Dynamic Elastography Group

 

 

Activities      

3D harmonic and transient dynamic vascular elastography

2D dynamic elastography

Rheology of biological soft tissues

Time-varying viscoelasticity of a mimicking deep vein thrombi

Imaging facilities

Patents, first publications and scientific communications of the group

Group members

Lab address and location

 

 

 Activities

 

                                               3D harmonic and transient dynamic

vascular elastography

The harmonic case

Analytical

Experimental

350 Hz harmonic shear wave

450 Hz harmonic shear wave

Examples of a 3D harmonic scattering patterns of plane shear waves by a soft cylindrical heterogeneity of 9.8 mm diameter. The top and bottom videos correspond to the scattering of a 350 Hz and 450 Hz harmonic incident waves, respectively. A quarter-volume was cut out from the entire volume in order to better visualize the displacement field into the inclusion.

 

An original application of dynamic elastography to venous and arterial pathologies was developed. The aim was to model analytically and to study, theoretically and experimentally, shear-wave scattering by a venous clot, modeled by a cylindrical soft inclusion, surrounded by an infinite soft medium.

Using a modal decomposition technique, a 3D analytical model was developed to simulate the scattering of a harmonic plane shear wave by a cylindrical inclusion for an arbitrary incident angle. The superposition principle of harmonic solutions (stationary displacement fields) served to obtain the 3D scattered field for an arbitrary incident transient plane shear wave. One can note that this model can be coupled with magnetic resonance elastography or sonoelastography techniques.

The transient case

Analytical

Experimental

Example of a transient plane shear wave, with 350 Hz central frequency and 46° inclination, scattered by a soft cylindrical heterogeneity of 9.8 mm diameter. The view represents the half of the volume to visualize the behavior of the wave into the inclusion during the propagation.

 

In the examples given here, from a mechanical point of view, the heterogeneity and surrounding materials modeled a deep venous thrombosis. Both media were assumed to be homogeneous, isotropic and linear viscoelastic materials made of agar-gelatin mixture with viscoelasticity mean values equal to m = (14600 + 0.7iw) Pa for the surrounding medium and
m = (1150 + 0.035iw) Pa for the heterogeneity.

It is important to point out that the presence of oscillations in the heterogeneity observed in the horizontal planes and along the vertical direction are directly related to the inclusion constitutive material viscoelasticity. Indeed, on one hand oscillation wavelengths are a function of elasticity, and on the other hand their amplitudes depend on both elasticity and viscosity. Another scattered wave characteristic is its spatial distribution in a given horizontal plane, i.e. the shear wave slowing down after crossing the inclusion, the orientation of diffraction lobes in the surrounding medium, the 2D shape of oscillations into the inclusion, the wave diffraction angle into the inclusion with respect to its axis, etc. All these behaviors are related to the internal and external viscoelastic properties, but also to the contrast between them. Consequently, one could exploit this rich information to characterize mechanical properties of heterogeneous media.

 

 

2D dynamic elastography

 

Plane shear wave diffraction by a cylinder. Left: 3D representation of the diffraction problem. Right: view of the two-dimensional configuration.  

 

The incident plane shear wave is now considered to be parallel to the cylinder axis, propagating along the x-axis and polarized along the y-axis. Both media are assumed to be homogeneous, linear, viscoelastic and incompressible. Taking into account the geometrical and mechanical conditions of the problem, one can assume a plane strain mechanical state which reduce the acoustical problem to a two dimensional one. Consequently, displacement field in both inclusion and surrounding medium is contained in the x-y plane. This configuration corresponds to a particular case of the general 3D configuration.

 

                         Experimental

                      Analytical

Experimental (left) and simulated (right) transverse displacements of a 200 Hz harmonic shear wave at different moments after the wave generation. The inclusion, radius equal to 4.0 mm, was filled with coagulated blood.

 

The figure above shows the typical experimental and theoretical propagation of a 200 Hz harmonic shear wave interacting with a cylindrical inclusion (diameter equal to 8.0 mm) filled with coagulated blood. The motion source positioned on the left side generated a plane shear wave that traveled form left to right. After the shear wave diffraction by the inclusion, a distortion and a deceleration appeared due to viscoelastic differences between the clot, m = (943 +0.35iw) Pa, and surrounding medium, m = (14600 +0.7iw) Pa,. Pattern distributions observed into the inclusion clearly depicted shorter wavelengths than in the agar-gelatin surrounding medium. These behaviors can be exploited in an inverse problem to characterize the viscoelastic properties of both inclusion (heterogeneity) and surrounding media.

                                                                                                               

 

Rheology of biological soft tissues

The coagulated blood example

 

Deep venous thrombosis (DVT) is a vascular pathology annually diagnosed in 67 per 10000 individuals for the general population. This pathology is characterized by the formation of a blood clot or thrombi in lower limb veins and can lead to pulmonary embolism. Screening of deep vein thrombus formation and its spatio-temporal mechanical evolution are of importance for determining an appropriate therapy. Most imaging methods proposed so far suffer from two important drawbacks: the viscoelasticity reconstruction is biaised, and the elasticity is assessed only when the blood clot is formed. This section presents the validation a Voigt viscoelastic model to simulate the rheological behavior of blood clots.

Multi-frequency study of a large volume of blood completely coagulated. Voigt’s and Maxwell’s models were fitted to the velocity (vs) and attenuation (a) of experimental data.

To validate the assumption of the Voigt’s model as a simple and realistic viscoelastic representation of blood clots, we represent the frequency dependence (50-190 Hz) of a plane shear wave velocity (vs) and attenuation (a) 3 hours after adding CaCl2 to blood (to force coagulation) at a hematocrit of 40%. The plane shear wave was propagating into a homogeneous and parallelepipedal volume of coagulated blood. Voigt’s and Maxwell’s models fitted on experimental data are plotted on the same figure. The Voigt’s model (m = 943 Pa, h = 0.35 Pa.s) correctly predicted the blood clot mechanical behavior. Indeed, both models fitted well the velocity (around 0.92 m/s) but only the Voigt’s model was appropriate for the description of viscous effects on attenuation.

(left) Time-varying velocity (vs) and attenuation (a) of a 40% hematocrit blood clot homogenous sample. (right) Elasticity (m) and viscosity (h) variations calculated from vs and a profiles by assuming a Voigt’s model. Harmonic shear waves had a frequency of 70 Hz. 

The study of plane shear wave propagation into a homogeneous blood sample also permit to assess the viscoelasticity evolution during clotting. The shear wave velocity and attenuation during the formation of a blood clot were studied from 50 min (liquid to solid transition) to more than 3 hours following the addition of CaCl2 (see figure above). From these results, we calculated the elasticity (m) and viscosity (h) corresponding to Voigt’s model. It is shown that when the medium became solid (after the clotting time), the 1D dynamic elastography permits to follow the clot mechanical evolution: the shear wave velocity increases (from 0.76 m/s to 1.01 m/s) and the attenuation decreases (from 95 Np/m to 54 Np/m). Retrieved elasticity and viscosity showed an evolution in two phases: blood clot hardening (m and h increasing) during approximately 50 min followed by a mechanical structure stabilization when the viscoelastic parameters reach a plateau (m @ 1100 Pa, h @ 0.3 Pa.s).

 

 

Time-varying viscoelasticity of a mimicking deep vein thrombi

Inverse problem

Staging mechanical properties of deep vein thrombi (elasticity and viscosity) can be of importance for therapy planning because the compactness of a blood clot impacts the efficiency of thrombolysis drugs. Dynamic Vascular Elastography (DVE) can serve to evaluate these mechanical properties. In the current example, it consists to retrieve viscoelastic parameters of 8-mm diameter blood clot cylindrical inclusions, embedded in an agar-gelatin material, from the diffraction characteristics of a harmonic shear wave.

Block diagram of the inverse problem used to estimate, from RF images, elasticity (m) and viscosity (h) of the blood inclusion (material 1) and surrounding tissue (material 2).

The technique firstly implies the generation of a harmonic plane shear wave (with a frequency of 200 Hz) in the heterogeneous medium and the tracking of this wave with an ultra-fast ultrasound scanner (frame rate > 3000 Hz). Using the 2D dimensional model presented above, an inverse problem was formulated as a least-square minimization between simulations and experimental results of viscoelasticity. Dynamic Vascular Elastography proved to have sufficient sensitivity to follow the time-varying blood coagulation process and to differentiate mechanical properties of blood samples with different hematocrits.

Time-varying elasticity (m) and viscosity (h) of 8-mm diameter cylindrical blood clot inclusions at 30% (H30) and 50% (H50) hematocrit levels. Clotting times (transition time between the liquid and the solid state) are defined as tH30 and tH50.

One can observe that the lower the hematocrit, the harder and more viscous was the blood clot. We also showed that the clotting time was affected by the hematocrit. The results given by the Dynamic Vascular Elastography method are promising to quantify the time-varying mechanical properties of a small blood inclusion during coagulation. This approach may be applicable in vivo.

 

 

 

Imaging facilities

Dynamic Macro-Elastography

Sonix RP ultrasonic scanner (Ultrasonix Medical Corporation, Burnaby, BC, Canada)

Dynamic Micro-Elastography

VisualSonics scanner Vevo 770 (VisualSonics Inc., Toronto, Ontario, Canada)

Dynamic Macro-Elastography set-up

Dynamic Micro-Elastography set-up

 

Patents, first publications and scientific communications of the group

 

 

A. Hadj Henni, C. Schmitt and G. Cloutier, “Shear wave induced resonance for dynamic elastography and material characterization”, United States Provisional Patent L80004902US, July 30, 2008.

A. Hadj Henni, C. Schmitt and G. Cloutier, “3D transient and harmonic shear-wave scattering by a soft cylinder for dynamic vascular elastography”, J. Acoust. Soc. Am. (October 2008) (in press).

A. Hadj Henni, C. Schmitt and G. Cloutier, “Shear Wave Induced Resonance: a new excitation mode for dynamic elastography imaging”, IEEE Ultrasonics Symposium, 2-5 November 2008, Beijing, China.

C. Schmitt, A. Hadj Henni and G. Cloutier, “Dynamic Micro-Elastography (DME) applied to viscoelastic characterization of mimicking carotid arteries”, IEEE Ultrasonics Symposium, 2-5 November 2008, Beijing, China.

C. Schmitt, A. Hadj Henni and G. Cloutier, “Viscoelastic characterization of soft tissues by dynamic micro-elastography (DME) in the frequency range of 300 Hz -1500 Hz”, IEEE Ultrasonics Symposium, 2-5 November 2008, Beijing, China.

A. Hadj Henni, C. Schmitt and G. Cloutier, “Analytical modeling of plane shear wave diffraction by a radially layered cylinder for dynamic vascular elastography”, IEEE Ultrasonics Symposium, 28-31 October 2007, New York, USA.

C. Schmitt, A. Hadj Henni and G. Cloutier, “Characterization of time-varying mechanical viscoelastic parameters of mimicking deep vein thrombi with 2D dynamic elastography”, IEEE Ultrasonics Symposium, 28-31 October 2007, New York, USA.

E. Montagnon, A. Hadj Henni, C. Schmitt and G. Cloutier, “Shear-wave induced resonance elastography (SWIRE) of elliptical mechanical heterogeneities”, International Conference on the Ultrasonic Measurement and Imaging of Tissue Elasticity, 27-30 October 2008, Austin, USA.

A. Hadj Henni, C. Schmitt and G. Cloutier, 3D Analytical modeling of transient and harmonic plane shear wave diffraction by a soft cylinder for dynamic vascular elastography , International Conference on the Ultrasonic Measurement and Imaging of Tissue Elasticity, 2-5 November 2007, Santa Fe, USA.

 

Group members

 

 

Guy CLOUTIER

ing/Ph.D, Lab director.

Anis HADJ HENNI 

ing/Ph.D, Postdoctoral fellow.

e-mail

guy.cloutier@umontreal.ca

e-mail

anis.hadjhenni@crchum.qc.ca

Tel

+1  514-890-8000 (24703)

Tel

+1  514-890-8000 (24773)

Fax

+1  514-412-7505

Fax

+1  514-412-7505

Cédric SCHMITT 

Ing, M.Sc, Ph.D student (CV)

Emmanuel MONTAGNON 

M.Sc. student.

e-mail

schmitt.cedric@gmail.com

e-mail

emmanuelmontagnon@gmail.com

Tel

+1  514-890-8000 (24773)

Tel

+1  514-890-8000 (24773)

Fax

+1  514-412-7505

Fax

+1  514-412-7505

Elizabeth MERCURE

M. Sc. Research assistant

 

 

e-mail

elizabeth.mercure@crchum.qc.ca

 

 

Tel

+1  514-890-8000 (24773)

 

 

Fax

+1  514-412-7505

 

 

                                                                                                                                         

 

Lab address and location

 

Laboratory of Biorheology and Medical Ultrasonics
Research Center, University of Montreal Hospital
Pavilion J.A. de Sève (room Y-1619)
2099 Alexandre de Sève
Montreal
, Quebec, Canada,
H2L 2W5.

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