Pitt Shield

Acoustic Transmission Factor through the Rat Skull as a Function of Body Mass, Frequency and Position.

Authors: Gerstenmayer M, Fellah B, Magnin R, Selingue E, Larrat B

In many transcranial ultrasound studies on rats, the transmission factor is assumed to be independent of animal weight and losses resulting from non-normal incidence angles of the beam are not accounted for. In this study, we measured acoustic transmission factors through 13 excised skulls of male Sprague-Dawley rats weighing between 90 and 520g, at different positions on each skull and at 1, 1.25, 1.5, 1.75 and 2MHz. Our results revealed that insertion loss through rat skull increases linearly with both body mass and frequency and strongly depends on the position, decreasing from the front to the back and from the midline to the lateral sides. Skull thickness also scales linearly with body mass. Reflection explains the main part of the insertion loss compared with attenuation and aberration. These data are helpful in predicting the acoustic pressure at the focus in the brain.

Introduction

Purpose Other
Study Objective Determine how acoustic transmission through the rat skull varies with body mass, acoustic frequency, and skull position.
Animal model / Human subject Rat (species: rat), strain Sprague-Dawley, age not specified, sex male
Disease model Healthy

Outcomes and Safety

Summary of Outcomes They quantified acoustic transmission through rat skulls and found transmission depends strongly on body mass, ultrasound frequency, and skull position; lower acoustic frequencies and particular skull positions produced the highest transmission.
Safety-related matter This is an ex vivo study using excised rat skulls, no in vivo experiments

Brain Region

Visualization unavailable

Ultrasound Parameters

Ultrasound instrument Mono-element concave MR-compatible transducer
FUS Frequency 1.5 MHz
FUS Pressure 0.8 MPa
FUS Mode pulsed
Focal Characteristics Focal depth: 20 mm; Focal length: None; Aperture size: None

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