Evidence map›Paper›PMID 41415613›Full record

ArticleArXiv2025

The choice of viscous or viscoelastic models affects attenuation and velocity determination in simplified skull-mimicking digital phantoms.

Samuel Clinard, Taylor Webb, Henrik Odéen, Dennis L Parker, Douglas A Christensen

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In one paragraph

Article in ArXiv, 2025. The graph could read no effect estimate from its abstract, so it casts no vote on the map. Not yet cited in PubMed.

0numbers the graph read from it
0cells of the map it votes in
0citing papers in PubMed
–field-weighted citation impact
1 · What the graph read from it

What it found

Each row is one number read from the abstract, on the scale the paper reported it, with its interval. Left of the dashed line favours the treatment, right favours the comparator. Under each row is the sentence it came from. New to these charts? A ten-minute tutorial.

The abstract states no effect estimate the extractor could read, or names no intervention and outcome on the map, so this paper lights no cell and moves no belief. It is still indexed, cited and linked below.

2 · The registry

The trial behind it

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Neither the registry nor the abstract names a trial number. If this is a trial report, that itself is worth knowing.

3 · Its place in the literature

Who cites it

0 citing papers in PubMed.

No citing paper in PubMed yet.

4 · The record

Corrections and comments

PubMed lists nothing against this paper. Absence here is not a guarantee, only a check that was made.

5 · Who and what money

Authors and funding

5 authors.

Samuel ClinardDepartment of Biomedical Engineering, University of Utah, Salt Lake City, Utah, USA.
Taylor WebbDepartment of Radiology and Imaging Sciences, University of Utah, Salt Lake City, USA.
Henrik OdéenDepartment of Radiology and Imaging Sciences, University of Utah, Salt Lake City, USA.
Dennis L ParkerDepartment of Radiology and Imaging Sciences, University of Utah, Salt Lake City, USA.
Douglas A ChristensenDepartment of Biomedical Engineering, University of Utah, Salt Lake City, Utah, USA.

Funding

Toward the next generation in transcranial MR-guided focused ultrasound: Innovations in thermal and acoustic model-based planning and monitoring for improved safety, efficacy and efficiencyR01EB028316 · NIBIB · UNIVERSITY OF UTAH · PI PARKER, DENNIS L, RIEKE, VIOLA · 2019 to 2022
$2.5M
Feasibility of transcranial histotripsy for pediatric neuro-oncology applications using a hemispherical transducerR21EB033117 · NIBIB · UNIVERSITY OF UTAH · PI ODEEN, HENRIK CARL AXEL · 2022 to 2024
$627k
Acoustic Modeling of skull bone for improved transcranial MR-guided focused ultrasound therapyF31DE032916 · NIDCR · UNIVERSITY OF UTAH · PI CLINARD, SAM · 2023 to 2024
$85k
NIBIB NIH HHS R01 EB028316NIBIB NIH HHS R21 EB033117NIDCR NIH HHS F31 DE032916
6 · The paper itself

Abstract

Objective: Simulation-guided transcranial focused ultrasound therapies rely on accurately estimating the skull's acoustic properties with pretreatment imaging. The typical imaging resolution (0.5 mm isotropic) is insufficient to resolve the bone microstructure, and as a result, the acoustic properties are underdetermined. Consequently, the determination of acoustic properties is sensitive to methodology. Here, we investigate how viscous or viscoelastic models predict variations in attenuation and phase velocity due to microstructure. Approach: Using viscous and viscoelastic k-Wave implementations, we simulated the transmission of a broadband 625 kHz tone burst ( -6 dB bandwidth: 250 kHz-1 MHz) through skull-mimicking digital phantoms. The phantoms consisted of spherical marrow pores (0.1 mm-1.0 mm diameter) randomly placed within a solid cortical background (2.5%-90% porosity). Virtual sensors measured the attenuation and phase velocity by the time-distance matrix approach. Results: Both models predict that attenuation increases with increasing pore size for a fixed porosity, but the strength of the relationship and its dependence on porosity depend on the simulation technique applied. The viscoelastic model generally predicts that the attenuation peaks at larger porosity values than those predicted by the viscous model. For example, for 1.0 mm pore phantoms, the viscous attenuation peak (1.98 Np/cm) occurs at 20% porosity, while the viscoelastic peak (2.98 Np/cm) occurs at 70%. In general, the phase velocity decreases for larger pore phantoms for both techniques, but the phase velocity/porosity relationship predicted by the viscoelastic model is less sensitive to pore size compared to the viscous model. Significance: Viscous and viscoelastic models predict different attenuation and phase velocity behavior for these idealized bone models. While both approaches predict that properties of bone microstructure have a large impact on acoustic attenuation within the skull, the viscous model indicates that bone microstructure impacts phase velocity within the skull, whereas the viscoelastic model suggests that phase velocity is less sensitive to microstructure. This study highlights the acoustic model's role in predicting transcranial propagation and the need to identify which approach most accurately reflects the physics of the human skull.

Identifiers

PMID41415613
PMCPMC12709493

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Read under generation 80e0d062 · epoch 390. Bibliography from PubMed, PubMed Central and OpenAlex; grants from NIH RePORTER; trial links from ClinicalTrials.gov; estimates, votes and beliefs from the OpenQuestion graph.