| Literature DB >> 35215636 |
Chuang-Yen Huang1, Kuo-Min Su1, Hsueh-Hsing Pan2,3, Fung-Wei Chang1, Yu-Ju Lai1, Hung-Chih Chang4, Yu-Chi Chen4, Chi-Kang Lin1, Kuo-Chih Su4,5,6.
Abstract
During certain clinical situations, some parturients require instruments for operative vaginal delivery, and various designs of vacuum extractors may affect the fetal head. To investigate the biomechanical effects of divergent sizes of silicone rubber vacuum extractors, we employed finite element analysis in this study. First, we constructed computer models for different vacuum extractor sizes (diameters: 40 mm, 50 mm, 60 mm, and 70 mm), flat surface, hemispherical ball, and fetal head shape. A hemispherical ball was the main design for the vacuum extractor model, and the material used for the vacuum extractor was silicone rubber. Next, the settings of 1 mm vacuum extractor displacement and vacuum cap pressure of 60 cmHg were applied. The main observation markers of this study were the respective von Mises stresses on the vacuum extractor and skull by the reaction force on the fixed end. The concluded results revealed that vacuum extractors with larger diameters lead to greater reaction force, stress, and strain on fetal heads. Therefore, this study's biomechanical analytic consequences suggest that clinicians avoid selecting larger vacuum extractors during operative instrumental delivery so that fetal heads will experience less external force, deformation, and resultant complications. It could also provide a practical reference for obstetricians for instrumental vaginal delivery with the vacuum extractor made of silicone rubber.Entities:
Keywords: biomechanics; finite element analysis; operative delivery; silicone rubber vacuum extractors
Year: 2022 PMID: 35215636 PMCID: PMC8879916 DOI: 10.3390/polym14040723
Source DB: PubMed Journal: Polymers (Basel) ISSN: 2073-4360 Impact factor: 4.329
Figure 1Computer models of 4 vacuum extractors with different sizes.
Figure 2Finite element analysis computer models of vacuum extractors acting on flat surface, hemispherical ball, and fetal head.
Figure 3Two load conditions (internal pressure of vacuum extractors and vacuum extractor displacement).
Figure 4Location of boundary condition and load condition in the finite element analysis computer model.
Material properties setting in this study [24,25].
| Material | Young’s Modulus (MPa) | Poisson’s Ratio |
|---|---|---|
| Scalp | 16.7 | 0.42 |
| Skull | 2500 | 0.22 |
| Silicone rubber | 10.3 | 0.49 |
Figure 5Finite element analysis computer model mesh status of vacuum extractors acting on flat surface, hemispherical ball, and fetal head.
Number of nodes and elements in the computer finite element analysis model used in this study.
| Different Shapes | Mesh | 40 mm | 50 mm | 60 mm | 70 mm |
|---|---|---|---|---|---|
| Flat surface | Nodes | 26,708 | 39,160 | 58,294 | 70,466 |
| Elements | 6127 | 9253 | 14,068 | 17,244 | |
| Hemispherical ball | Nodes | 38,822 | 48,834 | 51,177 | 66,890 |
| Elements | 10,721 | 12,542 | 13,141 | 17,134 | |
| Fetal head | Nodes | 130,054 | 131,198 | 132,961 | 134,778 |
| Elements | 64,734 | 65,270 | 66,097 | 66,969 |
Reaction forces of various fixed ends.
| Different Shapes | 40 mm | 50 mm | 60 mm | 70 mm | |
|---|---|---|---|---|---|
| Flat surface | X Axis | 1.0443 × 10−12 N | 3.2591 × 10−11 N | 1.2457 × 10−11 N | 3.3406 × 10−14 N |
| Y Axis | −14.993 N | −15.881 N | −16.836 N | −18.065 N | |
| Z Axis | 6.9628 × 10−12 N | −4.036 × 10−11 N | −1.9115 × 10−11 N | 4.4828 × 10−12 N | |
| Total | 14.993 N | 15.881 N | 16.836 N | 18.065 N | |
| Hemispherical ball | X Axis | 2.1072 × 10−10 N | 6.9963 × 10−11 N | −1.7853 × 10−10 N | −2.5786 × 10−10 N |
| Y Axis | −14.331 N | −15.369 N | −16.491 N | −17.568 N | |
| Z Axis | 1.1635 × 10−10 N | −2.0118 × 10−13 N | −7.1072 × 10−11 N | 6.4573 × 10−12 N | |
| Total | 14.331 N | 15.369 N | 16.491 N | 17.568 N | |
| Fetal head | X Axis | 6.132 × 10−5 N | 1.5367 × 10−4 N | −4.1151 × 10−5 N | 7.9199 × 10−5 N |
| Y Axis | −14.303 N | −15.212 N | −16.206 N | −17.406 N | |
| Z Axis | −3.5533 × 10−6 N | 1.4878 × 10−4 N | −1.1716 × 10−5 N | −1.3267 × 10−4 N | |
| Total | 14.303 N | 15.212 N | 16.206 N | 17.406 N |
Stiffness value for different groups.
| Stiffness | 40 mm | 50 mm | 60 mm | 70 mm |
|---|---|---|---|---|
| Flat surface | 14.993 N/mm | 15.881 N/mm | 16.836 N/mm | 18.065 N/mm |
| Hemispherical ball | 14.331 N/mm | 15.369 N/mm | 16.491 N/mm | 17.568 N/mm |
| Fetal head | 14.303 N/mm | 15.212 N/mm | 16.206 N/mm | 17.406 N/mm |
Figure 6von Mises stress distribution on different vacuum extractors.
Figure 7von Mises strain distribution on different vacuum extractors.
Figure 8von Mises stress distribution on skull materials when vacuum extractors act on different shapes.
Figure 9von Mises strain distribution on skull materials when vacuum extractors act on different shapes.
Figure 10Content in the Mechanics of Material textbook was used for explanation. The greater the sphere size (inner radius r), the greater the force [27].