmil
J. Clin. Med. 2024, 13(21), 6321; https://doi.org/10.3390/jcm13216321 - 23 Oct 2024
Viewed by 489
Abstract
Background: Erectile dysfunction (ED) can stem from various organic and functional causes but is often linked to vascular health and cardiovascular disease. Limited data exist on how cardiovascular disease markers correlate with objective ED tests like the Nocturnal Penile Tumescence and Rigidity (NPTR) [...] Read more.
Background: Erectile dysfunction (ED) can stem from various organic and functional causes but is often linked to vascular health and cardiovascular disease. Limited data exist on how cardiovascular disease markers correlate with objective ED tests like the Nocturnal Penile Tumescence and Rigidity (NPTR) test and Penile Color Doppler Ultrasound (PCDU). Methods: A prospective observational study was performed, and 58 men with ED were assessed using the International Index of Erectile Function-15 (IIEF-15), NPTR test, and PCDU. Peripheral vascular health was evaluated through carotid intima-media thickness (cIMT) and brachial flow-mediated dilation (FMD). Results: Out of the participants, 44 had normal NPTR results, while 14 had abnormal results. The group with abnormal NPTR results was significantly older and had higher rates of hypertension and diabetes. Although the IIEF-15 scores were similar between the two groups, those with abnormal NPTR results had a lower peak systolic velocity (PSV) and a higher prevalence of impaired PSV. Correlations between the IIEF, NPTR, PCDU, and peripheral vascular markers lost significance after the age adjustment. Conclusions: This study suggests that abnormal NPTR results, combined with cardiovascular risk factors, may signal vascular ED and generalized vasculopathy, highlighting the need for cardiovascular assessment. An accurate ED diagnosis should integrate clinical evaluation with multiple tests while considering aging as a key risk factor. Full article
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