NASA Cold Land Processes Experiment (CLPX 2002/03): Local Scale Observation Site

Size: px
Start display at page:

Download "NASA Cold Land Processes Experiment (CLPX 2002/03): Local Scale Observation Site"

Transcription

1 1434 J O U R N A L O F H Y D R O M E T E O R O L O G Y VOLUME 9 NASA Cold Land Pocesses Expeiment (CLPX 2002/03): Local Scale Obsevation Site JANET HARDY,* ROBERT DAVIS,* YEOHOON KOH,* DON CLINE, KELLY ELDER, # RICHARD HANS-PETER THOMAS PAINTER, & GILLES CASTRES SAINT-MARTIN,** ROGER DEROO,** KAMAL SARABANDI,** TOBIAS GRAF, TOSHIO KOIKE, AND KYLE MCDONALD ## * Cold Regions Reseach and Engineeing Laboatoy, Enginee Reseach and Development Cente, U.S. Amy Cops of Enginees, Hanove, New Hampshie NOAA/NWS/National Opeational Hydologic Remote Sensing Cente, Chanhassen, Minnesota # USDA Foest Sevice, Fot Collins, Univesity of Coloado, Boulde, Coloado & Univesity of Utah, Salt Lake City, Utah ** Univesity of Michigan, Ann Abo, Michigan Univesity of Tokyo, Tokyo, Japan ## NASA Jet Populsion Laboatoy, Califonia Institute of Technology, Pasadena, Califonia (Manuscipt eceived 12 Januay 2007, in final fom 19 Mach 2008) ABSTRACT The local scale obsevation site (LSOS) is the smallest study site (0.8 ha) of the 2002/03 Cold Land Pocesses Expeiment (CLPX) and is located within the Fase mesocell study aea. It was the most intensively measued site of the CLPX, and measuements hee had the geatest tempoal component of all CLPX sites. Measuements made at the LSOS wee designed to poduce a compehensive assessment of the snow, soil, and vegetation chaacteistics viewed by the gound-based emote sensing instuments. The objective of the gound-based micowave emote sensing was to collect time seies of active and passive micowave spectal signatues ove snow, soil, and foest, which is coincident with the intensive physical chaacteization of these featues. Gound-based emote sensing instuments included fequency modulated continuous wave (FMCW) adas opeating ove multiple micowave bandwidths; the Gound-Based Micowave Radiomete (GBMR-7) opeating at channels 18.7, 23.8, 36.5, and 89 GHz; and in 2003, an L-, C-, X- and Ku-band scatteomete ada system. Snow and soil measuements included standad snow physical popeties, snow wetness, snow depth tansects, and soil moistue. The stem and canopy tempeatue and xylem sap flux of seveal tees wee monitoed continuously. Five micometeoological towes monitoed ambient conditions and povided focing datasets fo 1D snow and soil models. Aays of pyanometes (0.3 3 m) and a scanning themal adiomete (8 12 m) chaacteized the vaiability of adiative eceipt in the foests. A field spectoadiomete measued the hypespectal hemispheical-diectional eflectance of the snow suface. These measuements, togethe with the gound-based emote sensing, povide the famewok fo evaluating and impoving micowave adiative tansfe models and coupling them to land suface models. The dataset is achived at the National Snow and Ice Data Cente (NSIDC) in Boulde, Coloado. 1. Intoduction The local scale obsevation site (LSOS) is the smallest study site of the Cold Land Pocesses Expeiment (CLPX; D. Cline et al. 2008, unpublished manuscipt) and Coesponding autho addess: Janet P. Hady, CRREL, Enginee Reseach and Development Cente, U.S. Amy Cops of Enginees, 72 Lyme Road, Hanove, NH janet.p.hady@usace.amy.mil is located within the Fase mesocell study aea (MSA), nea the Fase Expeimental Foest headquates facility in Fase, Coloado [ N, W; 2780 m asl (metes above sea level); Fig. 1]. The 0.8-ha tiangula site consists of a small cleaing, a managed unifom pine canopy, and a discontinuous, mixed age canopy (Fig. 2). The LSOS was the most intensively measued site in the CLPX, whee the measuement detail fa exceeded simila measuements at the lage scales. The data collected at the LSOS allows fo a DOI: /2008JHM Ameican Meteoological Society

2 DECEMBER 2008 H A R D Y E T A L A netwok of footpaths was established thoughout the LSOS to pevent the disuption of the specific measuement sites. 2. Summay of collected data paametes FIG. 1. The LSOS ( ) elative to the thee Fase ISAs and Fase, CO. complete and detailed chaacteization of the local snow conditions, soil popeties, vegetation, and enegy balance chaacteistics. Additionally, measued goundbased micowave emote sensing (active and passive) at the LSOS povided data to elate to the measued snow and canopy popeties as well as emote sensing signatues. The dataset is achived at the National Snow and Ice Data Cente (NSIDC) in Boulde, Coloado (available online at The pupose of the LSOS measuements was to allow scaling between gound-based and aibone- and satellite-based instuments. The detailed measuements allow full chaacteization of the test site and can be used to validate small-scale models and futhe extapolate and test algoithms at lage scales. The gound-based emote sensos viewed a homogeneous snow-coveed cleaing and a small foest stand. Snow scattes the micowave emissions fom the soil, and the amount of this scatte is elated to the snow popeties, including snow wate equivalent (SWE), gain size, wetness, depth, and density. Suface enegetics dive the enegy balance components that influence these snowpack physical popeties, which in tun affect the signal eceived by the gound-based sensos. The measuement appoach within the LSOS consisted of a high sampling density within elatively unifom aeas of the LSOS to facilitate a compaison of micowave emote sensing data, adiative tansfe models, detailed physical models of the snow and the undelying soil, and gound obsevations. a. Canopy chaacteization In the fall of 2001, Cold Regions Reseach and Engineeing Laboatoy (CRREL) scientists of the Enginee Reseach and Development Cente (ERDC) defined and extensively mapped the canopy in the LSOS. The aea was divided into seventy-eight 10 m 10 m plots (Fig. 2), and the canopy in each plot was chaacteized using hemispheic photogaphy. The individual tee locations in 62 plots wee mapped and linked to thei physical measuements (tee height, cown height, diamete at beast height, and cown diamete). The LSOS was gouped into thee main canopy types: unifom pine canopy, discontinuous pine canopy, and small cleaing. b. Snowpack physical popeties Snow pits at the LSOS consist of thee snow pits pe day duing all intensive obsevation peiods (IOPs): one in each of the two canopy types and one in the cleaing. The potocol fom all the physical measuements used in the intensive study aeas (ISAs) (Elde et al. 2009a) wee used fo all the LSOS measuements to ensue data compatibility and to facilitate modeling and compaisons acoss scales. In addition to the standad potocol, we measued snow wetness duing the sping IOPs at 10-cm depth intevals including the snow suface using the Denoth snow wetness mete. Additionally, scientists opeating the Gound-Based Micowave Radiomete (GBMR-7) measued the snow popeties outside the IOPs to suppot thei adiomete measuements. c. Snow suveys Systematic measuements of snow depth and snow wate equivalent (SWE) wee made duing each IOP in each of the thee canopy types. Snow depth was measued to the neaest centimete using a calibated snow pobe inseted into the snow each mete along the paths. In 2003 only, SWE and density measuements wee made appoximately evey 5 10 m along the paths using the Canadian ESC-30 sample. d. Subcanopy enegetics Standad meteoological data collected at the LSOS anged fom subcanopy tempeatue, elative humidity,

3 1436 J O U R N A L O F H Y D R O M E T E O R O L O G Y VOLUME 9 FIG. 2. Map showing the layout of the LSOS with appoximate locations of instumentation. The unifom pine canopy is southeast of the cleaing. The discontinuous pine canopy is nothwest of the cleaing. and wind speed measued in the unifom canopy in 2002 to five full weathe stations (unifom canopy, cleaing, two in discontinuous canopy, and one appoximately 500 m west of the LSOS) and an eddy covaiance (EC) system in 2003 (Maks et al. 2008). The measued meteoological data included sola and longwave downwad adiation, snow, soil and ai tempeatue, elative humidity, wind speed and diection, pecipitation, soil heat flux, and soil moistue. Aays of ten sola and two longwave adiometes sampled enegy beneath the unifom conifeous canopy and the discontinuous canopy. The U.S. Foest Sevice measued the above-canopy adiation as well as othe meteoological components at the LSOS (Elde et al. 2009b). Spatial vaiations in the longwave adiation emitted wee compaed between the tee tunks, snow, and gound foliage using a themal infaed imaging adiomete (8 12 m). The measuements of the hypespectal hemispheical diectional eflectance facto (HDRF) of the snow suface (wavelength ange m), using a field spectoadiomete, povided calibation data fo the optical aibone and spacebone imaging spectometes and the multispectal images used in the CLPX. These measuements will also be compaed with field micowave measuements fo synthesizing the models snow popeties, including gain size, albedo, and suface liquid wate content. e. Micowave adiomete systems The Univesity of Michigan Radiation Laboatoy managed a passive micowave adiomete system that opeated at 1.4, 6.7, 19, and 37 GHz. These systems measued adiometic bightness in vetical (V) and hoizontal (H) polaizations. The 19- and 37-GHz systems have beamwidths of 10 each, while the 1.4 and 6.7-GHz systems have beamwidths of 22 each. These systems wee mounted on the end of a 10-m telescoping boom and allowed fo incidence angle vaiation fom nadi (0 ) to zenith (180 ; Fischman 2001). The adiomete systems wee configued to opeate continuously duing IOP3 and IOP4, with an objective to chaacteize micowave emission fom the snow cove and adjacent tees. The 6.7-, 19-, and 37-GHz systems collected micowave bightness data of a snow field at 54 incidence angle. Altenate tagets wee measued seveal times pe day: 1) a scan in elevation fom 0 to 65 of upwelling bightness fom the snow field, 2) a scan in azimuth of upwelling bightness at 54 fom shot tees to the southwest of the adiometes, 3) a scan in azimuth of upwelling bightness at 54 fom the sides of

4 DECEMBER 2008 H A R D Y E T A L snowpack popeties. The adiomete was mounted on a flexible positioning system, which allowed fo vaiety in the obsevation diection and incident angle. Two obsevation aeas have been used fo the expeiment: 1) the snowpack notheast of the adiomete (Fig. 2) was undistubed duing the winte and egulaly scanned with vaying incident angles (between 30 and 70 ), and 2) the nothen aea was used fo obseving bae soil (afte emoving snow) and new snow on the gound. Both taget aeas wee scanned seveal times a day duing the IOPs. FIG. 3. Photo of the GBMR-7 in opeation at the LSOS. tees talle than the tuck boom to the noth and nothwest, and 4) a scan in elevation fom 90 to 135 of the downwelling bightness fom the same tall tees (De Roo et al. 2007). f. Gound-based micowave adiomete The Univesity of Tokyo opeated the GBMR-7 Advanced Micowave Scanning Radiomete (AMSR) simulato (Fig. 3), which obseved the bightness tempeatue at 18.7, 23.8, 36.5, and 89 GHz (Kazama et al. 1999). The objectives of this passive micowave adiomete wee to 1) obseve the influence of snowpack metamophism and the melting efeezing cycle on the bightness tempeatue of the snow cove, and 2) develop a scheme, which couples a adiative tansfe model with a physical-based snow model using data assimilation. To develop and validate the assimilation scheme, a vey detailed dataset was collected, which compised focing data, adiomete obsevations, and g. L- and K u -band scatteomete The Univesity of Michigan opeated a scatteomete, a ada system capable of measuing the amplitude and phase of the backscatteed signal, in the lage cleaing in the LSOS. The system opeated at L-band ( GHz) and Ku-band ( GHz; Tassoudji et al. 1989). The measuements wee taken fom thee diffeent incidence angles (20, 35, and 50 fom nadi). A total of 401 fequency points wee ecoded ove the bandwidth fo both scatteometes, and data collection was pefomed ove 60 independent spatial samples at 20, and 30 independent spatial samples at 35 and 50. The measued data wee calibated using a metallic 36-cm diamete sphee and the single taget calibation technique (STCT; Saabandi and Ulaby 1990) algoithm. The polaimetic scatteing data afte calibation was fomatted in Muelle matix fom and stoed. h. Fequency modulated continuous wave adas The CRREL/ERDC and the Univesity of Coloado obtained ada gound measuements using FMCW adas in thee fequency bands [2 6 GHz (C-band), 8 12 GHz (X-band), and GHz (Ku-band)] as well as naow-band measuements (bandwidth 1 GHz and 100 MHz) centeed in each fequency ange (Stove 1992). Metal eflectos placed on the suface and in the TABLE 1. Tempoal esolution of measued data. Refe to specific datasets fo moe details. PeIOPs IOP Inteim IOPs IOP IOP Inteim IOPs IOP Canopy chaacteization Snow popeties and snow suveys Subcanopy enegetics Micowave adiomete GBMR-7 adiomete * Scatteomete FMCW ada Biophysical popeties Ongoing, beginning with IOP1 * Data only fo 25 Ma 2003.

5 1438 J O U R N A L O F H Y D R O M E T E O R O L O G Y VOLUME 9 TABLE 2. Measued micowave fequencies (GHz) of vaious instuments. Hee, indicates bandwidths Micowave adiomete GBMR-7 adiomete Scatteomete FMCW ada bands snowpack allowed fo calibation and attenuation calculations. These ada measuements simulated satellite and aibone measuements. This multifequency appoach fo ada emote sensing was designed to suppot the investigation of snowpack paametes such as density, depth, and wetness. As the ada fequency inceases, the effect of snow gain size becomes moe impotant. Radas opeating in the Ku-band contain the most infomation about the intenal featues of a dy snowpack; howeve, in a wet snowpack, the suface eflection dominates and gound etun is insignificant. Radas opeating at lowe fequencies (C-band) ae pefeable fo achieving the necessay penetation though a wet snowpack. i. Biophysical activity in tees The NASA Jet Populsion Laboatoy (JPL) monitoed biophysical activity in six selected tees with instuments that included themistos implanted in the soil and in the hydoactive tissues of the tee tunks, xylem sap flow sensos, and dielectic pobes. Xylem flux was monitoed using a constant enegy input method (Ganie 1987). The micowave dielectic constant of the hydoactive stem tissue was monitoed with an automated dielectic monitoing system (McDonald et al. 1999). Data acquied by these instuments chaacteized the themal egime within the tees and soil, and the wate consumed by the plant. Two goals of this eseach wee to detemine the wate conductive state of the tees duing spingtime thaw and to elate this infomation to measuements acquied with micowave emote sensing instuments. The genealized tempoal esolution of all collected data is summaized in Table 1. The peiop was conducted fom 2 to 6 Novembe 2001, IOP1 fom 17 to 24 Febuay 2002, IOP2 fom 24 to 30 Mach 2002, IOP3 fom 17 to 25 Febuay 2003, and IOP4 fom 25 Mach though 1 Apil Table 2 summaizes the measued micowave fequencies of all adas and adiometes opeating at the LSOS. 3. Example esults The data volume fom the LSOS is too lage fo full pesentation. To explain the esults fom the LSOS, we FIG. 4. Patial meteoological data fom the discontinuous pine site on 25 Ma Sola and longwave iadiance data ae fom two pyanometes (PSP 3-tee well and PSP 10-canopy gap) and one pygeomete (PIR 1-tee well). pesent a sample of data collected fom most sensos on one day of IOP4: 25 Mach Data included snow and meteoological obsevations, gound-based micowave adiomete data, gound-based ada data, and biophysical measuements. a. Snow and meteoological data On 25 Mach 2003, the sky was clea, midday ai tempeatues climbed above feezing, and the measued daily total incoming sola iadiance beneath the discontinuous pine site vaied between a minimum of 6.5 MJ m 2 (nea a tee tunk) to a maximum of 20.6 MJ m 2 (canopy gap; Fig. 4). Hemispheical diectional eflectance facto specta data of the snow suface in FIG. 5. HDRF specta measued with a field spectoadiomete on 25 Ma 2003 at 1230 local time (LT). The sola zenith and azimuth angles wee 38 and 188, espectively. Each of the thee lines epesents a diffeent measue of the specta.

6 DECEMBER 2008 H A R D Y E T A L TABLE 3. Snowpack popeties in the cleaing on 25 Ma 2003 at 1300 LT. UTM is Univesal Tansvese Mecato. Pit: LSOS_2a Date: UTM-E UTM-N Total Depth 107 Time: 1300 Location (UTM) Hit above gound Top Bottom Mean density kg m 3 Snow wetness % Height above gound Snow tempeatue C Hit above gound Top Bottom Gain size (mm) Sm Med Lg Snow suface n/a n/a 7 0 Snowpack mean: * ounded gains. Gain type* Comments Wet snow Had cust Satuated laye Depth hoa Depth hoa the cleaing ae pesented in Fig. 5. Snow pit data collected fom the cleaing at midday showed an isothemal snowpack of 1.07-m depth with ounded gains and a mean snowpack density of 284 kg m 3 (Table 3). Of paticula inteest fo intepetation of the adiomete and ada data was the measued statigaphy and snow wetness data showing a wet snow laye at the suface and a midpack satuated laye height of m. Snow depths in the discontinuous pine site wee moe vaiable than in the unifom pine site with a mean LSOS depth of 0.91 m (n 275; Fig. 6). snow wetness elationships on 25 Mach 2003 (Figs. 7 and 8). In Fig. 7, the Univesity of Michigan measued inceases in the 19-GHz bightness tempeatues at midday and again aound 0200 LT on 26 Mach 2003, coinciding with ising ai tempeatues. Similaly, the GBMR-7, opeated by the Univesity of Tokyo, showed an incease in bightness tempeatue fom moning though midaftenoon on 25 Mach, coesponding with an incease in snow wetness (Fig. 8a). Because of the unique micowave spectal signatue of snow, the diffeence in bightness tempeatue between b. Micowave adiomete systems Micowave adiomete data fom two sepaate sensos show bightness tempeatue, ai tempeatue, and FIG. 6. Snow depth tansect though both foest types. Each measued data point is 1 m apat. FIG. 7. Relationship between ai tempeatue and snow suface bightness tempeatue as measued at 19 GHz by Univesity of Michigan s micowave adiomete on 25 Ma 2003.

7 1440 J O U R N A L O F H Y D R O M E T E O R O L O G Y VOLUME 9 FIG. 8. (a) Influence of wet snow on the bightness tempeatue as measued by the GBMR-7 with hoizontal and vetical polaization. (b) Estimated SWE based on the bightness tempeatue diffeence. Because of the wet snow suface, note that (b) incoectly indicates the snowpack melted out completely afte 1200 LT on 25 Ma the lowe (e.g., 18.7 GHz) and the highe (e.g., 36.5 GHz) fequencies povides an indication of the SWE (Schmugge et al. 2002). Howeve, this elationship is only valid fo a completely dy snowpack and will fail at the pesence of liquid wate. Fo example, in Fig. 8b, the SWE is calculated using an algoithm based on the wok of Chang et al. (1987), SWE 4.77 TB 18.7H TB 36.5H, whee SWE epesents the snow wate equivalent (in millimetes), and TB 18.7H and TB 36.5H ae epesenting the bightness tempeatue obsevations at 18.7 GHz and 36.5 GHz (hoizontal polaization). Figue 8b also povides a good example of the effect of a wet snowpack. The low SWE in the moning was caused by the wet midlaye snowpack (see Table 3). Duing late obsevations, the bightness tempeatue diffeences deceases because of an inceasing snow suface wetness. Coespondingly, the estimated SWE deceases, and the obsevation afte 1200 LT incoectly suggests the absence of snow on the gound. c. Scatteomete and FMCW ada Figue 9 shows a epesentative set of polaimetic backscatteing coefficients collected on 26 Mach 2003 by the Univesity of Michigan s ada at Ku-band ( GHz). The data show simila copolaized backscatteing coefficients, which indicates that the snow volume entiely dominated the scatteing. This esult is also evident fom the copolaized atio to the coss-polaized atio ( 9 db), which is mainly caused by the multiple scatteing within the snow medium. CRREL/ERDC and the Univesity of Coloado s multiband ada pofile fo the wet snow of 25 Mach (Figs. 10a and 10b) showed the pesence of a small amount of wate affected ada inteaction with the snowpack. C-band (2 8 GHz) measuements (Fig. 10a) esolved the lowe layes in the snowpack; howeve, at the Ku-band (14 18 GHz) fequencies (Fig. 10b), the suface eflection was the dominant effect in the wet snow, and gound etun was insignificant. Fo this wet snowpack, adas opeating at lowe fequencies wee pefeable to achieve necessay penetation. These esults suggest that a dual-fequency appoach fo ada emote sensing is necessay to etieve snowpack paametes such as density, depth, and wetness. d. Biophysical activity in tees An example of the NASA JPL dataset fom one of the six tees continuously monitoed fo two yeas shows snow, soil, and stem tempeatues below feezing on 25 Mach 2003 (Fig. 11). These data change damatically late in the sping as ai, soil, and stem tempeatues incease and sap flow begins. This change is used FIG. 9. Time seies of backscatteing coefficients as a function of the incidence angle fo the Ku-band scatteomete on 26 Ma The backscatteing coefficient is the atio of the ada coss section of the taget to its aeal extent, expessed in decibels.

8 DECEMBER 2008 H A R D Y E T A L FIG. 10. (a) C-band and (b) Ku-band data fom the FMCW ada on 25 Ma Black indicates stong eflection, and white indicates no eflection. Note that the C-band measuement penetates to the gound in this wet snowpack and shows eflections fom midpack layes. The Ku-band measuement has a vey stong suface eflection as a esult of the moistue content and shows midpack eflections, but it is attenuated befoe eaching the snow gound inteface. to detemine the onset of the gowing season fo LSOS conife tees. These data will augment and suppot the intepetation of the measuements acquied with micowave emote sensing instuments. 4. Summay Data wee collected at the local scale obsevation site ove a peiod of two yeas and by seveal coopeating institutions and numeous people. The data pesented hee wee intended to show the contents of the lage database. This database povides details of fully chaacteized snow, soil, canopy, enegy balance, and micowave popeties. Using this database, physically based models, emote sensing etieval algoithms, and theoies can be confidently evaluated with minimal ambiguity. Scaling execises, in conjunction with the full CLPX dataset, will test the pefomance of these algoithms and models at the 1- and 25-km scales (ISA and MSA, espectively), and the egional scale. Acknowledgments. This wok was funded though coopeation of many agencies and oganizations including the National Aeonautics and Space Administation (NASA), the U.S. Amy Cops of Enginees Civil Woks Remote Sensing Reseach Pogam, the U.S. Amy Basic Reseach Pogam, the Japan Aeospace Exploation Agency (JAXA), the Japan Science and Technology Agency, and the National Assembly fo Wales, Stategic Reseach Investment Fund, Cadiff. A potion of this wok was conducted at the Jet Populsion Laboatoy at the Califonia Institute of Technology, unde contact to NASA. Many individuals contibuted to the success of the data collection effot at the LSOS. Ou gatitude is extended to H. Boyne, M. J. Bodzik, T. England, R. Essey, R. Foeste, H. Fujii, G. Koenig, T. Link, D. Maks, M. Matinez, R. Melloh, N. Mulhein, E. Podest, J. Pomeoy, A. Rowlands, A. Twombly, and othe staff at the U.S. Foest Sevice, Fase Expeimental Foest. REFERENCES FIG. 11. Stem tempeatue monitoed at 1.5-m height and at the stem base of one lodgepole pine tee on 25 Ma Snowpack tempeatue at 0.1 m above the gound suface, and soil tempeatue at the gound suface and at 0.1-m depth. Chang, A. T. C., J. L. Foste, and D. K. Hall, 1987: Nimbus-7 SMMR deived global snow cove paametes. Ann. Glaciol., 9, De Roo, R. D., A. R. Chang, and A. W. England, 2007: Radiobightness at 6.7-, 19-, and 37-GHz downwelling fom matue evegeen tees obseved duing the Cold Lands Pocesses Expeiment in Coloado. IEEE Tans. Geosci. Remote Sens., 45, Elde, K., D. Cline, A. Goodbody, P. House, G. Liston, L. Maht, and N. Rutte, 2009a: NASA Cold Land Pocesses Expeiment (CLPX 2002/03): Gound-based and nea-suface meteoological obsevations. J. Hydometeo., in pess.,, G. Liston, and R. Amstong, 2009b: NASA Cold

9 1442 J O U R N A L O F H Y D R O M E T E O R O L O G Y VOLUME 9 Land Pocesses Expeiment (CLPX 2002/03): Field measuements of snowpack popeties and soil moistue. J. Hydometeo., in pess. Fischman, M. A., 2001: Development of a diect-sampling digital coelation adiomete fo Eath emote sensing applications. Ph.D. dissetation, Univesity of Michigan, 232 pp. Ganie, A., 1987: Evaluation of tanspiation in a Douglas-fi stand by means of sap flow measuements. Tee Physiol., 3, Kazama, S., T. Rose, R. Zimmeman, and R. Zimmeman, 1999: A pecision autocalibating 7 channel adiomete fo envionmental eseach applications. J. Remote Sens. Soc. Japan, 19, Maks, D., M. Reba, J. Pomeoy, T. Link, A. Winstal, G. Flechinge, and K. Elde, 2008: Compaing simulated and measued sensible and latent heat fluxes ove snow unde a pine canopy to impove an enegy balance snowmelt model. J. Hydometeo., 9, McDonald, K. C., R. Zimmemann, J. B. Way, and W. Chun, 1999: Automated instumentation fo continuous monitoing of the dielectic popeties of woody vegetation: System design, implementation, and selected in situ measuements. IEEE Tans. Geosci. Remote Sens., 37, Saabandi, K., and F. T. Ulaby, 1990: A convenient technique fo polaimetic calibation of single-antenna ada systems. IEEE Tans. Geosci. Remote Sens., 28, Schmugge, T. S., W. P. Kustas, J. C. Ritchie, T. J. Jackson, and A. Rango, 2002: Remote sensing in hydology. Adv. Wate Resou., 25, Stove, A. G., 1992: Linea FMCW ada techniques. IEE Poc. Pat F: Rada Signal Pocess., 139, Tassoudji, M. A., K. Saabandi, and F. T. Ulaby, 1989: Design consideation and implementation of the LCX polaimetic scatteomete (POLARSCAT). Radiation Laboatoy Rep T-2, 79 pp.

Permittivity of Human Skin in the Millimetre Wave Band

Permittivity of Human Skin in the Millimetre Wave Band Pemittivity of Human Skin in the Millimete Wave Band C. M. Alabaste, Canfield Univesity. E-mail: c.m.alabaste@mcs.canfield.ac.uk Abstact: The complex pemittivity of a human skin sample is measued ove the

More information

RETRIEVAL OF VERTICAL RAIN RATE PROFILE BY DUAL-FREQUENCY RADAR DATA

RETRIEVAL OF VERTICAL RAIN RATE PROFILE BY DUAL-FREQUENCY RADAR DATA P5R.8 RETRIEVAL OF VERTICAL RAIN RATE PROFILE BY DUAL-FREQUENCY RADAR DATA Koyuu Iwanami 1 Yohei Chono 2 Toshio Haimaya 2 Jacques Testud 3 Masayuki Maki 1 Ryohei Misumi 1 Sang-Goon Pak 1 1: National Reseach

More information

1) Emits radiation at the maximum intensity possible for every wavelength. 2) Completely absorbs all incident radiation (hence the term black ).

1) Emits radiation at the maximum intensity possible for every wavelength. 2) Completely absorbs all incident radiation (hence the term black ). Radiation laws Blackbody adiation Planck s Law Any substance (solid, liquid o gas) emits adiation accoding to its absolute tempeatue, measued in units of Kelvin (K = o C + 73.5). The efficiency at which

More information

Black Body Radiation and Radiometric Parameters:

Black Body Radiation and Radiometric Parameters: Black Body Radiation and Radiometic Paametes: All mateials absob and emit adiation to some extent. A blackbody is an idealization of how mateials emit and absob adiation. It can be used as a efeence fo

More information

ANALYSIS OF SURF ZONE RADAR BACKSCATTER MEASUREMENTS

ANALYSIS OF SURF ZONE RADAR BACKSCATTER MEASUREMENTS ANALYSIS OF SURF ZONE RADAR BACKSCATTER MEASUREMENTS LONG-TERM GOAL David R. Lyzenga Naval Achitectue and Maine Engineeing Dept. Univesity of Michigan Ann Abo, MI 48109-2145 phone: (734) 764-3216 fax:

More information

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials

Coupled Electromagnetic and Heat Transfer Simulations for RF Applicator Design for Efficient Heating of Materials Coupled Electomagnetic and Heat Tansfe Simulations fo RF Applicato Design fo Efficient Heating of Mateials Jeni Anto 1 and Raj C Thiagaajan 2 * 1 Reseache, Anna Univesity, Chennai, 2 ATOA Scientific Technologies

More information

Retrieval of three-dimensional distribution of rainfall parameters for rain attenuation correction using multi-parameter radar

Retrieval of three-dimensional distribution of rainfall parameters for rain attenuation correction using multi-parameter radar Retieval of thee-dimensional distibution of ainfall paametes fo ain attenuation coection using multi-paamete ada Dong-Soon Kim 1, Dong-In Lee 1, Masayuki Maki 2 and Ji-Young Gu 1 1 Depatment of Envionmental

More information

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects

Pulse Neutron Neutron (PNN) tool logging for porosity Some theoretical aspects Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Intoduction Pehaps the most citicism of Pulse Neuton Neuon (PNN) logging methods has been chage that PNN is to sensitive to the

More information

Determining solar characteristics using planetary data

Determining solar characteristics using planetary data Detemining sola chaacteistics using planetay data Intoduction The Sun is a G-type main sequence sta at the cente of the Sola System aound which the planets, including ou Eath, obit. In this investigation

More information

OSCILLATIONS AND GRAVITATION

OSCILLATIONS AND GRAVITATION 1. SIMPLE HARMONIC MOTION Simple hamonic motion is any motion that is equivalent to a single component of unifom cicula motion. In this situation the velocity is always geatest in the middle of the motion,

More information

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer.

15 B1 1. Figure 1. At what speed would the car have to travel for resonant oscillations to occur? Comment on your answer. Kiangsu-Chekiang College (Shatin) F:EasteHolidaysAssignmentAns.doc Easte Holidays Assignment Answe Fom 6B Subject: Physics. (a) State the conditions fo a body to undego simple hamonic motion. ( mak) (a)

More information

The nature of electromagnetic radiation.

The nature of electromagnetic radiation. Lectue 3 The natue of electomagnetic adiation. Objectives: 1. Basic intoduction to the electomagnetic field: Definitions Dual natue of electomagnetic adiation lectomagnetic spectum. Main adiometic quantities:

More information

Levitation force analysis of ring and disk shaped permanent magnet-high temperature superconductor

Levitation force analysis of ring and disk shaped permanent magnet-high temperature superconductor Inn Jounal of Pue & Applied Physics Vol. 55, Apil 017, pp. 61-68 Levitation foce analysis of ing and disk shaped pemanent magnet-high tempeatue supeconducto Sinan Basaan & Selim Sivioglu* Depatment of

More information

A scaling-up methodology for co-rotating twin-screw extruders

A scaling-up methodology for co-rotating twin-screw extruders A scaling-up methodology fo co-otating twin-scew extudes A. Gaspa-Cunha, J. A. Covas Institute fo Polymes and Composites/I3N, Univesity of Minho, Guimaães 4800-058, Potugal Abstact. Scaling-up of co-otating

More information

The geometric construction of Ewald sphere and Bragg condition:

The geometric construction of Ewald sphere and Bragg condition: The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in

More information

Impedance-based Biosensors. Pittsburgh, PA 15213, U.S.A.

Impedance-based Biosensors. Pittsburgh, PA 15213, U.S.A. Impedance-based Biosensos X. Huang, 1 D.W. Geve, 1 I. Nausieda, 1 D. Nguyen, 2 and M.M. Domach 2 1 Depatment of Electical and Compute Engineeing, Canegie Mellon Univesity, Pittsbugh, PA 15213, U.S.A. 2

More information

Sensor and Simulation Notes. Note 525. Oct Lens Design for a Prolate-Spheroidal Impulse radiating Antenna (IRA)

Sensor and Simulation Notes. Note 525. Oct Lens Design for a Prolate-Spheroidal Impulse radiating Antenna (IRA) Senso and Simulation Notes Note 55 Oct 7 Lens Design fo a Polate-Spheoidal Impulse adiating Antenna (IRA) Sehat Altunc, Cal E. Baum, Chistos G. Chistodoulou and Edl Schamiloglu Univesity of New Mexico

More information

I. Introduction to ecological populations, life tables, and population growth models

I. Introduction to ecological populations, life tables, and population growth models 3-1 Population ecology Lab 3: Population life tables I. Intoduction to ecological populations, life tables, and population gowth models This week we begin a new unit on population ecology. A population

More information

The Millikan Experiment: Determining the Elementary Charge

The Millikan Experiment: Determining the Elementary Charge LAB EXERCISE 7.5.1 7.5 The Elementay Chage (p. 374) Can you think of a method that could be used to suggest that an elementay chage exists? Figue 1 Robet Millikan (1868 1953) m + q V b The Millikan Expeiment:

More information

Supporting Information. and NaCl at the Air/Aqueous Interface revealed by Heterodyne Detected. Phase-Sensitive Sum Frequency

Supporting Information. and NaCl at the Air/Aqueous Interface revealed by Heterodyne Detected. Phase-Sensitive Sum Frequency Suppoting Infomation lectic Field Revesal of Na SO 4, (NH 4 ) SO 4, and Na CO 3 elative to CaCl and NaCl at the Ai/Aqueous Inteface evealed by Heteodyne Detected Phase-Sensitive Sum Fequency Wei Hua, Aaon

More information

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES

EKT 345 MICROWAVE ENGINEERING CHAPTER 2: PLANAR TRANSMISSION LINES EKT 345 MICROWAVE ENGINEERING CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and close

More information

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere

Absorption Rate into a Small Sphere for a Diffusing Particle Confined in a Large Sphere Applied Mathematics, 06, 7, 709-70 Published Online Apil 06 in SciRes. http://www.scip.og/jounal/am http://dx.doi.og/0.46/am.06.77065 Absoption Rate into a Small Sphee fo a Diffusing Paticle Confined in

More information

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below.

11) A thin, uniform rod of mass M is supported by two vertical strings, as shown below. Fall 2007 Qualifie Pat II 12 minute questions 11) A thin, unifom od of mass M is suppoted by two vetical stings, as shown below. Find the tension in the emaining sting immediately afte one of the stings

More information

Chapter 13 Gravitation

Chapter 13 Gravitation Chapte 13 Gavitation In this chapte we will exploe the following topics: -Newton s law of gavitation, which descibes the attactive foce between two point masses and its application to extended objects

More information

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE

MODULE 5 ADVANCED MECHANICS GRAVITATIONAL FIELD: MOTION OF PLANETS AND SATELLITES VISUAL PHYSICS ONLINE VISUAL PHYSICS ONLIN MODUL 5 ADVANCD MCHANICS GRAVITATIONAL FILD: MOTION OF PLANTS AND SATLLITS SATLLITS: Obital motion of object of mass m about a massive object of mass M (m

More information

Mathematisch-Naturwissenschaftliche Fakultät I Humboldt-Universität zu Berlin Institut für Physik Physikalisches Grundpraktikum.

Mathematisch-Naturwissenschaftliche Fakultät I Humboldt-Universität zu Berlin Institut für Physik Physikalisches Grundpraktikum. Mathematisch-Natuwissenschaftliche Fakultät I Humboldt-Univesität zu Belin Institut fü Physik Physikalisches Gundpaktikum Vesuchspotokoll Polaisation duch Reflexion (O11) duchgefüht am 10.11.2009 mit Vesuchspatne

More information

Analysis and Optimization of a Special Type of Dielectric Loaded Resonant Cavity for Mobile Communication Filters

Analysis and Optimization of a Special Type of Dielectric Loaded Resonant Cavity for Mobile Communication Filters 328 Analysis and Optimization of a Special Type of Dielectic Loaded Resonant Cavity fo Mobile Communication Filtes Haold S. Showes, Banmali S. Rawat *, Syam S. Challa Depatment of Electical and Biomedical

More information

THE STUDY AND IMPROVEMENT OF X-BAND ATTENUATION ESTIMATION USING DUAL POLARIMETRIC RADAR TECHNIQUES

THE STUDY AND IMPROVEMENT OF X-BAND ATTENUATION ESTIMATION USING DUAL POLARIMETRIC RADAR TECHNIQUES THE STUDY AND IMPROVEMENT OF X-BAND ATTENUATION ESTIMATION USING DUAL POLARIMETRIC RADAR TECHNIQUES Yuxiang Liu Advisos: V.N. Bingi and V. Chandaseka Decembe 4, 006 T ct } ) ( ) ( 4 ln exp{ ), ( 1 0 1

More information

Liquid gas interface under hydrostatic pressure

Liquid gas interface under hydrostatic pressure Advances in Fluid Mechanics IX 5 Liquid gas inteface unde hydostatic pessue A. Gajewski Bialystok Univesity of Technology, Faculty of Civil Engineeing and Envionmental Engineeing, Depatment of Heat Engineeing,

More information

EKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES

EKT 356 MICROWAVE COMMUNICATIONS CHAPTER 2: PLANAR TRANSMISSION LINES EKT 356 MICROWAVE COMMUNICATIONS CHAPTER : PLANAR TRANSMISSION LINES 1 Tansmission Lines A device used to tansfe enegy fom one point to anothe point efficiently Efficiently minimum loss, eflection and

More information

Pulse Neutron Neutron (PNN) tool logging for porosity

Pulse Neutron Neutron (PNN) tool logging for porosity Pulse Neuton Neuton (PNN) tool logging fo poosity Some theoetical aspects Hotwell Handelsges.m.b.H Oedenbuge Stasse 6 7013 Klingenbach, AUSTRIA Tel.: +43 (0) 687-48058 Fax: +43 (0) 687 48059 office@hotwell.at

More information

Basic Bridge Circuits

Basic Bridge Circuits AN7 Datafoth Copoation Page of 6 DID YOU KNOW? Samuel Hunte Chistie (784-865) was bon in London the son of James Chistie, who founded Chistie's Fine At Auctionees. Samuel studied mathematics at Tinity

More information

LIDAR AEROSOL RETRIEVALS FROM ICESAT USING A MODEL-BASED CONSTRAINED RATIO APPROACH

LIDAR AEROSOL RETRIEVALS FROM ICESAT USING A MODEL-BASED CONSTRAINED RATIO APPROACH LIDAR AEROSOL RETRIEVALS FROM ICESAT USING A MODEL-BASED CONSTRAINED RATIO APPROACH John Reagan 1 *, Xiaozhen Wang 1, Steve Palm 2 and James Spinhine 3 1 Univesity of Aizona, ECE Dept., Bldg. 104, Tucson,

More information

Ultrafast effects in 3D Metamaterials

Ultrafast effects in 3D Metamaterials Ultafast effects in 3D Metamateials Nkoni Katte,2 and Philip G.Evans 3 Electical Engineeing Wilbefoce Univesity, 2 Sensos Laboatoy Wight State Univesity and 3 Oak idge National Laboatoy *Coesponding autho:

More information

Physics 211: Newton s Second Law

Physics 211: Newton s Second Law Physics 211: Newton s Second Law Reading Assignment: Chapte 5, Sections 5-9 Chapte 6, Section 2-3 Si Isaac Newton Bon: Januay 4, 1643 Died: Mach 31, 1727 Intoduction: Kinematics is the study of how objects

More information

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY

Centripetal Force OBJECTIVE INTRODUCTION APPARATUS THEORY Centipetal Foce OBJECTIVE To veify that a mass moving in cicula motion expeiences a foce diected towad the cente of its cicula path. To detemine how the mass, velocity, and adius affect a paticle's centipetal

More information

Uniform Circular Motion

Uniform Circular Motion Unifom Cicula Motion Intoduction Ealie we defined acceleation as being the change in velocity with time: a = v t Until now we have only talked about changes in the magnitude of the acceleation: the speeding

More information

Fresnel Diffraction. monchromatic light source

Fresnel Diffraction. monchromatic light source Fesnel Diffaction Equipment Helium-Neon lase (632.8 nm) on 2 axis tanslation stage, Concave lens (focal length 3.80 cm) mounted on slide holde, iis mounted on slide holde, m optical bench, micoscope slide

More information

Experience from PV system performence including comparison of on-roof and façade systems. (Case study on BIPV systems.)

Experience from PV system performence including comparison of on-roof and façade systems. (Case study on BIPV systems.) Expeience fom PV system pefomence including compaison of on-oof and façade systems. (Case study on BIPV systems.) Vitezslav Benda CTU Pague, Faculty of Electical Engineeing Intelligent enegy management

More information

Field emission of Electrons from Negatively Charged Cylindrical Particles with Nonlinear Screening in a Dusty Plasma

Field emission of Electrons from Negatively Charged Cylindrical Particles with Nonlinear Screening in a Dusty Plasma Reseach & Reviews: Jounal of Pue and Applied Physics Field emission of Electons fom Negatively Chaged Cylindical Paticles with Nonlinea Sceening in a Dusty Plasma Gyan Pakash* Amity School of Engineeing

More information

Applications of radars: Sensing of clouds and precipitation.

Applications of radars: Sensing of clouds and precipitation. Lectue 1 Applications of adas: Sensing of clouds and pecipitation. Ojectives: 1. aticle ackscatteing and ada equation.. Sensing of pecipitation and clouds with adas (weathe adas, space adas: TMM and CloudSat).

More information

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology Electomagnetic scatteing Gaduate Couse Electical Engineeing (Communications) 1 st Semeste, 1390-1391 Shaif Univesity of Technology Geneal infomation Infomation about the instucto: Instucto: Behzad Rejaei

More information

Empirical Prediction of Fitting Densities in Industrial Workrooms for Ray Tracing. 1 Introduction. 2 Ray Tracing using DRAYCUB

Empirical Prediction of Fitting Densities in Industrial Workrooms for Ray Tracing. 1 Introduction. 2 Ray Tracing using DRAYCUB Empiical Pediction of Fitting Densities in Industial Wokooms fo Ray Tacing Katina Scheebnyj, Muay Hodgson Univesity of Bitish Columbia, SOEH-MECH, Acoustics and Noise Reseach Goup, 226 East Mall, Vancouve,

More information

Between any two masses, there exists a mutual attractive force.

Between any two masses, there exists a mutual attractive force. YEAR 12 PHYSICS: GRAVITATION PAST EXAM QUESTIONS Name: QUESTION 1 (1995 EXAM) (a) State Newton s Univesal Law of Gavitation in wods Between any two masses, thee exists a mutual attactive foce. This foce

More information

B. Spherical Wave Propagation

B. Spherical Wave Propagation 11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We

More information

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING

STUDY ON 2-D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Study Rev. Adv. on -D Mate. shock Sci. wave 33 (13) pessue 111-118 model in mico scale lase shock peening 111 STUDY ON -D SHOCK WAVE PRESSURE MODEL IN MICRO SCALE LASER SHOCK PEENING Y.J. Fan 1, J.Z. Zhou,

More information

Rotor Blade Performance Analysis with Blade Element Momentum Theory

Rotor Blade Performance Analysis with Blade Element Momentum Theory Available online at www.sciencediect.com ScienceDiect Enegy Pocedia 5 (7 ) 3 9 The 8 th Intenational Confeence on Applied Enegy ICAE6 Roto Blade Pefomance Analysis with Blade Element Momentum Theoy Faisal

More information

Sylwester Arabas 1, Hanna Pawlowska 1 and Wojciech W. Grabowski 2

Sylwester Arabas 1, Hanna Pawlowska 1 and Wojciech W. Grabowski 2 EFFECTIVE RADIUS AND DROPLET SPECTRAL WIDTH FROM RICO OBSERVATIONS Sylweste Aabas 1, Hanna Pawlowska 1 and Wojciech W. Gabowski 2 1 Institute of Geophysics, Univesity of Wasaw, Wasaw, Poland 2 National

More information

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra

Analytical Solutions for Confined Aquifers with non constant Pumping using Computer Algebra Poceedings of the 006 IASME/SEAS Int. Conf. on ate Resouces, Hydaulics & Hydology, Chalkida, Geece, May -3, 006 (pp7-) Analytical Solutions fo Confined Aquifes with non constant Pumping using Compute Algeba

More information

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations

MATH 415, WEEK 3: Parameter-Dependence and Bifurcations MATH 415, WEEK 3: Paamete-Dependence and Bifucations 1 A Note on Paamete Dependence We should pause to make a bief note about the ole played in the study of dynamical systems by the system s paametes.

More information

Analysis of high speed machining center spindle dynamic unit structure performance Yuan guowei

Analysis of high speed machining center spindle dynamic unit structure performance Yuan guowei Intenational Confeence on Intelligent Systems Reseach and Mechatonics Engineeing (ISRME 0) Analysis of high speed machining cente spindle dynamic unit stuctue pefomance Yuan guowei Liaoning jidian polytechnic,dan

More information

Improvement in Accuracy for Design of Multidielectric Layers Microstrip Patch Antenna

Improvement in Accuracy for Design of Multidielectric Layers Microstrip Patch Antenna 498 Impovement in Accuacy fo Design of Multidielectic Layes Micostip Patch Antenna Sami Dev Gupta*, Anvesh Gag and Anuag P. Saan Jaypee Institute of Infomation Technology Univesity Noida, Utta Padesh,

More information

Mathematical Model of Magnetometric Resistivity. Sounding for a Conductive Host. with a Bulge Overburden

Mathematical Model of Magnetometric Resistivity. Sounding for a Conductive Host. with a Bulge Overburden Applied Mathematical Sciences, Vol. 7, 13, no. 7, 335-348 Mathematical Model of Magnetometic Resistivity Sounding fo a Conductive Host with a Bulge Ovebuden Teeasak Chaladgan Depatment of Mathematics Faculty

More information

Phys 774: Ellipsometry

Phys 774: Ellipsometry Dielectic function Phys 774: Ellipsomety Optical vibations (phonons) Fee electons (plasma) Electonic tansitions (valence conduction band) Dielectic function and efactive index ae geneally complex: ε ε

More information

Lab #4: Newton s Second Law

Lab #4: Newton s Second Law Lab #4: Newton s Second Law Si Isaac Newton Reading Assignment: bon: Januay 4, 1643 Chapte 5 died: Mach 31, 1727 Chapte 9, Section 9-7 Intoduction: Potait of Isaac Newton by Si Godfey Knelle http://www.newton.cam.ac.uk/at/potait.html

More information

7.2. Coulomb s Law. The Electric Force

7.2. Coulomb s Law. The Electric Force Coulomb s aw Recall that chaged objects attact some objects and epel othes at a distance, without making any contact with those objects Electic foce,, o the foce acting between two chaged objects, is somewhat

More information

F g. = G mm. m 1. = 7.0 kg m 2. = 5.5 kg r = 0.60 m G = N m 2 kg 2 = = N

F g. = G mm. m 1. = 7.0 kg m 2. = 5.5 kg r = 0.60 m G = N m 2 kg 2 = = N Chapte answes Heinemann Physics 4e Section. Woked example: Ty youself.. GRAVITATIONAL ATTRACTION BETWEEN SMALL OBJECTS Two bowling balls ae sitting next to each othe on a shelf so that the centes of the

More information

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR

Research Article EXPERIMENTAL STUDY OF HEAT TRANSFER CHARACTERISTICS OF STAINLESS STEEL FIBROUS FLOW INSULATOR Tansactions of the TSME (16) Vol. 4, No. 2, 148 155 Jounal of seach and Applications in Mechanical Engineeing Copyight 16 by TSME ISSN 2229-2152 pint DOI: 1.14456/jame.16.15 seach Aticle EXPERIMENTAL STUDY

More information

Monitoring and modeling short-wave radiation in a broad-leaf forest

Monitoring and modeling short-wave radiation in a broad-leaf forest F S P M 4 Monitoing and modeling shot-wave adiation in a boad-leaf foest R. Giuliani, M.B. Thonton and K.J. Bown Depatment of Envionmental and Plant Biology, Ohio Univesity, Athens, OH 471 USA Intoduction

More information

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods

Hydroelastic Analysis of a 1900 TEU Container Ship Using Finite Element and Boundary Element Methods TEAM 2007, Sept. 10-13, 2007,Yokohama, Japan Hydoelastic Analysis of a 1900 TEU Containe Ship Using Finite Element and Bounday Element Methods Ahmet Egin 1)*, Levent Kaydıhan 2) and Bahadı Uğulu 3) 1)

More information

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1)

EM-2. 1 Coulomb s law, electric field, potential field, superposition q. Electric field of a point charge (1) EM- Coulomb s law, electic field, potential field, supeposition q ' Electic field of a point chage ( ') E( ) kq, whee k / 4 () ' Foce of q on a test chage e at position is ee( ) Electic potential O kq

More information

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other

17.1 Electric Potential Energy. Equipotential Lines. PE = energy associated with an arrangement of objects that exert forces on each other Electic Potential Enegy, PE Units: Joules Electic Potential, Units: olts 17.1 Electic Potential Enegy Electic foce is a consevative foce and so we can assign an electic potential enegy (PE) to the system

More information

Experiment I Voltage Variation and Control

Experiment I Voltage Variation and Control ELE303 Electicity Netwoks Expeiment I oltage aiation and ontol Objective To demonstate that the voltage diffeence between the sending end of a tansmission line and the load o eceiving end depends mainly

More information

Teachers notes. Beyond the Thrills excursions. Worksheets in this book. Completing the worksheets

Teachers notes. Beyond the Thrills excursions. Worksheets in this book. Completing the worksheets Beyond the Thills excusions Teaches notes Physics is the science of how the wold (and Univese) woks. Luna Pak Sydney is a lage hands-on physics laboatoy full of fee falling objects, otating systems and

More information

Substances that are liquids or solids under ordinary conditions may also exist as gases. These are often referred to as vapors.

Substances that are liquids or solids under ordinary conditions may also exist as gases. These are often referred to as vapors. Chapte 0. Gases Chaacteistics of Gases All substances have thee phases: solid, liquid, and gas. Substances that ae liquids o solids unde odinay conditions may also exist as gases. These ae often efeed

More information

Modeling Fermi Level Effects in Atomistic Simulations

Modeling Fermi Level Effects in Atomistic Simulations Mat. Res. Soc. Symp. Poc. Vol. 717 Mateials Reseach Society Modeling Femi Level Effects in Atomistic Simulations Zudian Qin and Scott T. Dunham Depatment of Electical Engineeing, Univesity of Washington,

More information

Measurement of Electrical Properties of Rapeseed Seeds with LCR Meter Good Will 8211

Measurement of Electrical Properties of Rapeseed Seeds with LCR Meter Good Will 8211 Intenational Jounal o Applied Science and Technology Vol 2 No 8; Octobe 212 Measuement o Electical Popeties o Rapeseed Seeds with LCR Mete Good Will 8211 Kassimia Kadjilova Depatment o Physics Technical

More information

NATURAL CONVECTION HEAT TRANSFER WITHIN VERTICALLY ECCENTRIC DOMED SKYLIGHTS CAVITIES

NATURAL CONVECTION HEAT TRANSFER WITHIN VERTICALLY ECCENTRIC DOMED SKYLIGHTS CAVITIES Poceedings: Building Simulation 007 NATURAL CONVECTION HEAT TRANSFER WITHIN VERTICALLY ECCENTRIC DOMED SKYLIGHTS CAVITIES A. Satipi, A. Laouadi, D. Naylo 3, R. Dhib 4 Depatment of Mechanical and Industial

More information

Motion in One Dimension

Motion in One Dimension Motion in One Dimension Intoduction: In this lab, you will investigate the motion of a olling cat as it tavels in a staight line. Although this setup may seem ovesimplified, you will soon see that a detailed

More information

INFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS. Abstract

INFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS. Abstract INFLUENCE OF GROUND INHOMOGENEITY ON WIND INDUCED GROUND VIBRATIONS Mohammad Mohammadi, National Cente fo Physical Acoustics, Univesity of Mississippi, MS Caig J. Hicey, National Cente fo Physical Acoustics,

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 303: Electomagnetic Fields and Waves Fall 007 Homewok 8 Due on Oct. 19, 007 by 5:00 PM Reading Assignments: i) Review the lectue notes.

More information

Identification of the degradation of railway ballast under a concrete sleeper

Identification of the degradation of railway ballast under a concrete sleeper Identification of the degadation of ailway ballast unde a concete sleepe Qin Hu 1) and Heung Fai Lam ) 1), ) Depatment of Civil and Achitectual Engineeing, City Univesity of Hong Kong, Hong Kong SAR, China.

More information

Improved Dielectric Model for Polyvinyl Alcohol-Water Hydrogel at Microwave Frequencies

Improved Dielectric Model for Polyvinyl Alcohol-Water Hydrogel at Microwave Frequencies Ameican Jounal of Applied Sciences 7 (2): 270-276, 2010 ISSN 1546-9239 2010 Science Publications Impoved Dielectic Model fo Polyvinyl Alcohol-Wate Hydogel at Micowave Fequencies 1 You Kok Yeow, 2 Zulkifly

More information

#7A&B Magnetic force between two conductors

#7A&B Magnetic force between two conductors #7A& Magnetic foce between two conductos This expeiment will be done duing two lab sessions. n the fist we become familia with the appaatus and make one set of measuements. n the second session, we complete

More information

THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN

THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN THE INFLUENCE OF THE MAGNETIC NON-LINEARITY ON THE MAGNETOSTATIC SHIELDS DESIGN LIVIU NEAMŢ 1, ALINA NEAMŢ, MIRCEA HORGOŞ 1 Key wods: Magnetostatic shields, Magnetic non-lineaity, Finite element method.

More information

V G. In this class, we will look at a possible hypothesis for way the time dependence is t

V G. In this class, we will look at a possible hypothesis for way the time dependence is t ECE65R : Reliability Physics of anoelectonic Devices Lectue : CI Time Exponents Date : Dec. 4, 6 Classnote : Saakshi Gangwal Review : Lutfe A Siddiqui. Review We have spent seveal weeks discussing discussing

More information

Contact impedance of grounded and capacitive electrodes

Contact impedance of grounded and capacitive electrodes Abstact Contact impedance of gounded and capacitive electodes Andeas Hödt Institut fü Geophysik und extateestische Physik, TU Baunschweig The contact impedance of electodes detemines how much cuent can

More information

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS

ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS THE 9 TH INTERNATIONAL CONFERENCE ON COMPOSITE MATERIALS ELASTIC ANALYSIS OF CIRCULAR SANDWICH PLATES WITH FGM FACE-SHEETS R. Sbulati *, S. R. Atashipou Depatment of Civil, Chemical and Envionmental Engineeing,

More information

Alignment of the ZEUS Micro- Vertex Detector Using Cosmic Tracks

Alignment of the ZEUS Micro- Vertex Detector Using Cosmic Tracks Alignment of the ZEUS Mico- Vetex etecto Using Cosmic acks akanoi Kohno (Univesity of Oxfod), ZEUS MV Goup Intenational Wokshop on Advanced Computing and Analysis echniques in Physics Reseach (ACA5) ESY,

More information

IN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES

IN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES IN SITU SOUND ABSORPTION COEFFICIENT MEASUREMENT OF VARIOUS SURFACES PACS REFERENCES : 43.20.El, 43.20.Ye, 43.55.Ev, 43.58.Bh Michel Béengie 1 ; Massimo Gaai 2 1 Laboatoie Cental des Ponts et Chaussées

More information

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS

MAGNETIC FIELD AROUND TWO SEPARATED MAGNETIZING COILS The 8 th Intenational Confeence of the Slovenian Society fo Non-Destuctive Testing»pplication of Contempoay Non-Destuctive Testing in Engineeing«Septembe 1-3, 5, Potoož, Slovenia, pp. 17-1 MGNETIC FIELD

More information

T. Raja Rani. Military Technological College, Muscat, Oman. Abstract

T. Raja Rani. Military Technological College, Muscat, Oman. Abstract ISSN: 78-8 Vol. Issue, Octobe - Fee Convection ove a Vaying all Vetical Cylinde embedded in a Poous medium ith effect of Radiation, Vaiable Fluid Popeties and Statification. T. Raja Rani Militay Technological

More information

Light Time Delay and Apparent Position

Light Time Delay and Apparent Position Light Time Delay and ppaent Position nalytical Gaphics, Inc. www.agi.com info@agi.com 610.981.8000 800.220.4785 Contents Intoduction... 3 Computing Light Time Delay... 3 Tansmission fom to... 4 Reception

More information

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in

Supplementary Figure 1. Circular parallel lamellae grain size as a function of annealing time at 250 C. Error bars represent the 2σ uncertainty in Supplementay Figue 1. Cicula paallel lamellae gain size as a function of annealing time at 50 C. Eo bas epesent the σ uncetainty in the measued adii based on image pixilation and analysis uncetainty contibutions

More information

Interaction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r)

Interaction of Feedforward and Feedback Streams in Visual Cortex in a Firing-Rate Model of Columnar Computations. ( r) Supplementay mateial fo Inteaction of Feedfowad and Feedback Steams in Visual Cotex in a Fiing-Rate Model of Columna Computations Tobias Bosch and Heiko Neumann Institute fo Neual Infomation Pocessing

More information

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007

School of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007 School of Electical and Compute Engineeing, Conell Univesity ECE 33: Electomagnetic Fields and Waves Fall 7 Homewok 6 Due on Oct. 5, 7 by 5: PM Reading Assignments: i) Review the lectue notes. ii) Review

More information

Chapter 5 Force and Motion

Chapter 5 Force and Motion Chapte 5 Foce and Motion In Chaptes 2 and 4 we have studied kinematics, i.e., we descibed the motion of objects using paametes such as the position vecto, velocity, and acceleation without any insights

More information

Position Error Estimation of a Laser Illuminated Object

Position Error Estimation of a Laser Illuminated Object SCIENTIFIC PUBLICATIONS OF THE STATE UNIVERSITY OF NOVI PAZAR SER. A: APPL. MATH. INFORM. AND MECH. vol. 3, 1 (2011, 59-69 Position Eo Estimation of a Lase Illuminated Object Ž. P. Babaić Abstact: Position

More information

Surveillance Points in High Dimensional Spaces

Surveillance Points in High Dimensional Spaces Société de Calcul Mathématique SA Tools fo decision help since 995 Suveillance Points in High Dimensional Spaces by Benad Beauzamy Januay 06 Abstact Let us conside any compute softwae, elying upon a lage

More information

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small.

Water flows through the voids in a soil which are interconnected. This flow may be called seepage, since the velocities are very small. Wate movement Wate flows though the voids in a soil which ae inteconnected. This flow may be called seepage, since the velocities ae vey small. Wate flows fom a highe enegy to a lowe enegy and behaves

More information

Duality between Statical and Kinematical Engineering Systems

Duality between Statical and Kinematical Engineering Systems Pape 00, Civil-Comp Ltd., Stiling, Scotland Poceedings of the Sixth Intenational Confeence on Computational Stuctues Technology, B.H.V. Topping and Z. Bittna (Editos), Civil-Comp Pess, Stiling, Scotland.

More information

Gaia s Place in Space

Gaia s Place in Space Gaia s Place in Space The impotance of obital positions fo satellites Obits and Lagange Points Satellites can be launched into a numbe of diffeent obits depending on thei objectives and what they ae obseving.

More information

Computational Modeling of Wave Propagation in a Geophysical Domain

Computational Modeling of Wave Propagation in a Geophysical Domain Except fom the Poceedings of the COMSOL Confeence 008 Boston Computational Modeling of Wave Popagation in a Geophysical Domain Jason McKenna 1 Mihan McKenna 1 Segei Yushanov Jeffey Compton and Kyle Koppenhoefe

More information

Charge Profiling of the p-algan Electron Blocking Layer in AlGaInN Light Emitting Diode Structures

Charge Profiling of the p-algan Electron Blocking Layer in AlGaInN Light Emitting Diode Structures Mate. Res. Soc. Symp. Poc. Vol. 892 2006 Mateials Reseach Society 0892-FF19-03.1 Chage Pofiling of the p-algan Electon Blocking Laye in AlGaInN Light Emitting Diode Stuctues Y. Xia 1,2, Y. Li 1,2, W. Zhao

More information

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1

Phys102 Second Major-182 Zero Version Monday, March 25, 2019 Page: 1 Monday, Mach 5, 019 Page: 1 Q1. Figue 1 shows thee pais of identical conducting sphees that ae to be touched togethe and then sepaated. The initial chages on them befoe the touch ae indicated. Rank the

More information

APPLICATION OF MAC IN THE FREQUENCY DOMAIN

APPLICATION OF MAC IN THE FREQUENCY DOMAIN PPLICION OF MC IN HE FREQUENCY DOMIN D. Fotsch and D. J. Ewins Dynamics Section, Mechanical Engineeing Depatment Impeial College of Science, echnology and Medicine London SW7 2B, United Kingdom BSRC he

More information

Electrostatics (Electric Charges and Field) #2 2010

Electrostatics (Electric Charges and Field) #2 2010 Electic Field: The concept of electic field explains the action at a distance foce between two chaged paticles. Evey chage poduces a field aound it so that any othe chaged paticle expeiences a foce when

More information

Lecture 2 Date:

Lecture 2 Date: Lectue 2 Date: 5.1.217 Definition of Some TL Paametes Examples of Tansmission Lines Tansmission Lines (contd.) Fo a lossless tansmission line the second ode diffeential equation fo phasos ae: LC 2 d I

More information

General Railgun Function

General Railgun Function Geneal ailgun Function An electomagnetic ail gun uses a lage Loentz foce to fie a pojectile. The classic configuation uses two conducting ails with amatue that fits between and closes the cicuit between

More information

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM

A NEW VARIABLE STIFFNESS SPRING USING A PRESTRESSED MECHANISM Poceedings of the ASME 2010 Intenational Design Engineeing Technical Confeences & Computes and Infomation in Engineeing Confeence IDETC/CIE 2010 August 15-18, 2010, Monteal, Quebec, Canada DETC2010-28496

More information