In the present paper a continuum poroelastic model for high frequency acoustic waves in hydrogels has been developed. The model has been used to obtain the acoustic longitudinal wave equation for ultrasound. In order to obtain a satisfactory model for hydrogels, a viscoelastic force describing the interaction between the polymer network of the matrix and the bounded water is introduced. The model is validated by means of ultrasound (US) wave speed and attenuation measurements in polyvinylalcohol (PVA) hydrogel samples as a function of their water volume fraction "ß" and polymer matrix cross-linking. Themodel predicts that the law??(1+d) for ultrasound attenuation can be applied as a function of the frequency ?, where d is the frequency exponent of the polymer-boundedwater viscosity. This outcome canwell explain the attenuation of the US frequency in natural gelswhere d is typically about 0.25÷0.50while the value for purewater is 1. The theory and experiments show that US attenuation in hydrogels decreases steadily with the increase of its water volume fraction ß in a linear. The newproposed dissipativemechanismleads to a USwave speed c that follows the law: c=cw(ß-?)-3/2, where cw is the US wave speed in water and ? is the volume fraction of the bounded water. Since 0bßb1 and ?N0, the hydrogel US velocity is always higher than that of pure water. If ß tends to 1 (100% water), then the US speed in hydrogels converges to a higher value than that of pure water. The US speed gap at ß=1, between hydrogels and water, is the direct consequence of the introduction of the polymer network-bounded water interaction. This is in linewith the experimental results that show that the US speed gap atß=1 decreases in the gel samples with amore cross-linked polymermatrix that has a lower bounded water volume fraction. On the contrary, if thewater content is very low(i.e., ßb0.4), the measured US speed converges to that of the dry hydrogelmatrixwhich increases in the samples with a higher degree of network cross-linkingwith greater elastic moduli.
Acoustic waves in hydrogels: A bi-phasic model for ultrasound tissue-mimicking phantom
Chiarelli P
2008
Abstract
In the present paper a continuum poroelastic model for high frequency acoustic waves in hydrogels has been developed. The model has been used to obtain the acoustic longitudinal wave equation for ultrasound. In order to obtain a satisfactory model for hydrogels, a viscoelastic force describing the interaction between the polymer network of the matrix and the bounded water is introduced. The model is validated by means of ultrasound (US) wave speed and attenuation measurements in polyvinylalcohol (PVA) hydrogel samples as a function of their water volume fraction "ß" and polymer matrix cross-linking. Themodel predicts that the law??(1+d) for ultrasound attenuation can be applied as a function of the frequency ?, where d is the frequency exponent of the polymer-boundedwater viscosity. This outcome canwell explain the attenuation of the US frequency in natural gelswhere d is typically about 0.25÷0.50while the value for purewater is 1. The theory and experiments show that US attenuation in hydrogels decreases steadily with the increase of its water volume fraction ß in a linear. The newproposed dissipativemechanismleads to a USwave speed c that follows the law: c=cw(ß-?)-3/2, where cw is the US wave speed in water and ? is the volume fraction of the bounded water. Since 0bßb1 and ?N0, the hydrogel US velocity is always higher than that of pure water. If ß tends to 1 (100% water), then the US speed in hydrogels converges to a higher value than that of pure water. The US speed gap at ß=1, between hydrogels and water, is the direct consequence of the introduction of the polymer network-bounded water interaction. This is in linewith the experimental results that show that the US speed gap atß=1 decreases in the gel samples with amore cross-linked polymermatrix that has a lower bounded water volume fraction. On the contrary, if thewater content is very low(i.e., ßb0.4), the measured US speed converges to that of the dry hydrogelmatrixwhich increases in the samples with a higher degree of network cross-linkingwith greater elastic moduli.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.
