| Literature DB >> 31435087 |
Pedro Henrique de Marqui Moraes1, Rosa Sigrist1, Marcelo Straus Takahashi2, Marcelo Schelini1, Maria Cristina Chammas1.
Abstract
The elastic properties of tissue have always been of interest in clinical practice. In the past, the identification of structures that were stiffer on physical palpation would raise the suspicion that "there was something wrong". With the development and advancement of medicine, there proved to be a true correlation in the prediction of malignancy of a lesion: malignant disease tends to stiffen the affected tissue, either by increased cell proliferation or fibrosis. Palpation is the oldest method for the detection of thyroid nodules, which is informed by the knowledge that malignant thyroid lesions tend to be much harder than benign ones. Unfortunately, palpation is a highly subjective method that is dependent on the size and location of the lesion, as well as on the skill of the physician. In cases where these nodules are very small or are located in deep regions, their detection by palpation is difficult or even impossible. In addition, although a malignant lesion differs in terms of elasticity, it may not have echogenic properties, preventing its detection by conventional ultrasound. Imaging that indicates the stiffness or deformation of tissues, through the use of ultrasound elastography techniques, adds new information related to their structural formation. In this article, we review the basic physical principles of elastography and the evolution of the method for the evaluation of thyroid nodules, as well as the limitations of and future perspectives for its use.Entities:
Keywords: Elasticity imaging techniques/methods; Shear wave elastography; Thyroid gland; Thyroid nodule/diagnostic imaging; Ultrasonography/methods
Year: 2019 PMID: 31435087 PMCID: PMC6696751 DOI: 10.1590/0100-3984.2018.0084
Source DB: PubMed Journal: Radiol Bras ISSN: 0100-3984
Figure 1Physics of ultrasound elastography and the methods of measurement. In stress imaging (A), the tissue displacement is measured by correlating the radiofrequency echo signals between search windows (boxes) in the pre- and post-compression states. In the shear wave image (B), the particle motion is perpendicular to the direction of wave propagation, with shear wave velocity (cs) related to the shear modulus (G).
Figure 2Ultrasound elastography techniques. The elastography techniques currently available can be categorized by the physical quantity measured: compression imaging (A) and shear wave imaging (B). Excitation methods include quasi-static mechanically induced displacement via active external compression or passively induced physiological movement (in orange), dynamic compression induced by “beating” the transducer on the tissue surface to produce shear waves (in green), and dynamic ultrasound, defined as displacement of the induced tissue and the generation of shear waves through ARFI excitation (in blue).
Figure 3Photograph of B-mode ultrasound (A) and color-coded elastogram (B) of a thyroid nodule in the right lobe during compression elastography. The nodule appears hypoechoic with poorly defined contours in the anatomical B-mode ultrasound image. The elastogram shows normal thyroid tissue encoded with red color (soft tissue) and the nodule with blue staining (stiff tissue), suggesting a malignant nodule. This was confirmed by histology, which showed papillary thyroid carcinoma.
Summary of studies evaluating compression elastography for the identification of malignant thyroid lesions.
| Study | Patients (n) | Lesions (n) | Malignant | Technique | Parameter | Sensitivity (%) | Specificity (%) |
|---|---|---|---|---|---|---|---|
| Bojunga et al.[ | 530 | 639 | 153 | Strain elastography | Strain ratio | 92.0 | 90.0 |
| Moon et al.[ | 676 | 703 | 217 | Strain elastography | Strain ratio (4-point scale) | 65.4 | 58.2 |
| Strain ratio (5-point scaled) | 15.7 | 95.3 | |||||
| Azizi et al.[ | 706 | 912 | 86 | Strain elastography | Strain ratio | 80.2 | 70.2 |
| Trimboli et al.[ | 446 | 498 | 126 | Strain elastography | Strain ratio | 81.0 | 62.0 |
Asteria score[(16)];
Rago score[(19)].
Figure 4B-mode ultrasound (A) showing a hypoechoic thyroid nodule with poorly defined margins in the right lobe, suggesting a malignant etiology. The corresponding color-coded elastogram (B) shows greater stiffness in the ROI within the nodule than in the surrounding normal parenchyma (130.92 kPa vs. 24.83 kPa), suggesting that the nodule is malignant. A subsequent biopsy confirmed the diagnostic hypothesis of papillary carcinoma.
Summary of studies of 2D-SWE evaluating nodule elasticity index cutoff points above which the risk of carcinoma is increased.
| Study | Patients | Lesions | Malignant | Technique | Equipment | Parameter | Cutoff | AUC | Sensitivity | Specificity | PPV | NPV |
|---|---|---|---|---|---|---|---|---|---|---|---|---|
| Hang et al.[ | 244 | 289 | 170 | 2D-SWE | Aixplorer | YM (kPa) mean | 69 | 0.76 | 75.3 | 75.3 | — | — |
| Sebag et al.[ | 93 | 146 | 29 | 2D-SWE | Aixplorer | YM (kPa) mean | 65 | 0.93 | 85.2 | 85.2 | 80.0 | 95.9 |
| Veyrieres et al.[ | 148 | 297 | 35 | 2D-SWE | Aixplorer | YM (kPa) mean | 66 | 0.85 | 80.0 | 80.0 | — | 97.1 |
| Kim et al.[ | 99 | 99 | 21 | 2D-SWE | Aixplorer | YM (kPa) mean | 62 | 0.76 | 66.6 | 66.6 | 40.6 | 85.7 |
AUC, area under the curve; PPV, positive predictive value; NPV, negative predictive value; YM, Young’s modulus.
SuperSonic Imagine; Aix-en-Provence, France.