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Quantifying errors due to frequency changes and target location uncertainty for radar refractivity retrievals

机译:量化由于频率变化和目标位置不确定性导致的雷达折射率检索误差

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摘要

Radar refractivity retrievals can capture near-surface humidity changes, but noisy phase changes of the ground clutter returns limit the accuracy for both klystron- and magnetron-based systems. Observations with a C-band (5.6 cm) magnetron weather radar indicate that the correction for phase changes introduced by local oscillator frequency changes leads to refractivity errors no larger than 0.25 N units: equivalent to a relative humidity change of only 0.25% at 20°C. Requested stable local oscillator (STALO) frequency changes were accurate to 0.002 ppm based on laboratory measurements. More serious are the random phase change errors introduced when targets are not at the range-gate center and there are changes in the transmitter frequency (ΔfTx) or the refractivity (ΔN). Observations at C band with a 2-μs pulse show an additional 66° of phase change noise for a ΔfTx of 190 kHz (34 ppm); this allows the effect due to ΔN to be predicted. Even at S band with klystron transmitters, significant phase change noise should occur when a large ΔN develops relative to the reference period [e.g., ~55° when ΔN = 60 for the Next Generation Weather Radar (NEXRAD) radars]. At shorter wavelengths (e.g., C and X band) and with magnetron transmitters in particular, refractivity retrievals relative to an earlier reference period are even more difficult, and operational retrievals may be restricted to changes over shorter (e.g., hourly) periods of time. Target location errors can be reduced by using a shorter pulse or identified by a new technique making alternate measurements at two closely spaced frequencies, which could even be achieved with a dual–pulse repetition frequency (PRF) operation of a magnetron transmitter.
机译:雷达折射率检索可以捕获近地表的湿度变化,但是地面杂波回波的嘈杂相位变化会限制速调管和磁控管系统的精度。用C波段(5.6厘米)磁控管气象雷达进行的观测表明,由本地振荡器频率变化引起的相位变化校正会导致折射率误差不大于0.25 N单位:相当于20°C时相对湿度变化仅为0.25% C。根据实验室测量,要求的稳定本地振荡器(STALO)频率变化精确到0.002 ppm。更严重的是,当目标不在测距门中心并且发射器频率(ΔfTx)或折射率(ΔN)有变化时,会引入随机相变误差。在C波段以2 µs脉冲进行的观察表明,对于ΔkHz,ΔfTx为190 kHz(34 ppm)时,会产生另外的66°相变噪声。这使得可以预测由于ΔN引起的影响。即使在速调管发射机的S波段,当相对于参考周期产生较大的ΔN时(例如,对于下一代气象雷达(NEXRAD)雷达,当ΔN= 60时约为55°),也应出现明显的相变噪声。在较短的波长(例如C和X波段)处,尤其是在磁控管发射机的情况下,相对于较早参考周期的折射率检索甚至更加困难,并且操作检索可能会限于较短(例如每小时)时间段内的变化。目标位置误差可以通过使用更短的脉冲来减少,或者通过一种新技术来识别,该技术可以在两个紧密间隔的频率上进行交替测量,甚至可以通过磁控管发射机的双脉冲重复频率(PRF)操作来实现。

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