Keith A Wear, Christopher R Fury, Andre V Alvarenga
{"title":"针水听器的空间分辨率限制从0.5到20 MHz与经颅超声的意义。","authors":"Keith A Wear, Christopher R Fury, Andre V Alvarenga","doi":"10.1109/TUFFC.2025.3610361","DOIUrl":null,"url":null,"abstract":"<p><p>Hydrophone spatial resolution and spatial averaging effects are determined by the frequency-dependent effective sensitive element diameter d<sub>eff</sub>(f) rather than the geometrical sensitive element diameter d<sub>g</sub>. The objective of this work was to quantify average d<sub>eff</sub>(f) for needle hydrophones as a function of d<sub>g</sub> and f. Estimates of effective radii a<sub>eff</sub>(f) = d<sub>eff</sub>(f) / 2 were inferred from directivity measurements from 0.5 to 20 MHz on 16 needle hydrophones with d<sub>g</sub> = 2a<sub>g</sub> ranging from 75 to 1000 μm (139 hydrophone / frequency combinations). Effective sensitive element diameter d<sub>eff</sub>(f) exceeded d<sub>g</sub> by over 100 % when λ > 4d<sub>g</sub> (where λ is the wavelength). For ka<sub>g</sub> > 0.75 (where k=2π/λ), d<sub>eff</sub>(f) was consistent with the \"rigid piston\" (RP) theory, reinforcing a previous report from our laboratories. However, for ka<sub>g</sub> < 0.75, d<sub>eff</sub>(f) showed noticeable deviations from RP theory and fell between predictions from RP theory and predictions for an unbaffled (UB) circular piston. Examples: 1) For a needle hydrophone with d<sub>g</sub> = 75 μm at 1 MHz (ka<sub>g</sub> = 0.16), the data imply that average d<sub>eff</sub> = 505 μm. 2) For a needle hydrophone with d<sub>g</sub> = 400 μm at 500 kHz (common parameters for human transcranial neuromodulation; ka<sub>g</sub> = 0.42), the data imply that average d<sub>eff</sub> = 1215 μm.</p>","PeriodicalId":13322,"journal":{"name":"IEEE transactions on ultrasonics, ferroelectrics, and frequency control","volume":"PP ","pages":""},"PeriodicalIF":3.7000,"publicationDate":"2025-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Spatial Resolution Limits for Needle Hydrophones from 0.5 to 20 MHz with Implications for Transcranial Ultrasound.\",\"authors\":\"Keith A Wear, Christopher R Fury, Andre V Alvarenga\",\"doi\":\"10.1109/TUFFC.2025.3610361\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>Hydrophone spatial resolution and spatial averaging effects are determined by the frequency-dependent effective sensitive element diameter d<sub>eff</sub>(f) rather than the geometrical sensitive element diameter d<sub>g</sub>. The objective of this work was to quantify average d<sub>eff</sub>(f) for needle hydrophones as a function of d<sub>g</sub> and f. Estimates of effective radii a<sub>eff</sub>(f) = d<sub>eff</sub>(f) / 2 were inferred from directivity measurements from 0.5 to 20 MHz on 16 needle hydrophones with d<sub>g</sub> = 2a<sub>g</sub> ranging from 75 to 1000 μm (139 hydrophone / frequency combinations). Effective sensitive element diameter d<sub>eff</sub>(f) exceeded d<sub>g</sub> by over 100 % when λ > 4d<sub>g</sub> (where λ is the wavelength). For ka<sub>g</sub> > 0.75 (where k=2π/λ), d<sub>eff</sub>(f) was consistent with the \\\"rigid piston\\\" (RP) theory, reinforcing a previous report from our laboratories. However, for ka<sub>g</sub> < 0.75, d<sub>eff</sub>(f) showed noticeable deviations from RP theory and fell between predictions from RP theory and predictions for an unbaffled (UB) circular piston. Examples: 1) For a needle hydrophone with d<sub>g</sub> = 75 μm at 1 MHz (ka<sub>g</sub> = 0.16), the data imply that average d<sub>eff</sub> = 505 μm. 2) For a needle hydrophone with d<sub>g</sub> = 400 μm at 500 kHz (common parameters for human transcranial neuromodulation; ka<sub>g</sub> = 0.42), the data imply that average d<sub>eff</sub> = 1215 μm.</p>\",\"PeriodicalId\":13322,\"journal\":{\"name\":\"IEEE transactions on ultrasonics, ferroelectrics, and frequency control\",\"volume\":\"PP \",\"pages\":\"\"},\"PeriodicalIF\":3.7000,\"publicationDate\":\"2025-09-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"IEEE transactions on ultrasonics, ferroelectrics, and frequency control\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://doi.org/10.1109/TUFFC.2025.3610361\",\"RegionNum\":2,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"ACOUSTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE transactions on ultrasonics, ferroelectrics, and frequency control","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1109/TUFFC.2025.3610361","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"ACOUSTICS","Score":null,"Total":0}
Spatial Resolution Limits for Needle Hydrophones from 0.5 to 20 MHz with Implications for Transcranial Ultrasound.
Hydrophone spatial resolution and spatial averaging effects are determined by the frequency-dependent effective sensitive element diameter deff(f) rather than the geometrical sensitive element diameter dg. The objective of this work was to quantify average deff(f) for needle hydrophones as a function of dg and f. Estimates of effective radii aeff(f) = deff(f) / 2 were inferred from directivity measurements from 0.5 to 20 MHz on 16 needle hydrophones with dg = 2ag ranging from 75 to 1000 μm (139 hydrophone / frequency combinations). Effective sensitive element diameter deff(f) exceeded dg by over 100 % when λ > 4dg (where λ is the wavelength). For kag > 0.75 (where k=2π/λ), deff(f) was consistent with the "rigid piston" (RP) theory, reinforcing a previous report from our laboratories. However, for kag < 0.75, deff(f) showed noticeable deviations from RP theory and fell between predictions from RP theory and predictions for an unbaffled (UB) circular piston. Examples: 1) For a needle hydrophone with dg = 75 μm at 1 MHz (kag = 0.16), the data imply that average deff = 505 μm. 2) For a needle hydrophone with dg = 400 μm at 500 kHz (common parameters for human transcranial neuromodulation; kag = 0.42), the data imply that average deff = 1215 μm.
期刊介绍:
IEEE Transactions on Ultrasonics, Ferroelectrics and Frequency Control includes the theory, technology, materials, and applications relating to: (1) the generation, transmission, and detection of ultrasonic waves and related phenomena; (2) medical ultrasound, including hyperthermia, bioeffects, tissue characterization and imaging; (3) ferroelectric, piezoelectric, and piezomagnetic materials, including crystals, polycrystalline solids, films, polymers, and composites; (4) frequency control, timing and time distribution, including crystal oscillators and other means of classical frequency control, and atomic, molecular and laser frequency control standards. Areas of interest range from fundamental studies to the design and/or applications of devices and systems.