<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">ACS</journal-id><journal-title-group><journal-title>Atmospheric and Climate Sciences</journal-title></journal-title-group><issn pub-type="epub">2160-0414</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/acs.2016.63034</article-id><article-id pub-id-type="publisher-id">ACS-67799</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Earth&amp;Environmental Sciences</subject></subj-group></article-categories><title-group><article-title>
 
 
  Profile and Precipitation Retrievals and Validation Based on Geostationary Sub-Millimeter Atmospheric Sounder
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Jieying</surname><given-names>He</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Shengwei</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hao</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ying</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Key Laboratory of Microwave Remote Sensing, National Space Science Center, Chinese Academy of Sciences, Beijing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>hejieying@mirslab.cn(JH)</email>;<email>hejieying@mirslab.cn(SZ)</email>;<email>hejieying@mirslab.cn(HL)</email>;<email>hejieying@mirslab.cn(YZ)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>23</day><month>05</month><year>2016</year></pub-date><volume>06</volume><issue>03</issue><fpage>415</fpage><lpage>424</lpage><history><date date-type="received"><day>4</day>	<month>May</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>26</month>	<year>June</year>	</date><date date-type="accepted"><day>29</day>	<month>June</month>	<year>2016</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  The key factors of temporal and spatial resolution for typhoon observation played an important role in the design of radiometer used for observing typhoon. The NCEP (National Centres for Environmental Prediction) operational global analysis data prepared operationally every six hours were used as the initial field for mesoscale weather research and forecasting model (WRF) and drove the model to output atmospheric parameters such as hydrometeor content, temperature and humidity profiles at different time, which were inputs for the Atmospheric Radiative Transfer Simulator (ARTS) to calculate brightness temperature observed from geostationary earth orbit at oxygen absorption and water absorption band. The atmospheric humidity and temperature profiles of typhoon domain were retrieved from geostationary sub-millimetre atmospheric sounder. The results show that the profile retrievals using BP-NN algorithm have a best agreement with those from radiosonde, which is less than 20% and 1 K of root mean square error, respectively. For precipitation rate retrievals, much better agreement with rain gauge and ECMWF datasets, the RMS is between 0.84 to 32.4 mm/h for sea surface 0.89 and 36.13 mm/h for land surface according to the classification by precipitation type. 
   
  
 
</p></abstract><kwd-group><kwd>Atmospheric</kwd><kwd> Profile</kwd><kwd> Precipitation</kwd><kwd> Geostationary Sub-Millimetre Atmospheric Sounder</kwd><kwd> Neural Network</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The current polar-orbiting meteorological satellite observation system ensures that the observation period is six hours, which is unable to monitor typhoon and other fast changing situations. Only instruments on geostationary or comparable platforms can view regional disaster at the 15-min interval that is necessary to monitor rapidly evolving typhoon or cyclone events. This paper discusses the abilities of passive microwave/ sub-millimeter sensor which is being developed by our institute to retrieve atmospheric temperature and humidity profiles. Furthermore, we also carry out the work of retrieving surface precipitation rates and hydrometeor water paths.</p><p>Geostationary atmospheric sounder based on interferometric technology is the newest field of microwave remote sensing. Equipped with a sub-millimeter atmospheric remote sensing instruments on the geostationary orbit, meteorological satellite platform will increase the frequency of observations, at the same time, improve the cloud detection capability [<xref ref-type="bibr" rid="scirp.67799-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.67799-ref3">3</xref>] .</p></sec><sec id="s2"><title>2. Instrument Description</title><p>According to the atmospheric sounding theory and gasous absorption coefficients from 0 - 1000 GHz, the final frequencies are chosen to derive atmospheric temperature and humidity profiles for geostationary sub-millimeter sounder, which are list in <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="table" rid="table1">Table 1</xref>, <xref ref-type="table" rid="table2">Table 2</xref> shows characteristics of ultimately selected frequencies and their applications.</p><p>Since atmospheric absorbing characteristics of water vapor and oxygen, using satellite-borne microwave radiometer to derive atmospheric temperature and humidity profiles is possible. According to the principle above,</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The standard atmospheric profiles</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x6.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Candidate frequencies for geostationary sub-millimeter sounder</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >No.</th><th align="center" valign="middle" >Frequency (GHz)</th><th align="center" valign="middle" >Characteristics</th><th align="center" valign="middle" >Applications</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >55 - 64</td><td align="center" valign="middle" >Oxygen</td><td align="center" valign="middle" >Temperature profiles</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >118.75</td><td align="center" valign="middle" >Oxygen</td><td align="center" valign="middle" >Temperature profiles</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >150.0</td><td align="center" valign="middle" >window</td><td align="center" valign="middle" >Surface information</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >183.31</td><td align="center" valign="middle" >Water vapor</td><td align="center" valign="middle" >Humidity profiles</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >220.0</td><td align="center" valign="middle" >Window</td><td align="center" valign="middle" >Surface information</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >380.19</td><td align="center" valign="middle" >Water vapor</td><td align="center" valign="middle" >Humidity profiles</td></tr><tr><td align="center" valign="middle" >7</td><td align="center" valign="middle" >424.76</td><td align="center" valign="middle" >Oxygen</td><td align="center" valign="middle" >Temperature profiles</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >556.93</td><td align="center" valign="middle" >Water vapor</td><td align="center" valign="middle" >Humidity profiles</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Characteristics of ultimately selected frequencies</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >No.</th><th align="center" valign="middle" >Frequency (GHz)</th><th align="center" valign="middle" >Characteristics</th><th align="center" valign="middle" >Applications</th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >118.75</td><td align="center" valign="middle" >Oxygen</td><td align="center" valign="middle" >Temperature profiles</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >183.31</td><td align="center" valign="middle" >Oxygen</td><td align="center" valign="middle" >Humidity profiles</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >380.197</td><td align="center" valign="middle" >Window</td><td align="center" valign="middle" >Humidity profiles</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >424.763</td><td align="center" valign="middle" >Water vapor</td><td align="center" valign="middle" >Temperature profiles</td></tr></tbody></table></table-wrap><p>when the radiometer operated at frequencies 50 - 1000 GHz, the contribution of surface background noise can be reduced to negligible magnitude, because the transmittance of the atmosphere at these frequencies is approximately equal to 0.</p><p>Atmospheric opacity thickness with pressure integration can be expressed as:</p><disp-formula id="scirp.67799-formula1857"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x7.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x8.png" xlink:type="simple"/></inline-formula> is atmospheric at altitude z, z' is height from surface to satellite.</p><p>For oxygen absorbing channels, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x9.png" xlink:type="simple"/></inline-formula>is basically due to the contribution of oxygen.</p><p>Equation (1) can be expressed as the weighted integral of temperature:</p><disp-formula id="scirp.67799-formula1858"><label>. (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x10.png"  xlink:type="simple"/></disp-formula><p>The temperature weighing function can be expressed as:</p><disp-formula id="scirp.67799-formula1859"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x11.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.67799-formula1860"><label>. (4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x12.png"  xlink:type="simple"/></disp-formula><p>Furthermore, water vapor weighing function can be expressed as:</p><disp-formula id="scirp.67799-formula1861"><label>. (5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x13.png"  xlink:type="simple"/></disp-formula><p>Weighting function is the weight of atmospheric radiance at height z from surface to the height of the satellite. The plane parallel atmosphere was divided into N layers, the absorbing coefficient of atmospheric parameters was assumed uniform in each layer, and then attenuation contributions of entire atmosphere including the surface layer can be accumulated. Atmospheric absorbing coefficients in each channel can be calculated combining MPM93 [<xref ref-type="bibr" rid="scirp.67799-ref4">4</xref>] and PWR04 [<xref ref-type="bibr" rid="scirp.67799-ref5">5</xref>] model. Therefore, we can choose the central frequency and bandwidth for each channel of geostationary sub-millimeter atmospheric sounder according to the weighting functions, which is displayed in <xref ref-type="fig" rid="fig2">Figure 2</xref>.</p></sec><sec id="s3"><title>3. Data Processing</title><sec id="s3_1"><title>3.1. Simulation of Full-Disk Model of Earth</title><p>Brightness temperatures are simulated by the validated global reference physical model, NCEP/WRF/ARTS, composed of the US National Center for Environment Prediction (NCEP) analyses, the new generation National Center for Atmospheric Research/Penn State Mesoscale Model (WRF) and the Atmospheric Radiative Transfer Simulator, ARTS, which is a software for performing simulations of atmospheric radiative transfer [<xref ref-type="bibr" rid="scirp.67799-ref6">6</xref>] - [<xref ref-type="bibr" rid="scirp.67799-ref9">9</xref>] . The output of WRF model consists of temperature and humidity profiles, pressure profiles, surface mask, and surface parameters and so on.</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The standard atmospheric profiles.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x14.png"/></fig><fig id ="fig2_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x15.png"/></fig></fig-group><p>By using the WRF (weather research and forecasting) model, the paper simulated the seasonal tropical cyclone activity over western North Pacific at 53.596 GHz from 1 June to 30 September 2015, like <xref ref-type="fig" rid="fig3">Figure 3</xref> shows. Therefore the results show that: 1) the simulated total number of Typhoons is close to that from Best-track dataset; 2) The simulated intensity of typhoons is comparable to that from Best-track data set, but the time limit needs further exploration.</p></sec><sec id="s3_2"><title>3.2. Observation from MWHTS</title><p>Until now, no observation data from geostationary satellite can be used to realize the profile and precipitation rates retrievals. To solve this problem, this paper uses the observing data from microwave humidity and temperature sounder onboard FY-3C (FY-3C MWHTS) which plays an important role in monitoring extreme climate, especially for typhoon since September 30<sup>th</sup>, 2013, such as typhoon “kujira”, “Linfa”, “chan-hom” and “Nangka”, monitoring their procedure of generating, evolution, strengthen and die out (as showing in <xref ref-type="fig" rid="fig4">Figure 4</xref> and</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> Brightness temperature simulation for typhoon evolution. Time: 8, 9, 10, 11, 12 and 13 o’clock.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x17.png"/></fig><fig id ="fig3_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x16.png"/></fig><fig id ="fig3_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x19.png"/></fig><fig id ="fig3_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x18.png"/></fig><fig id ="fig3_5"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x21.png"/></fig><fig id ="fig3_6"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x20.png"/></fig></fig-group><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> Brightness temperatures distribution at different pressure-level at 118 GHz</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x22.png"/></fig><p><xref ref-type="fig" rid="fig5">Figure 5</xref>), especially locating the typhoon eye area clearly and intuitively with the resolution of 15 kilometers, and also predicting the heavy rainfall caused by typhoon for South China [<xref ref-type="bibr" rid="scirp.67799-ref10">10</xref>] - [<xref ref-type="bibr" rid="scirp.67799-ref12">12</xref>] .</p></sec></sec><sec id="s4"><title>4. Retrieval Algorithm</title><p>ANN is essentially a nonlinear statistical regression between a set of predictors (in this case the observation vectors X) and a set of predictands (in this case profiles of atmospheric temperature Z) [<xref ref-type="bibr" rid="scirp.67799-ref13">13</xref>] . The structure of the ANN is shown in <xref ref-type="fig" rid="fig6">Figure 6</xref>. In this paper, we construct a three layer ANN model. The layers 1, 2, and 3 represent the input layer, the hidden layer, and the output layer, respectively.</p><p>The neurons of the input layer are represented by vector X<sub>i</sub> (X<sub>1</sub>, X<sub>2</sub>, X<sub>3</sub>, ・・・, X<sub>L</sub>), where L is the number of the input neurons. The neurons of the middle layer are represented by vector Y<sub>i</sub> (Y<sub>1</sub>, Y<sub>2</sub>, Y<sub>3</sub>, ・・・, Y<sub>M</sub>), where M is the number of the hidden neurons. The neurons of the output layer are represented by vector Z<sub>i</sub> (Z<sub>1</sub>, Z<sub>2</sub>, Z<sub>3</sub>, ・・・, Z<sub>N</sub>), where N is the number of the output neurons.</p><p>The node in the hidden layer can be expressed as:</p><disp-formula id="scirp.67799-formula1862"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x23.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x24.png" xlink:type="simple"/></inline-formula>is the weighting of the connection between the j<sup>th</sup> hidden neuron and the i<sup>th</sup> input neuron and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x24.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x25.png" xlink:type="simple"/></inline-formula>denotes the bias in the j<sup>th</sup> neuron of the hidden layer. The linear function is applied between the output layer and the hidden layer. Where, S denotes the sigmoid function:</p><disp-formula id="scirp.67799-formula1863"><label>. (7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x26.png"  xlink:type="simple"/></disp-formula><p>According to the characteristics of sigmoid function, the values of both input and output layers should be transformed to the range [0, 1]. Outputs can be expressed as:</p><disp-formula id="scirp.67799-formula1864"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-4700494x27.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x28.png" xlink:type="simple"/></inline-formula> is the weight of the connection between the j<sup>th</sup> hidden neuron and the k<sup>th</sup> output neuron; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-4700494x29.png" xlink:type="simple"/></inline-formula>is the bias in the k<sup>th</sup> neuron of the output layer.</p><p>For geostationary sub-millimeter atmospheric sounder, several kinds of ANN are used according to the types of surface and sky, like land and sea, clear-sky, cloudy sky, rainy sky, typhoon-sky and so on. The schematic</p><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> Brightness temperatures distribution when three typhoons happened at July 7<sup>th</sup>, 2015. Left to right: Typhoon “Linfa”, “chan-hom” and “Nangka”</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x30.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> Schematic of retrieving flow</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x31.png"/></fig><p>algorithm is showed in <xref ref-type="fig" rid="fig7">Figure 7</xref>.</p></sec><sec id="s5"><title>5. Retrieval Results and Analysis</title><p><xref ref-type="fig" rid="fig8">Figure 8</xref> shows the profile retrievals of temperature and humidity (T&amp;H) using simulated brightness temperatures from microwave radiometer onboard gestational platform, which also gives the root mean square error distribution, respectively.</p><p>For the temperature profile, when there is a thin inversion layer, large deviations occur from the neural network retrieval model. It is mainly because of its own shortcoming for nonlinear neural network. When the inversion layer is thick enough, the neural network inverse model can be well reflected for the details of atmospheric temperature changes. Water vapor varies significantly from time to time and from space to space. Certainly the fact is that water vapor is the source of all clouds and precipitation which would be enough to explain its retrieving difficulties. Therefore compared to temperature, water vapor and relative humidity profiles are retrieved with relatively larger difficulty with challenge. The retrievals show that the RMS of atmospheric temperature profile is less than 2.5 K, RMS of atmospheric relative humidity profile is better than 20%, which can be converted to atmospheric absolute humidity, and the RMS is less than 0.4 g/m<sup>3</sup> as shown in <xref ref-type="fig" rid="fig8">Figure 8</xref>.</p><p>For precipitation the primary radiometric signal at frequencies around 183 GHz from precipitating scenes results from the scattering by ice hydrometeors. This scattering can result in significant brightness temperature</p><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> Schematic of retrieving flow</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x32.png"/></fig><fig-group id="fig8"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> Profile retrievals of temperature and humidity (T&amp;H) using simulated brightness temperatures from microwave radiometer onboard gestational platform.</title></caption><fig id ="fig8_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x34.png"/></fig><fig id ="fig8_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x33.png"/></fig><fig id ="fig8_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x36.png"/></fig><fig id ="fig8_4"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x35.png"/></fig><fig id ="fig8_5"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x38.png"/></fig><fig id ="fig8_6"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x37.png"/></fig></fig-group><fig-group id="fig9"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> Rain detection according to the brightness temperature analysis.</title></caption><fig id ="fig9_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x41.png"/></fig><fig id ="fig9_2"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x40.png"/></fig><fig id ="fig9_3"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/5-4700494x39.png"/></fig></fig-group><p>depressions (several 10’s K) relative to non-precipitating surroundings, and is therefore a sensitive proxy for the presence of precipitation at the surface.</p><p>According to the global difference distributions of brightness temperatures on Jan 20, 2015, a) channel 10 plus channel 15, b) for channel 10 plus channel 9, and c) for channel 9 plus channel 15 for FY-3C MWHTS, using neural network method, the precipitation and rain detection can be derived, which is shown in <xref ref-type="fig" rid="fig9">Figure 9</xref> and <xref ref-type="table" rid="table3">Table 3</xref>.</p></sec><sec id="s6"><title>6. Summary and Conclusions</title><p>According to the retrievals and analysis, geostationary sub-millimeter atmospheric sounder will play an important role in studying global climate and is the main remote sensing instrument for meteorology and disaster. It works in all weather and all day providing the observation of brightness temperature which can be used to retrieve temperature and humidity profiles and precipitation rate.</p><p>There is a well agreement in temperature and humidity profiles between radiosonde and retrievals. Compared to radiosonde, the retrievals show that the RMS of atmospheric temperature profile is less than 1 K, RMS of atmospheric relative humidity profile is less than 20%, which can be converted to atmospheric absolute humidity,</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Rain detection of typhoon domain by geostationary sub-millimeter atmospheric sounder between Jan. 1 to Oct. 31, 2014</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Location</th><th align="center" valign="middle" >Rain rate (mm/h)</th><th align="center" valign="middle" >Land rms/K</th><th align="center" valign="middle" >Sea rms/K</th></tr></thead><tr><td align="center" valign="middle"  rowspan="6"  >Typhoon domain</td><td align="center" valign="middle" >0.1 - 1</td><td align="center" valign="middle" >0.89</td><td align="center" valign="middle" >0.84</td></tr><tr><td align="center" valign="middle" >1 - 5</td><td align="center" valign="middle" >4.03</td><td align="center" valign="middle" >3.54</td></tr><tr><td align="center" valign="middle" >5 - 10</td><td align="center" valign="middle" >7.45</td><td align="center" valign="middle" >6.78</td></tr><tr><td align="center" valign="middle" >10 - 30</td><td align="center" valign="middle" >20.21</td><td align="center" valign="middle" >17.21</td></tr><tr><td align="center" valign="middle" >30 - 50</td><td align="center" valign="middle" >23.28</td><td align="center" valign="middle" >21.23</td></tr><tr><td align="center" valign="middle" >50 - 65</td><td align="center" valign="middle" >36.13</td><td align="center" valign="middle" >32.4</td></tr></tbody></table></table-wrap><p>and the RMS is less than 0.4 g/m<sup>3</sup>.</p><p>For the recent work, the surface is classified the surface mark as land, sea and coastal, using the observing data to detect weather it is rain or not and then test and validate the accuracy of the rain rate. Therefore, the work provides algorithms and data analysis of temperature and humidity profiles and precipitation distribution. So, the work will play an important role in the design and development of following meteorological satellites.</p><p>Because it is not enough, the authors are doing further improvement, like considering the surface covered by snow, ice and rainforest. Also, the rain rate is excepted to be retrieved more accurately. The radar data are also needed to validate the accuracy of rain detection. All of above will be described in future paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Jieying He,Shengwei Zhang,Hao Liu,Ying Zhang, (2016) Profile and Precipitation Retrievals and Validation Based on Geostationary Sub-Millimeter Atmospheric Sounder. 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