"你能感觉到吗?":一个早期的经验与模拟振动来重建状腺发声
Jason A Strelzow1, Jonathan R Kusins2, Louis M Ferreira2,3
1The University of Chicago Medicine, Department of Orthopaedic Surgery and Rehabilitation Medicine, Chicago, Illinois.
JB & JS open access
|June 28, 2023
概括
这项研究引入了一种用于肩膀关节整形训练的新型模拟器,成功地复制了状腺回振动. 专家外科医生验证了它的高保真性和作为外科模拟教育工具的实用性.
科学领域:
- 生物医学工程 生物医学工程
- 外科教育的外科教育
- 整形外科 整形外科 整形外科
背景情况:
- 触觉反对于外科手术中有效的教育模拟器至关重要.
- 在可用的模拟器中存在一个缺口,用于肩膀关节整形手术程序.
- 开发现实的模拟器可以提高外科训练和患者的治疗效果.
研究的目的:
- 开发和验证一款用于肩部关节整形的新型模拟器,专注于模拟状腺回振动.
- 用专家外科医生评估来评估模拟器的触觉反忠实度.
- 为了确定这个模拟器作为训练辅助器的潜力.
主要方法:
- 使用振动传感器和3D打印的眼膜,建造了一个定制的模拟器.
- 九名受过培训的肩部外科医生通过模拟的回忆任务来评估模拟器的忠实性.
- 验证后的调查问卷评估了专家外科医生的经验和感知到的效用.
主要成果:
- 专家在识别表面形状 (52%) 和软骨层 (69%) 中取得了高准确度.
- 模拟器在区分软骨和亚冠骨 (77%) 中表现出高准确度.
- 该模拟器在作为教学工具的实用性 (4/5) 和现实性 (4.11/5) 方面获得了高评分.
结论:
- 开发的状腺回忆模拟器有效模拟振动触觉.
- 专家验证证实了模拟器的高保真性和作为一个有价值的培训工具的潜力.
- 这款新型模拟器可以作为额外的辅助剂,用于肩膀关节整形手术培训.
相关概念视频
Deformation in a Circular Shaft
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One of the distinctive characteristics of circular shafts is their ability to maintain their cross-sectional integrity under torsion. In other words, each cross-section continues to exist as a flat, unaltered entity, simply rotating like a solid, rigid slab. To understand the distribution of shearing stress within such a shaft, consider a cylindrical section inside this circular shaft. This section has a length of L and a radius of R, with one end fixed. The radius of the cylindrical section is...
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Residual Stresses in Circular Shafts
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In materials that exhibit elastic and plastic behavior, known as elastoplastic materials, residual stresses can accumulate when these materials experience plastic deformation. This deformation arises from either high levels of shearing stress or significant strains. Residual stresses are internal stresses that persist within a material after removing the external force causing deformation. This phenomenon is demonstrated when observing the behavior of a shaft under torque; notably, the...
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Circular Shaft - Stresses in Linear Range
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Consider a scenario where a circular shaft is subject to torque that remains within the boundaries of Hooke's Law, avoiding any permanent deformation. So, the formula for shearing strain is revisited. This formula is multiplied by the modulus of rigidity, and then Hooke's Law for the shearing stress and strain is applied. As a result, the equation for shearing stress in a shaft can be derived.
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