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Displacement peak averages [μm] -Fig. 4.

Displacement peak averages [μm] -Fig. 4.

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Shear wave elasticity imaging (SWEI) was employed to track acoustic radiation force impulse (ARFI)-induced shear waves in the mid-myocardium of the left ventricular free wall (LVFW) of a beating canine heart. Shear waves were generated and tracked with a linear ultrasound transducer that was placed directly on the exposed epicardium. Acquisition wa...

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... Briefly, an acoustic radiation force impulse excitation "push" of 900 cycles at a 6.25-MHz center frequency was focused at a 20-mm depth within the phantom, 5-mm laterally from each target (Fig 2E), to generate a shear wave that was then tracked with pulse-echo US to determine local SWS of the material. Shear wave velocity through the phantom background and the inclusions was measured [39,41] to obtain Young's modulus estimates assuming a linear, isotropic, elastic medium. Each phantom was imaged 10 times for statistical analysis. ...
... Shear wave imaging data for the compliant elasticity phantom (Phantom 12) showed mean shear wave velocities between 1.6±0.1 and 2.3±0.1 m/s within regions of 5 and 12.5 seconds of cure time, respectively (S2 Table). These shear wave velocities correspond to Young's moduli of 7.6 and 15.6 kPa, respectively, assuming a linear, isotropic, elastic medium; these values are within the range reported for in vivo imaging of soft tissue [41]. The stiff elasticity phantom (Phantom 13) presented a similar trend of increasing shear wave velocity with cure time; however, Young's modulus estimates within the inclusions were significantly higher than typical soft tissue values, ranging from 72.9 to 123.6 kPa (S2 Table). ...
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... The shear wave elasticity imaging (SWEI) [40] technique was used to track mechanical waves due to radiation force in the left-ventricular myocardium of an open chest dog at several positions and depths in the LV free wall and reported speeds ranging from 0.82 to 2.65 m s −1 [41,42]. A similar method, supersonic shear imaging (SSI) [43], uses focused acoustic radiation force to generate mechanical waves in tissue by moving the source of vibration at a supersonic speed along the line of excitation, creating a wave front. ...
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... It is targeted mainly at radiology applications such as liver cirrhosis and breast cancer diagnosis (Parker et al. 2011 ). The suspected correlation between diastolic dysfunction and myocardial stiffness led to several ultrasound studies on the use of shear waves to measure the myocardial stiffness (Bouchard et al. 2009; Hollender et al. 2012; Kanai 2005; Song et al. 2013; Urban et al. 2013; Vos et al. Ultrasound in Med. ...
... They reported the propagation of a wave front along the anterior left ventricular wall with a propagation velocity that correlates well to the derived diastolic elasticity of the wall. Alternatively, the waves can be induced by external sources (Bouchard et al. 2009; Hollender et al. 2012; Song et al. 2013; Urban et al. 2013). Shear waves in soft biological tissue have a propagation velocity of 1–10 m/s, and this velocity is influenced by the stiffness of cardiac tissue (Couade et al. 2011; Kanai 2005; Urban et al. 2013). ...
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... Hence, very complex signal processing methods are required to accurately estimate the motion353637. This method has been used for investigation of phantoms, liver, prostate, and cardiac tissue [38, 39]. ...
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Conventional imaging of diagnostic ultrasound is widely used. Although it makes the differences in the soft tissues echogenicities’ apparent and clear, it fails in describing and estimating the soft tissue mechanical properties. It cannot portray their mechanical properties, such as the elasticity and stiffness. Estimating the mechanical properties increases chances of the identification of lesions or any pathological changes. Physicians are now characterizing the tissue’s mechanical properties as diagnostic metrics. Estimating the tissue’s mechanical properties is achieved by applying a force on the tissue and calculating the resulted shear wave speed. Due to the difficulty of calculating the shear wave speed precisely inside the tissue, it is estimated by analyzing ultrasound images of the tissue at a very high frame rate. In this paper, the shear wave speed is estimated using finite element analysis. A model is constructed to simulate the tissue’s mechanical properties. For a generalized soft tissue model, Agar-gelatine model is used because it has properties similar to that of the soft tissue. A point force is applied at the center of the proposed model. As a result of this force, a deformation is caused. Peak displacements are tracked along the lateral dimension of the model for estimating the shear wave speed of the propagating wave using the Time-To-Peak displacement (TTP) method. Experimental results have shown that the estimated speed of the shear wave is 5.2 m/sec. The speed value is calculated according to shear wave speed equation equals about 5.7 m/sec; this means that our speed estimation system’s accuracy is about 91 %, which is reasonable shear wave speed estimation accuracy with a less computational power compared to other tracking methods.
... In addition, variation of the wave speed through the thickness of the myocardium at different angles in an explanted heart sample was also reported. A study in open chest dogs using waves generated using ARF was reported by Bouchard et al (2009). Variation of shear modulus in Langendorff perfused isolated rat and rabbit hearts was also explored using ARF methods , Vejdani-Jahromi et al 2015. ...
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... In addition, variation of the wave speed through the thickness of the myocardium at different angles in an explanted heart sample was also reported. A study in open chest dogs using waves generated using ARF was reported by Bouchard et al (2009). Variation of shear modulus in Langendorff perfused isolated rat and rabbit hearts was also explored using ARF methods , Vejdani-Jahromi et al 2015. ...
Conference Paper
Shear wave elastography with acoustic radiation force (ARF) or harmonic vibration (HV) has been applied in animals and humans to evaluate myocardial material properties. The anisotropic myocardial structure presents a unique challenge to wave propagation methods because the fiber direction changes through the wall thickness. To investigate the effects of the frequency of excitation in the myocardium we constructed systolic and diastolic finite element models (FEMs) and performed an experiment on an ex vivo porcine heart. Both models were constructed with multiple elastic, transverse isotropic layers with a shear wave velocity (SWV) along and across the fibers where each layer has 1 mm thickness with the top and bottom in contact with water. The orientation of the muscle fibers was changed for each layer ranging from −50° to 80° from top to bottom. Harmonic excitations at 30, 50, 100, and 200 Hz and an impulsive force were used. An ex vivo porcine heart was tested using ARF excitations with a transesophogeal probe driven with a Verasonics ultrasound system applied directly to the left ventricular wall. We evaluated the measured orientation of the fibers in each layer by evaluating the angle with the highest SWV. The 30 and 50 Hz results showed little or no variation in the measured orientation angle in the layers. The 100 and 200 Hz results showed some variation of the orientation with respect to the layer. The impulse simulation results showed good agreement with the true orientations except near the top and bottom boundaries. The values of SWV were found to have different levels of bias depending on the excitation. The experimental results in the ex vivo heart showed similar trends as the FEM model results where the waves at lower frequencies had lower sensitivity to fiber direction. This multi-layered anisotropic model demonstrates how to resolve different anisotropic layers in the myocardium using ARF or HV while also revealing that using lower frequencies results in measurements that are less sensitive to anisotropy variation through the thickness of the myocardial wall.
... ARFI elastography has two modes: the tissue displacement at longitudinal direction provides a qualitative response for virtual tissue imaging (VTI), which measures qualitatively by the area ratio (AR); and a quantitative response for virtual touch tissue quantification (VTQ), which measures transverse SWV values in m/sec. Compared with previous conventional strain elastography, ARFI could evaluate the breast tissue stiffness without external compression and provide qualitative and quantitative information to help differentiation between malignant and benign breast lesions19202122. ...
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This meta-analysis was aimed to assess the diagnostic performance of acoustic radiation force impulse (ARFI) elastography for the differentiation of malignant and benign breast lesions. The databases of PubMed, Web of Science(TM), WanFang, Vip, SinoMed and China National Knowledge Infrastructure were searched for all studies that evaluated the diagnostic performance of ARFI including virtual touch tissue quantification (VTQ) and virtual touch tissue imaging (VTI). All the studies were published prior to Mar. 21, 2014. The studies published in English or Chinese were collected. A total of 11 studies, including 1,408 breast lesions from 1,245 women, were analyzed. The values of summary sensitivity and summary specificity were 0.843 (95% confidence interval [CI]: 0.811-0.872) and 0.932 (95% CI: 0.913-0.948) for VTQ of ARFI, and 0.864 (95% CI: 0.799-0.914) and 0.882 (95% CI: 0.832-0.922) for VTI of ARFI, respectively. Subgroup analysis excluding mucinous carcinoma and carcinoma in situ showed higher summary sensitivity (0.877 95% CI: 0.835-0.911), higher summary specificity (0.943 95% CI: 0.921-0.960) and lower heterogeneity (I(2)=23.5%). The cut-off values for shear wave velocity of VTQ ranged widely from 2.89 to 6.71 m/s, while the VTI ranged narrowly from 1.37 to 1.66. In general, ARFI elastography seems to be a good method for differentiation between benign and malignant breast lesions. However, its usefulness for identifying breast mucinous carcinoma and breast carcinoma in situ is limited. VTI seems to be more reliable and repeatable than VTQ.
... In addition, variation of the wave speed through the thickness of the myocardium at different angles in an explanted heart sample was also reported. A study in open chest dogs using waves generated using ARF was reported by Bouchard et al (2009). Variation of shear modulus in Langendorff perfused isolated rat and rabbit hearts was also explored using ARF methods , Vejdani-Jahromi et al 2015. ...
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... Similar in principle methods proposed by using magnetic resonance imaging (MRI) [18, 19] or by using ECG-2 gated technique [20]. More direct tissue characterization methods have been developed as well, typically referred to as elastography, and applied for the assessment of soft, bulky tissues like the liver [21, 22], breast [23], prostate [24], skeletal muscles [25], kidneys [26], and heart [27, 28] . These elasticity imaging techniques rely on the application of a force to an area of interest in the tissue and measure tissue's mechanical response. ...
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Supersonic shear wave imaging (SSI) is a noninvasive, ultrasound-based technique to quantify the mechanical properties of bulk tissues by measuring the propagation speed of shear waves (SW) induced in the tissue with an ultrasound transducer. The technique has been successfully validated in liver and breast (tumor) diagnostics and is potentially useful for the assessment of the stiffness of arteries. However, SW propagation in arteries is subjected to different wave phenomena potentially affecting the measurement accuracy. Therefore, we assessed SSI in a less complex ex vivo setup, that is, a thick-walled and rectangular slab of an excised equine aorta. Dynamic uniaxial mechanical testing was performed during the SSI measurements, to dispose of a reference material assessment. An ultrasound probe was fixed in an angle position controller with respect to the tissue to investigate the effect of arterial anisotropy on SSI results. Results indicated that SSI was able to pick up stretch-induced stiffening of the aorta. SW velocities were significantly higher along the specimen's circumferential direction than in the axial direction, consistent with the circumferential orientation of collagen fibers. Hence, we established a first step in studying SW propagation in anisotropic tissues to gain more insight into the feasibility of SSI-based measurements in arteries.