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Full Characterization of <i>in vivo</i> Muscle as an Elastic, Incompressible, Transversely Isotropic Material Using Ultrasonic Rotational 3D Shear Wave Elasticity Imaging

Anna E. Knight, Courtney A. Trutna, Ned C. Rouze, Lisa D. Hobson-Webb, Annette Caenen, Felix Q. Jin, Mark L. Palmeri, Kathryn R. Nightingale

2021IEEE Transactions on Medical Imaging61 citationsDOIOpen Access PDF

Abstract

Using a 3D rotational shear wave elasticity imaging (SWEI) setup, 3D shear wave data were acquired in the <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">vastus lateralis</i> of a healthy volunteer. The innate tilt between the transducer face and the muscle fibers results in the excitation of multiple shear wave modes, allowing for more complete characterization of muscle as an elastic, incompressible, transversely isotropic (ITI) material. The ability to measure both the shear vertical (SV) and shear horizontal (SH) wave speed allows for measurement of three independent parameters needed for full ITI material characterization: the longitudinal shear modulus <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${\mu }_{L}$ </tex-math></inline-formula> , the transverse shear modulus <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${\mu }_{T}$ </tex-math></inline-formula> , and the tensile anisotropy <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${\chi }_{E}$ </tex-math></inline-formula> . Herein we develop and validate methodology to estimate these parameters and measure them <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">in vivo</i> , with <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${\mu }_{L} = 5.77\pm 1.00$ </tex-math></inline-formula> kPa, <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${\mu }_{T} = 1.93\pm 0.41$ </tex-math></inline-formula> kPa (giving shear anisotropy <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${\chi _\mu } = 2.11\pm 0.92$ </tex-math></inline-formula> ), and <inline-formula xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink"> <tex-math notation="LaTeX">${\chi }_{E} = 4.67\pm 1.40$ </tex-math></inline-formula> in a relaxed <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">vastus lateralis</i> muscle. We also demonstrate that 3D SWEI can be used to more accurately characterize muscle mechanical properties as compared to 2D SWEI.

Topics & Concepts

Transverse isotropyMaterials scienceShear modulusShear (geology)AnisotropyElasticity (physics)ElastographyUltrasonic sensorShear wavesTransducerElastic modulusIsotropyAcousticsTransverse planeRotational speedSimple shearMagnetic resonance elastographyComposite materialLongitudinal waveUltrasoundYoung's modulusCompressibilityShear rateTransverse waveWave speedPure shearUltimate tensile strengthPenetration depthUltrasound Imaging and ElastographyUltrasonics and Acoustic Wave PropagationThermoelastic and Magnetoelastic Phenomena
Full Characterization of <i>in vivo</i> Muscle as an Elastic, Incompressible, Transversely Isotropic Material Using Ultrasonic Rotational 3D Shear Wave Elasticity Imaging | Litcius