2015
DOI: 10.1007/s10439-015-1294-7
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Characterisation of Elastic and Acoustic Properties of an Agar-Based Tissue Mimicking Material

Abstract: As a first step towards an acoustic localisation device for coronary stenosis to provide a non-invasive means of diagnosing arterial disease, measurements are reported for an agar-based tissue mimicking material (TMM) of the shear wave propagation velocity, attenuation and viscoelastic constants, together with one dimensional quasi-static elastic moduli and Poisson's ratio. Phase velocity and attenuation coefficients, determined by generating and detecting shear waves piezo-electrically in the range 300 Hz-2 k… Show more

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Cited by 7 publications
(5 citation statements)
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“…Therefore, anticipating how this might affect the results are challenging. Moreover, the soft tissue embedding the carotid arteries would further dampen the instabilities that would present on the skin surface, generally with a lower amplitude relative to the fluctuations induced by the turbulent-like post-stenotic flow 5…”
Section: Discussionmentioning
confidence: 99%
“…Therefore, anticipating how this might affect the results are challenging. Moreover, the soft tissue embedding the carotid arteries would further dampen the instabilities that would present on the skin surface, generally with a lower amplitude relative to the fluctuations induced by the turbulent-like post-stenotic flow 5…”
Section: Discussionmentioning
confidence: 99%
“…Therefore, the vertical strain related to the compression was estimated based on σ compression and the bulk modulus ( K ) definition: , where and is the vertical compression-related thickness change. Furthermore, is defined using the initial absolute shear modulus of the explant matrix: , where is the Poisson’s ratio of agarose: = 0.44 is based on 66 . The, the effective elastic modulus of the compressed explant-culture matrix is .…”
Section: Methodsmentioning
confidence: 99%
“…The key pieces that will be modeled are the loading profile (loading begins at t = Γ 1 and lasts until the weight begins to be released at t = Γ 3 ), which we will model as instantaneous loading to position A , and the oscillations after weight release (free oscillations begin at t = Γ 4 = 0) which are the main object of investigations here. For more information on the experimental setup, interested readers may refer to [27]. …”
Section: Methodsmentioning
confidence: 99%