用微波和光学系统测量的风波槽中的波-波相互作用

M. Keller, B. Gotwols, W. Plant, W. Keller
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摘要

长期以来,人们一直认为来自海洋表面的微波反向散射与布拉格共振波长的风波的光谱密度成正比。虽然重力-毛细波的谱密度主要是风强迫的函数,但与较长波的相互作用也是波-波能量传递的重要因素。因此,微波后向散射也会受到较长波的影响。任何测量较长波对后向散射的影响的努力,通常被称为调制传递函数,或mtf:应该包括直接测量后向散射和直接测量短波频谱密度。作者使用了10 GHz (x波段)、35 GHz (K/sub /spl alpha//波段)和70 GHz (V波段)的微波和毫米波散射计来测量反向散射。三种微波仪器都是连续波多普勒系统。x波段散射计将多普勒偏移400赫兹,这样就可以记录顺风和顺风的峰值。其余系统是I&Q仪器,其中射频信号调制60 MHz载波,I&Q在单独的部分从60 MHz载波中检索。用PC机的数据转换a /D卡对3khz的微波信号进行采样,数据存储在8mm EXABYTE型存储器中。微波和光学系统都对准了水面上的同一点,距离16.5米。
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Wave-wave interactions in a wind-wavetank as measured with microwave and optical systems
Microwave backscatter from the ocean surface has long been assumed to be proportional to the spectral density of windwaves at the Bragg-resonant wavelength. Although the spectral density of gravity-capilary waves is primarily a function of wind forcing, interactions with longer waves are also an important factor in wave-wave energy transfer. Thus, the microwave backscatter should be affected by the presence of longer waves as well. Any effort to measure the effects of longer waves on the backscatter, usually referred to as the modulation transfer function, or mtf: should include both direct measurement of the backscatter and direct measurement of the short-wave spectral density. The authors have used microwave and millimeter-wave scatterometers at 10 GHz (X-band), 35 GHz (K/sub /spl alpha// band), and 70 GHz (V band) to measure the backscatter. All three microwave instruments are CW Doppler systems. The X-band scatterometer offsets the Doppler by 400 Hz so both the upwind and downwind peaks can recorded. The remaining systems are I&Q instruments, where the RF signal modulates a 60 MHz carrier wave, and the I&Q are retrieved from the 60 MHz carrier in a separate section. The microwave signals are sampled at 3 kHz using a Data Translation A/D card in a PC, and the data are stored on 8 mm EXABYTE type. The microwave and optical systems were all aligned to view the same spot on the water, at a fetch of 16.5 meters.<>
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