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Non-invasive estimation of the mean pressure difference in aortic stenosis by Doppler ultrasound.

机译:多普勒超声无创估计主动脉瓣狭窄的平均压差。

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摘要

The mean pressure difference across the valve in aortic stenosis is an indicator of the severity of the obstruction to flow. Non-invasive determination of the mean pressure gradient by Doppler ultrasonography is, however, complicated by the squared relation between instantaneous velocities and pressure differences. The validity of a new simple formula for calculation of the mean pressure difference from the peak pressure difference was evaluated in 26 patients with aortic stenosis. The formula is: delta pmean = 0.64 delta ppeak, where delta pmean is the mean pressure gradient and delta ppeak the peak pressure gradient. There was a close correlation between the mean pressure differences determined by application of the formula to the peak pressure differences measured at catheterisation and the mean pressure differences obtained by planimetry (r = 0.97, SEE = 4.7 mm Hg). The correlation between mean pressure differences determined by continuous wave Doppler ultrasound and the formula and those measured by planimetry was also close (r = 0.91, SEE = 7.6 mm Hg) and only three patients showed a difference between the two methods of greater than 10 mm Hg. The new formula is a simple and reliable means of estimating the mean pressure difference from Doppler recordings and it facilitates the comparison of Doppler and catheterisation data.
机译:主动脉瓣狭窄时跨瓣的平均压力差是阻塞的严重程度的指标。但是,由于瞬时速度和压力差之间的平方关系,通过多普勒超声对平均压力梯度的非侵入式测定变得复杂。在26例主动脉瓣狭窄患者中评估了一个新的简单公式从峰值压力差计算平均压力差的有效性。计算公式为:delta pmean = 0.64 delta ppeak,其中delta pmean是平均压力梯度,而delta ppeak是峰值压力梯度。通过对导管插入术中测得的峰值压力差应用公式确定的平均压力差与通过平面测量获得的平均压力差之间存在密切相关性(r = 0.97,SEE = 4.7 mm Hg)。由连续波多普勒超声确定的平均压力差与公式和通过平面测量法测得的平均压力差之间的相关性也很接近(r = 0.91,SEE = 7.6 mm Hg),只有三名患者显示两种方法之间的差值大于10 mm汞新公式是一种简单可靠的方法,可从多普勒记录中估算出平均压力差,并且有助于对多普勒和导管插入数据进行比较。

著录项

  • 作者

    Teien, D; Karp, K; Eriksson, P;

  • 作者单位
  • 年度 1986
  • 总页数
  • 原文格式 PDF
  • 正文语种 en
  • 中图分类
  • 入库时间 2022-08-31 15:29:22

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