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影响无源传导植入物最坏情况梯度场加热的参数。

Parameters Affecting Worst-Case Gradient-Field Heating of Passive Conductive Implants.

机构信息

Division of Biomedical Physics, Center for Devices and Radiological Health, US Food and Drug Administration, Maryland, USA.

出版信息

J Magn Reson Imaging. 2022 Oct;56(4):1197-1204. doi: 10.1002/jmri.28321. Epub 2022 Jul 1.

Abstract

BACKGROUND

Testing MRI gradient-induced heating of implanted medical devices is required by regulatory organizations and others. A gradient heating test of the ISO 10974 Technical Specification (TS) for active implants was adopted for this study of passive hip implants. All but one previous study of hip implants used nonuniform gradient exposure fields in clinical scanners and reported heating of less than 5 °C. This present study adapted methods of the TS, addressing the unmet need for identifying worst-case heating via exposures to uniform gradient fields.

PURPOSE

To identify gradient-field parameters affecting maximum heating in vitro for a hip implant and a cylindrical titanium disk.

STUDY TYPE

Computational simulations and experimental validation of induced heating.

PHANTOM

Tissue-simulating gel.

FIELD STRENGTH

42 T/s RMS, sinusoidal, continuous B fields with high spatial uniformity ASSESSMENT: Hip implant heating at 1-10 kHz, via computational modeling, validated by limited point measurements. Experimental measurements of exposures of an implant at 42 T/s for 4, 6, and 9 kHz, analyzed at 50, 100, and 150 seconds.

STATISTICAL TESTS

One sample student's t-test to assess difference between computational and experimental results. Experimental vs. computational results were not significantly different (p < 0.05).

RESULTS

Maximum simulated temperature rise (10-minute exposure) was 10 °C at 1 kHz and 0.66 °C at 10 kHz. The ratio of the rise for 21 T/s vs. 42 T/s RMS was 4, after stabilizing at 50 seconds (dB/dt ratio squared).

DATA CONCLUSIONS

Heating of an implant is proportional to the frequency of the B field and the implant's cross-sectional area and is greater for a thickness on the order of its skin depth. Testing with lower values of dB/dt RMS with lower cost amplifiers enables prediction of heating at higher values for dB/dt squared (per ISO TS) with identical frequency components and waveforms, once thermal equilibrium occurs.

EVIDENCE LEVEL

1 TECHNICAL EFFICACY: Stage 1.

摘要

背景

监管机构和其他机构要求对植入式医疗器械的 MRI 梯度感应加热进行测试。本研究采用 ISO 10974 技术规范(TS)中针对有源植入物的梯度加热测试来测试无源髋关节植入物。除了一项之前对髋关节植入物的研究外,所有研究都在临床扫描仪中使用非均匀梯度照射场,并报告了低于 5°C 的加热。本研究采用了 TS 的方法,通过暴露于均匀梯度场来满足确定最坏情况下加热的需求。

目的

确定髋关节植入物和圆柱形钛盘在体外产生最大加热的梯度场参数。

研究类型

感应加热的计算模拟和实验验证。

仿体

组织模拟凝胶。

磁场强度

42 T/s 均方根值,正弦连续 B 场,具有高空间均匀性。

评估

通过计算建模评估髋关节植入物在 1-10 kHz 下的加热情况,并通过有限点测量进行验证。在 42 T/s 下对植入物进行 4、6 和 9 kHz 的暴露实验,在 50、100 和 150 秒时进行分析。

统计检验

采用单样本学生 t 检验评估计算结果和实验结果之间的差异。实验结果与计算结果无显著差异(p<0.05)。

结果

在 1 kHz 时,模拟的最大温升(10 分钟暴露)为 10°C,在 10 kHz 时为 0.66°C。在 50 秒后达到稳定时(平方 dB/dt 比),21 T/s 与 42 T/s 均方根值的上升比为 4。

数据结论

植入物的加热与 B 场的频率和植入物的横截面积成正比,并且对于厚度接近其趋肤深度的植入物,加热更大。使用具有较低成本放大器的较低 dB/dt RMS 值进行测试,可以预测在相同频率成分和波形下,dB/dt 平方(符合 ISO TS)更高值的加热,一旦达到热平衡。

证据水平

1 技术功效:阶段 1。

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