IEEE GEOSCIENCE AND REMOTE SENSING LETTERS, VOL. 10, NO. 3, MAY 2013 593
Estimation of the Sea-Surface Slope Variance
Based on the Power Spectrum Width
of a Radar Scatterometer
Min-Ho Ka, Member, IEEE, Aleksandr I. Baskakov, Vladimir A. Terechov, and Anatoliy A. Kononov
Abstract—In this letter, we introduce the possibility of the
sea-surface slope measurements using second-order statistics of
return waveforms from sea surface in a continuous-wave radar
scatterometer. It has been shown that the estimation of the vari-
ance of sea-surface slopes can be obtained by measuring the signal
power or the power-spectrum width of return waveforms. We
found that the power-spectrum-width-based estimation approach
is more sensitive to the variance of the sea-surface slope for weak
sea-surface disturbances in contrast to the power-based one.
Index Terms—Correlation function, power spectrum, radar
scatterometer, remote sensing, sea slope variance.
I. I NTRODUCTION
R
EAL-TIME monitoring of the sea-state condition and
other processes associated with the ocean surface dynam-
ics is necessary for reliable weather forecasts over continents
and oceans, as well as for other applications such as navigation,
scientific study of air and sea interaction, and global climate
phenomena [1], [2]. Thus, the development of methods and
remote-sensing instruments for real-time sea-state condition
measurement is of great current importance [3]–[6]. The inter-
est in rapid, accurate, and global scale measurements of the sea
state has favored the development of radar systems either in
high frequency or in the microwave domain. The microwave
sensors have the advantage of being usable in aircraft, as well
as in space platforms [2] [4] [5]. One of the on-board sensors
providing useful data on ocean surface (wind measurement) is
the microwave radar scatterometer. It can even operate from
small space platforms due to the advantage of low cost and low
power requirements. In addition to ocean wind measurements,
scatterometer data are also valuable in ice mapping, vegetation
classification, soil moisture retrieval, etc. [1], [2].
Manuscript received February 8, 2012; revised July 3, 2012; accepted
August 13, 2012. Date of publication October 11, 2012; date of current version
November 24, 2012. This work was supported by the Ministry of Knowledge
Economy under the “IT Consilience Creative Program” by the National IT
Industry Promotion Agency Korea.
M.-H. Ka is with the School of Integrated Technology, Yonsei University,
Incheon 406-840, Korea (e-mail: kaminho@yonsei.ac.kr).
A. I. Baskakov and V. A. Terechov are with Moscow Power Engineering
Institute, 111250 Moscow, Russia (e-mail: baskakovai@mpei.ru).
A. A. Kononov is with the STX Engine Corporation, Gyeonggi-do 449-915,
Korea (e-mail: kaa50ua@gmail.com).
Digital Object Identifier 10.1109/LGRS.2012.2215305
TABLE I
RELATION BETWEEN NEAR-SURFACE WIND AND SEA SLOPE VARIANCE
This letter addresses some issues related to the principle of
measurement to be employed in a down-looking continuous-
wave (CW) radar scatterometer that should be capable of pro-
viding accurate data on the variance of the sea-surface slope
from aircraft or small space platforms. The scatterometer does
not directly measure the wind. Instead, it measures variance
σ
2
θ
of the sea-surface slope. To infer the wind speed, the σ
2
θ
measurements should be then related to the near-surface wind
via appropriate geophysical model function. An example of
such a function in tabulated form is presented in Table I [7].
We will show that an estimate of the sea-surface slope
variance σ
θ2
can be extracted by measuring either the power-
spectrum width or the power of return waveforms. It will be
also shown that the spectral-width-based estimate exhibits high
sensitivity to the sea slope variance for weak sea disturbance.
II. RETURN WAVEFORM MODEL
The geometry for near-vertical sea-surface illumination (in-
cidence angle θ ≤ 15
◦
) in a down-looking radar scatterometer
is shown in Fig. 1.
The scatterometer, located at point A(0, 0,Z
0
), which is at
height H (Z
0
= H) above the mean flat sea surface, is assumed
to radiate monochromatic microwave signals at frequency ω
or wavelength λ. The XY plane corresponds to the mean flat
surface. Origin O of the coordinate system corresponds to the
projection of point A on the mean flat surface and moves
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