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A dealiasing method for use with ultrasonic pulsed Doppler in measuring velocity profiles and flow rates in pipes

机译:与超声脉冲多普勒一起使用的脱气方法,用于测量管道中的速度分布和流速

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The ultrasonic pulsed Doppler method (UDM) is a powerful tool for measuring velocity profiles in a pipe. However, the maximum detectable velocity is limited by the Nyquist sampling theorem. Furthermore, the maximum detectable velocity (also called Nyquist velocity), v(max), and the maximum measurable length are related and cannot be increased at the same time. If the velocity is greater than vmax, velocity aliasing occurs. Hence, the higher velocity that occurs with a larger pipe diameter, i.e. under higher flow rate conditions, cannot be measured with the conventional UDM. To overcome these limitations, dual-pulse repetition frequency (dual PRF) and feedback methods were employed in this study to measure velocity profiles in a pipe. The velocity distributions obtained with the feedback method were found to be more accurate than those obtained with the dual PRF method. However, misdetection of the Nyquist folding number using the feedback method was found to increase with the flow velocity. A feedback method with a moving average is proposed to improve the measurement accuracy. The method can accurately measure the velocity distributions at a velocity five times greater than the maximum velocity that can be measured with the conventional UDM. The measurement volume was found to be among the important parameters that must be considered in assessing the traceability of the reflector during the pulse emission interval. Hence, a larger measurement volume is required to measure higher velocities using the dual PRF method. Integrating velocity distributions measured using the feedback method with a moving average makes it possible to accurately determine flow rates six times greater than those that can be determined using the conventional pulsed Doppler method.
机译:超声脉冲多普勒方法(UDM)是用于测量管道中速度分布的强大工具。但是,最大可检测速度受到奈奎斯特采样定理的限制。此外,最大可检测速度(也称为奈奎斯特速度),v(max)和最大可测量长度是相关的,不能同时增加。如果速度大于vmax,则会发生速度混叠。因此,用传统的UDM无法测量在较大管径下(即在较高流速条件下)发生的较高速度。为了克服这些限制,在这项研究中采用了双脉冲重复频率(双PRF)和反馈方法来测量管道中的速度分布。发现通过反馈方法获得的速度分布比通过双重PRF方法获得的速度分布更准确。然而,发现使用反馈方法对奈奎斯特折叠数的错误检测随着流速的增加而增加。为了提高测量精度,提出了一种具有移动平均的反馈方法。该方法可以以比常规UDM可以测量的最大速度大五倍的速度精确测量速度分布。发现测量体积是评估脉冲发射间隔期间反射器的可追溯性必须考虑的重要参数之一。因此,使用双重PRF方法需要更大的测量量来测量更高的速度。将使用反馈方法测得的速度分布与移动平均值相结合,可以精确确定比使用常规脉冲多普勒方法确定的流速大六倍的流速。

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