A new 2-D Model to analyze uncertainty sources of sparse sea surface

Size: px
Start display at page:

Download "A new 2-D Model to analyze uncertainty sources of sparse sea surface"

Transcription

1 A new -D Moel to analyze uncetainty souces of spase sea suface O patial pessue Xiang Li,3,Minhan Dai, an Guizhi Wang, oesponence to: M. Dai, mai@xmu.eu.cn.state Key Laboatoy of Maine Envionmental Science, Xiamen Univesity, Xiamen, hina,. ollege of Ocean an Eath Science, Xiamen Univesity, Xiamen, hina, 3. School of Physics, Huazhong Univesity of Science & Technology. Abstact In oe to bette compehen the global cabon cycle an peict the pognosis fo the esponse to climate change, accuate assessment of sea-ai O flux is necessay. ompaing to the elative homogeneously istibution of atmospheic O, the p O in the sea suface wate is expose to huge spatio-tempoal vaiability, which leaves a pominent uncetainty esouce. Many egional stuies typically ivie the obsevational p O ata into gi boxes so as to obtain enough ata points statistically fo thei calculatio. Howeve, using the ata insie the gi box aeas to epesent its holistic popety (such as stana eviation to epesent spatial vaiance) will mix up thee iffeent uncetainty souces. Fist, the analytical eo in the p O etemination an the associate envionmental paametes use in eiving p O. Secon, the spatial vaiance because of inhomogenous spatial patten of sea suface p O, especially the egion with a amatically ynamic cicumstance like: coastal aeas, bounaies o fonts an etc. Thi, the estimation pocess in unesampling conition, specifically, this kin of uncetainty oigins fom the pocess that using a spase ata to epesent its holistic popety of the box aea. ommon uncetainty quantification by Stana Deviation will mix up the iffeent souces of uncetainty. In this pape, it intouces an optimize poceue to etemine thee souces of uncetainty ( st analytical eo, n spatial vaiance, 3 bias fom unesampling.) using the combine emote sensing-eive an fiel-measue po ata. In oe to povie a compehensive eo assessment epot. Special Section Pacific-Asian Maginal Seas Key Points Thee souces of uncetainty of spase po ata. A new -D moel intouce in Kiging Estimation. ouple with emote sensing-eive ata to fit the -D moel. The uncetainties of spase po ata ae estimate.

2 . Intouction: Figue. Fom Global abon Buget 04 The continuing api accumulation of O in atmosphee inevitably each to an unpeceente level in human histoy, the 400 ppm mak [Global abon Buget 04]. In oe to bette compehen the global cabon cycle an peict the pognosis fo the esponse to climate change, accuate assessment of sea-ai O flux is necessay [Takahashi et al., 009, 00, 997]. Since 993, a global coopeate pogam, the DIA Ocean abon Data Management Poject, has been establishe fo collecting iscete an uneway measuement po ata. Thanks to temenous effot contibute by iniviual investigatos an goups, up till 04, moe than 9.0 million measuements of suface wate p O ata points mae ove the global oceans have been inclue in the LDEO atabase [Vesion 03]. Howeve, compaing to the elative homogeneously istibution of atmospheic O, the p O in the sea suface wate is expose to huge spatio-tempoal vaiability, which leaves a pominent uncetainty esouce. It iectly casts a shaow on the eliability of estimating the sea-ai flux. Many egional stuies typically ivie the obsevational p O ata into gi boxes so as to obtain enough ata points statistically fo thei calculation[e.g., Takahashi et al., 009; Zhai et al., 03]. Howeve, using the ata insie the gi box aeas to epesent its holistic popety (such as stana eviation to epesent spatial vaiance) will mix up thee iffeent uncetainty souces [Wang et al., 04]. Fist, the analytical eo in the p O etemination an the associate envionmental paametes use in eiving p O. Secon, the spatial vaiance because of inhomogenous spatial patten of sea suface p O, especially the egion with a amatically ynamic cicumstance like: coastal aeas, bounaies o fonts an etc [Sweeney et al., 03]. Thi, the estimation pocess in unesampling conition, specifically, this kin of uncetainty

3 oigins fom the pocess that using a spase ata to epesent its holistic popety of the box aea. Because of inhomogeneously an spasely istibution of sampling station points is common, coectly an efficiently quantifying those thee kins of uncetainties is stongly equie. This stuy bases on the spatial analysis an Kiging estimation, using a new two-imensional spatial coelation moel to quantify the contibution of the spatial vaiance an unesampling uncetainty in sea suface po ata an futhe to optimize the assessment of sea-ai O flux.. Analytical Eo (Em). Spatial Vaiance 3. The isk fom estimation in unesampling conition. Given that its necessity when evaluating iffeent stuies, ou appoach shall have wiely applications as an uncetainty analysis tools.. p O atabase an methoology to quantify the uncetainty of spase ata. Monitoing the vaiability of sea suface p O, people use ships an othe platfoms geneates lage amounts of ata fom heteogenous souces. Since 993, a global coopeate pogam via a numbe of U.S. an intenational ocean-obseving pogams, the DIA Ocean abon Data Management Poject has been establishe fo collection of iscete an uneway measuements po ata. The atabase use in this stuy ae fom an uneway measuements in ES August, 009 an Global Ocean Suface Wate Patial Pessue of O Database (Vesion 03). Figue. Flowchat of the quantifying uncetainty fo po ata. RS- po epesents emote sensing-eive po ata, an uneway epesents fiel-measue po ata. Fo a given sea suface po fiel ata set, the analytical eo, Em, is nomally calculate by aggegating all the eos intouce in the measuement an ata euction of po in many stuies[]. In this stuy, it will focus on a stana poceue fo estimating the est two souces of uncetainty, the spatial vaiance an unesamping. An this methoology will be moe efficient with ai of a concuent high-spatial-esolution satellite-eive po ata set fom [Bai et al., 05] in the same stuying egion. But, it is not equie so. The potocol of this metho will be summaize in a simplifie way in Figue.. Fist, using spatial ata (Uneway o Remote-Sensing measuements) to o the spatial analysis fo estimating a new two-imensional spatial coelation

4 moel. Secon, combining the obtaine statistical moel an uneway measuements to quantify the coelation of each ata pai. Then, basing on Oinay Kiging (OK) Estimation to povie a full coveage ata set of the stuy egion. Finally, estimate the spatial vaiance via calculating the stana eviation of the full coveage ata set an the unesampling uncetainty fom the estimation vaiance of OK. The etails will be as the following steps.. Spatial analysis an cicula segment moel. Fo a given spatial ata set, such as ES August 009, nomally they have an inheent popety, the spatial epenence in attibute values, which means the values fo the same attibute measue at locations that ae nea to one anothe ten to be simila, an ten to be moe simila than values sepaate by lage istances. In this stuy, in oe to povie an efficient an simple algoithm, we assume the epenency stuctue is also isotopic, the same on both axes, which is an ieal conition. Although this assumption oes not sufficiently consie the ocean system, which is pesistently ynamic in physical, chemical an biological pocess, it eflects some basic infomation o popety fom ata itself. The paticula steps to quantifying the stuctue of spatial epenency in a ata set will be fully iscusse in [Robet Haining, 993]. ˆ( h) [(/ N( h)) ( z( i) z( j))] z( i) z( j) i j [( i, j) ( i, j) h)] Whee, (h) is the estimate of spatial covaiance at istance h. Figue. is a conceptual example of a typical semi-vaiogam fo the case whee spatial epenence in attibute values. This spatial autocoelation analysis is the basis fo the next estimation. () Figue.3 (onceptual moel fo an autocovaiance function (h)). i Fom the above spatial coelation analysis, the next step is fitting statistical moel. onsieing ealing with a -imensional poblem, we popose a new -D statistical moel as shown in Figue.3. This moel epesents the coelation of two ata points by calculating the segment aea of them, also in the case of an isotopic weakly stationay pocesses. This means that any pemissable covaiance function also can be use as a moel fo the semi-vaiogam of a weakly stationay pocess, the etaile explanation ae given by [essie, 99, p87].

5 Figue.4 The -imensional covaiance statistical moel. Whee the ovelap of two ciculas at a istance will be calculate by the flowing fomula: ) ( acsin 4 A ovelaping () The covaiance function of this D moel is: icula Moel: a h a h h h 0 0 ] acsin 4 [ 0 ) ( 0 (3) The sill is the plateau a function eaches an which coespons to (0). The ange is the istance at which the plateau is eache. Detail see in [Robet Haining, 993, p95].. Deiving fom Kiging Estimation. Afte finishing the spatial analysis an moel fitting, the thee constants of statistical moel, icula Moel, will be known. An using this obtaine moel, we coul statistically quantifying each ata pai s coelation on aveage. Then, eiving the equations fom oinay kiging with two conitions in tems of D covaiance function. This peiction is the homogeneously linea combination of the ata set that minizizes the mean squae peiction eo an will be fully iscusse in [essie, 99].

6 n n nn 0 n 0 0n (4) The above equation set is to calculate a single estimation point, eive by us following Kiging oinay metho. An the esults will be the following: Estimation of a single point Z0. Uncetainty of OK estimation that bings in. Z n * 0 i i i Z( x ) (5) n ( 0) i(x 0, x i ) OK (6) i Using this metho, povie a full coveage estimation of spase ata set. Then, using N s ( Z i Z ), (7) N i to estimate the spatial vaiance via calculating the stana eviation of the full coveage ata set an the unesampling uncetainty fom the estimation vaiance of OK. n ( 0) i(x 0, x i ) u (8) i Finally, integating the thee uncetainty, the analytical eo, the spatial vaiance an the unesampling vaiance, an in this case, thee of them all ae totally inepenent. The total uncetainty () is: T Em s u (9) 3. Applications of the Uncetainty Quantification to iffeent cases. Fom above, we intouce a moifie Kiging estimation metho. This metho of quantifying uncetainty was applie to iffeent case stuies, such as, the uneway suface po ata fom the East hina Sea collecte in August 009, shown in Figue. The stana poceue will be like, spatial analysis (Figue.4), estimation of -D statistical moel an estimation of full coveage ata (Fig.5.a) an its uncetainty (Fig.5.b).

7 Figue.4 (a) Uneway suface po ata fom the East hina Sea collecte in August 009 fom [Wang et al., 04 ], (b)spatial covaiance function to this ata set. 3. Results Valiation (ES August, 009) Figue.5 (a) A full coveage estimation of ES August, 009 ata set. (b) The unesampling uncetainty istibution of each estimation points. While calculating this ata set o othe case stuies of a fiel tip. Thee ae always some locations of ata stations having the same cooinates, which means moe than one measuement at a single location. An it will cast a citical poblem fo this OK metho, because the equation set () is singula, not full ank, so that they can not be solve. In this stuy, we have use a tick to eal with this poblem, anomly isplacing each ata station a vey little bit in space, that the isplacement is tenth lowe the minimum esolution of uneway measuement. Howeve, it is still nee moe stuies to evaluate how much uncetainty will be taken in ue to this ough tactic.

8 Meanwhile, we have a concuent high-spatial-esolution satellite-eive po ata set fom [Bai et al., 05] in the same stuying egion shown in Figue.6. We can see a pominent coheence between estimations esults (Figue.5.a) an Remote-Sensing ata (Figue.6). An most impotantly, the istibution of unesampling uncetainty was stongly popotional to the ensity of uneway ata, which is quite ecent an logically. Hee, in this metho, it uses the sum of the squae eviation, N times vaiance, as the maxim of the estimation uncetainty. An fo each estimation points, the uncetainty will ecease when having some ajacent ata points. Basing on coelate ata an infomation will euce the isks of estimation, o specifically, uncetainty. Figue Othe ase Stuies- If Heteogeneity? Fom the cuent huge amount of po atabase, Aiming to avoi the lagely tempoal vaiability, we only picke up some fiel tips within a shot time peio, nomally less than half a month. Two typical cases will be iscusse in the following. Figue.7 (a).uneway measuement of uise: Bal Jan 995, ata fom DIA. (b) The autocovaiance function of this ata set. Fom above, it showe an inconfomity between the auto-coelation function an ieal moel. So as the esult, it showe a poo quality of not only the full coveage of estimation but also the uncetainty of estimation points. So, to pomote the quality of esults, we ecommen to geogaphically efine subsets of ata set if heteogeneity is suspecte as the uneway measuement showe, the obsevation coveage of this fiel tip can not fully etect its spatial stuctue.

9 3.3. If Ovelapping? Figue.8 (a) Uneway measuement of uise: GG08 May 008, ata fom DIA. (b) The full coveage of estimation. (c) The uncetainty of estimation. As shown in Figue.8, hee is an anothe typical status with confomity between the auto-coelation function an ieal moel. But, some ata stations have ovelappe. This will esult in a phenomenon calle nugget effect an also weaken the efficiency of this metho. 4. Summay Fom all above, we intouce a geneal metho to calculate the thee uncetainties of spatial spase ata, such as ou focus, the sea suface po ata. It successfully povies a full coveage of estimation an its uncetainty fo calculating the spatial vaiance an unesampling uncetainty of stuying egion. An if with ai of a concuent high-spatial-esolution satellite-eive po ata set, this metho will povie a moe obust esult. Howeve, the application of this metho to some fiel tip measuement fom DIA atabase still eveal some citical weakness in seveal typical conitions, fo instance, heteogeneity an ovelapping. onsieing this stuy will have a wiespea application in the futue, thee ae still some optimizing wok nee to be one.

10 Refeences: Bai, Y., W.-J. ai, X. He, W. Zhai, D. Pan, M. Dai, an P. Yu (05), A mechanistic semi-analytical metho fo emotely sensing sea suface po in ive-ominate coastal oceans: A case stuy fom the East hina Sea, Jounal of Geophysical Reseach: Oceans, 0(3), essie, N. (99), STATISTIS FOR SPATIAL DATA, Tea Nova, 4(5), 63&nash;67. essie, N., an N. H. han (989), Spatial Moeling of Regional Vaiables, Jounal of the Ameican Statistical Association, 84(406), Haining, R. (003), Spatial Data Analysis, Spatial Data Analysis, by Robet Haining, pp. 45. ISBN ambige, UK: ambige Univesity Pess, June 003., (), 45. Le Quéé,., et al. (05), Global cabon buget 04, Eath System Science Data, 7(), Legene, P. (993), Spatial autocoelation: touble o a new paaigm, Ecology, 74(6), Legene, P., N. L. Oen, R. R. Sokal, A. Vauo, an J. Kim (990), Appoximate analysis of vaiance of spatially autocoelate egional ata, Jounal of lassification, 7(), Shen, S. S. P., H. Yin, an T. M. Smith (007), An Estimate of the Sampling Eo Vaiance of the Gie GHN Monthly Suface Ai Tempeatue Data, Jounal of limate, 0(0), Shen, S. S. P.,. K. Lee, an J. Lawimoe (0), Uncetainties, Tens, an Hottest an olest Yeas of U.S. Suface Ai Tempeatue since 895: An Upate Base on the USHN V TOB Data, Jounal of limate, 5(), T, T., F. RA, W. RF, W. RH,. DW, S. S, an T. TT (997), Global ai-sea flux of O : An estimate base on measuements of sea ai po iffeence, Poceeings of the National Acaemy of Sciences, 94(6), Takahashi, T., S.. Suthelan, R. Wanninkhof,. Sweeney, R. A. Feely, D. W. hipman, B. Hales, G. Fieeich, F. havez, an. Sabine (009), limatological mean an ecaal change in suface ocean po, an net sea ai O flux ove the global oceans, Deep Sea Reseach Pat II: Topical Stuies in Oceanogaphy, 56(), Takahashi, T., et al. (00), Global sea ai O flux base on climatological suface ocean p O, an seasonal biological an tempeatue effects, Deep Sea Reseach Pat II: Topical Stuies in Oceanogaphy, 49(9 0), Tans, P. P., I. Y. Fung, an T. Takahashi (990), Obsevational contains on the global atmospheic O buget, Science, 47(4949), Taylo, J. R. (997), An intouction to Eo Analysis, Univesity Science Books, 56(4), Wang, G., M. Dai, S. S. P. Shen, Y. Bai, an Y. Xu (04), Quantifying uncetainty souces in the gie ata of sea sufaceo patial pessue, Jounal of Geophysical Reseach: Oceans, 9(8), Wanninkhof, R., G. Pak, an T. Takahashi (0), Global ocean cabon uptake: magnitue, vaiability an tens, Biogeosciences Discussions, 0(8),

Supplementary Information for On characterizing protein spatial clusters with correlation approaches

Supplementary Information for On characterizing protein spatial clusters with correlation approaches Supplementay Infomation fo On chaacteizing potein spatial clustes with coelation appoaches A. Shivananan, J. Unnikishnan, A. Raenovic Supplementay Notes Contents Deivation of expessions fo p = a t................................

More information

A Crash Course in (2 2) Matrices

A Crash Course in (2 2) Matrices A Cash Couse in ( ) Matices Seveal weeks woth of matix algeba in an hou (Relax, we will only stuy the simplest case, that of matices) Review topics: What is a matix (pl matices)? A matix is a ectangula

More information

Equilibria of a cylindrical plasma

Equilibria of a cylindrical plasma // Miscellaneous Execises Cylinical equilibia Equilibia of a cylinical plasma Consie a infinitely long cyline of plasma with a stong axial magnetic fiel (a geat fusion evice) Plasma pessue will cause the

More information

Quantum Mechanics I - Session 5

Quantum Mechanics I - Session 5 Quantum Mechanics I - Session 5 Apil 7, 015 1 Commuting opeatos - an example Remine: You saw in class that Â, ˆB ae commuting opeatos iff they have a complete set of commuting obsevables. In aition you

More information

GRAVITATION. Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., New Delhi -18 PG 1

GRAVITATION. Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., New Delhi -18 PG 1 Einstein Classes, Unit No. 0, 0, Vahman Ring Roa Plaza, Vikas Pui Extn., New Delhi -8 Ph. : 96905, 857, E-mail einsteinclasses00@gmail.com, PG GRAVITATION Einstein Classes, Unit No. 0, 0, Vahman Ring Roa

More information

PH126 Exam I Solutions

PH126 Exam I Solutions PH6 Exam I Solutions q Q Q q. Fou positively chage boies, two with chage Q an two with chage q, ae connecte by fou unstetchable stings of equal length. In the absence of extenal foces they assume the equilibium

More information

( )( )( ) ( ) + ( ) ( ) ( )

( )( )( ) ( ) + ( ) ( ) ( ) 3.7. Moel: The magnetic fiel is that of a moving chage paticle. Please efe to Figue Ex3.7. Solve: Using the iot-savat law, 7 19 7 ( ) + ( ) qvsinθ 1 T m/a 1.6 1 C. 1 m/s sin135 1. 1 m 1. 1 m 15 = = = 1.13

More information

Homework Set 3 Physics 319 Classical Mechanics

Homework Set 3 Physics 319 Classical Mechanics Homewok Set 3 Phsics 319 lassical Mechanics Poblem 5.13 a) To fin the equilibium position (whee thee is no foce) set the eivative of the potential to zeo U 1 R U0 R U 0 at R R b) If R is much smalle than

More information

Physics 122, Fall December 2012

Physics 122, Fall December 2012 Physics 1, Fall 01 6 Decembe 01 Toay in Physics 1: Examples in eview By class vote: Poblem -40: offcente chage cylines Poblem 8-39: B along axis of spinning, chage isk Poblem 30-74: selfinuctance of a

More information

CHAPTER 2 DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE. 2.1 Derivation of Machine Equations

CHAPTER 2 DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE. 2.1 Derivation of Machine Equations 1 CHAPTER DERIVATION OF STATE EQUATIONS AND PARAMETER DETERMINATION OF AN IPM MACHINE 1 Deivation of Machine Equations A moel of a phase PM machine is shown in Figue 1 Both the abc an the q axes ae shown

More information

A Lattice Energy Calculation for LiH

A Lattice Energy Calculation for LiH A Lattice Enegy Calculation fo LiH Fank Riou Lithium hyie is a white cystalline soli with the face-centee cubic cystal stuctue (see lattice shown below). The moel fo LiH(s) popose in this stuy constists

More information

Morphology of composite films: a computer study. Stanislav Novák

Morphology of composite films: a computer study. Stanislav Novák Supeficies y acío 9, 48-5, Diciembe 1999 Mophology of composite films: a compute stuy Stanislav Novák Depatment of Physics, J.E.Pukynì Univesity, Èeské mláeže 8, 400 96 Ústí na Labem, Czech Republic Ruolf

More information

15. SIMPLE MHD EQUILIBRIA

15. SIMPLE MHD EQUILIBRIA 15. SIMPLE MHD EQUILIBRIA In this Section we will examine some simple examples of MHD equilibium configuations. These will all be in cylinical geomety. They fom the basis fo moe the complicate equilibium

More information

Section 5: Magnetostatics

Section 5: Magnetostatics ection 5: Magnetostatics In electostatics, electic fiels constant in time ae pouce by stationay chages. In magnetostatics magnetic fiels constant in time ae pouces by steay cuents. Electic cuents The electic

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

MAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates,

MAE 210B. Homework Solution #6 Winter Quarter, U 2 =r U=r 2 << 1; ) r << U : (1) The boundary conditions written in polar coordinates, MAE B Homewok Solution #6 Winte Quate, 7 Poblem a Expecting a elocity change of oe oe a aial istance, the conition necessay fo the ow to be ominate by iscous foces oe inetial foces is O( y ) O( ) = =

More information

Acoustic Impedances of Audiometric Earphones Coupled to Different Loads

Acoustic Impedances of Audiometric Earphones Coupled to Different Loads Acoustic Impeances of Auiometic Eaphones Couple to Diffeent Loas Dejan Ćiić, Dote Hammeshøi Depatment of Acoustics, Aalbog Univesity, DK-9 Aalbog, Feeik Bajes Vej 7B 5, Denmak, {c, h}@acoustics.aau.k The

More information

Psychometric Methods: Theory into Practice Larry R. Price

Psychometric Methods: Theory into Practice Larry R. Price ERRATA Psychometic Methods: Theoy into Pactice Lay R. Pice Eos wee made in Equations 3.5a and 3.5b, Figue 3., equations and text on pages 76 80, and Table 9.1. Vesions of the elevant pages that include

More information

Much that has already been said about changes of variable relates to transformations between different coordinate systems.

Much that has already been said about changes of variable relates to transformations between different coordinate systems. MULTIPLE INTEGRLS I P Calculus Cooinate Sstems Much that has alea been sai about changes of vaiable elates to tansfomations between iffeent cooinate sstems. The main cooinate sstems use in the solution

More information

Example

Example Chapte.4 iffusion with Chemical eaction Example.4- ------------------------------------------------------------------------------ fluiize coal eacto opeates at 45 K an atm. The pocess will be limite by

More information

Sensitivity Analysis of SAW Technique: the Impact of Changing the Decision Making Matrix Elements on the Final Ranking of Alternatives

Sensitivity Analysis of SAW Technique: the Impact of Changing the Decision Making Matrix Elements on the Final Ranking of Alternatives Ianian Jounal of Opeations Reseach Vol. 5, No. 1, 2014, pp. 82-94 Sensitivity Analysis of SAW Technique: the Impact of Changing the Decision Maing Matix Elements on the Final Raning of Altenatives A. Alinezha

More information

Mitscherlich s Law: Sum of two exponential Processes; Conclusions 2009, 1 st July

Mitscherlich s Law: Sum of two exponential Processes; Conclusions 2009, 1 st July Mitschelich s Law: Sum of two exponential Pocesses; Conclusions 29, st July Hans Schneebege Institute of Statistics, Univesity of Elangen-Nünbeg, Gemany Summay It will be shown, that Mitschelich s fomula,

More information

N igerian Journal of M athematics and Applications V olume 24, (2015),

N igerian Journal of M athematics and Applications V olume 24, (2015), N igeian Jounal of M athematics an Applications V olume 24, 205), 228 236 c N ig. J. M ath. Appl. http : //www.kwsman.com Flow of an Incompessible MHD Thi Gae Flui Though a Cylinical Pipe with Isothemal

More information

Solutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook

Solutions to Problems : Chapter 19 Problems appeared on the end of chapter 19 of the Textbook Solutions to Poblems Chapte 9 Poblems appeae on the en of chapte 9 of the Textbook 8. Pictue the Poblem Two point chages exet an electostatic foce on each othe. Stategy Solve Coulomb s law (equation 9-5)

More information

Nuclear Medicine Physics 02 Oct. 2007

Nuclear Medicine Physics 02 Oct. 2007 Nuclea Medicine Physics Oct. 7 Counting Statistics and Eo Popagation Nuclea Medicine Physics Lectues Imaging Reseach Laboatoy, Radiology Dept. Lay MacDonald 1//7 Statistics (Summaized in One Slide) Type

More information

Sensors and Actuators Introduction to sensors

Sensors and Actuators Introduction to sensors Sensos an ctuatos Intouction to sensos Sane Stuijk (s.stuijk@tue.nl) Depatment of Electical Engineeing Electonic Systems PITIE SENSORS (hapte 3., 7., 9.,.6, 3., 3.) 3 Senso classification type / quantity

More information

ON A CLASS OF SKEWED DISTRIBUTIONS GENERATED BY A MIXING MECHANISM

ON A CLASS OF SKEWED DISTRIBUTIONS GENERATED BY A MIXING MECHANISM Fa East Jounal of Mathematical Sciences (FJMS) 5 Pushpa Publishing House, Allahaba, Inia Publishe Online: Novembe 5 http://x.oi.og/.7654/fjmsdec5_857_87 Volume 98, Numbe 7, 5, Pages 857-87 ISSN: 97-87

More information

Recent Advances in Chemical Engineering, Biochemistry and Computational Chemistry

Recent Advances in Chemical Engineering, Biochemistry and Computational Chemistry Themal Conductivity of Oganic Liquids: a New Equation DI NICOLA GIOVANNI*, CIARROCCHI ELEONORA, PIERANTOZZI ARIANO, STRYJEK ROAN 1 DIIS, Univesità Politecnica delle ache, 60131 Ancona, ITALY *coesponding

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

Jerk and Hyperjerk in a Rotating Frame of Reference

Jerk and Hyperjerk in a Rotating Frame of Reference Jek an Hypejek in a Rotating Fame of Refeence Amelia Caolina Spaavigna Depatment of Applie Science an Technology, Politecnico i Toino, Italy. Abstact: Jek is the eivative of acceleation with espect to

More information

Electric Potential and Gauss s Law, Configuration Energy Challenge Problem Solutions

Electric Potential and Gauss s Law, Configuration Energy Challenge Problem Solutions Poblem 1: Electic Potential an Gauss s Law, Configuation Enegy Challenge Poblem Solutions Consie a vey long o, aius an chage to a unifom linea chage ensity λ a) Calculate the electic fiel eveywhee outsie

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

Stability of a Discrete-Time Predator-Prey System with Allee Effect

Stability of a Discrete-Time Predator-Prey System with Allee Effect Nonlinea Analsis an Diffeential Equations, Vol. 4, 6, no. 5, 5-33 HIKARI Lt, www.m-hikai.com http://.oi.og/.988/nae.6.633 Stabilit of a Discete-Time Peato-Pe Sstem with Allee Effect Ming Zhao an Yunfei

More information

Hidden Two-Step Phase Transition and Competing

Hidden Two-Step Phase Transition and Competing Suppoting Infomation fo Hien Two-Step Phase Tansition an Competing Reaction Pathways in LiFePO 4 Yukinoi Koyama, Takeshi Uyama, Yuki Oikasa, Takahio Naka, Hieyuki Komatsu, Keiji Shimoa, Hauno Muayama,

More information

arxiv: v2 [astro-ph] 16 May 2008

arxiv: v2 [astro-ph] 16 May 2008 New Anomalies in Cosmic Micowave Backgound Anisotopy: Violation of the Isotopic Gaussian Hypothesis in Low-l Modes Shi Chun, Su and M.-C., Chu Depatment of Physics and Institute of Theoetical Physics,

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

That is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton.

That is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton. PHY 8 Test Pactice Solutions Sping Q: [] A poton an an electon attact each othe electically so, when elease fom est, they will acceleate towa each othe. Which paticle will have a lage acceleation? (Neglect

More information

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms

Pearson s Chi-Square Test Modifications for Comparison of Unweighted and Weighted Histograms and Two Weighted Histograms Peason s Chi-Squae Test Modifications fo Compaison of Unweighted and Weighted Histogams and Two Weighted Histogams Univesity of Akueyi, Bogi, v/noduslód, IS-6 Akueyi, Iceland E-mail: nikolai@unak.is Two

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

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

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s

MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Depatment Physics 8.033 Decembe 5, 003 Poblem Set 10 Solutions Poblem 1 M s y x test paticle The figue above depicts the geomety of the poblem. The position

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

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

Do Managers Do Good With Other People s Money? Online Appendix

Do Managers Do Good With Other People s Money? Online Appendix Do Manages Do Good With Othe People s Money? Online Appendix Ing-Haw Cheng Haison Hong Kelly Shue Abstact This is the Online Appendix fo Cheng, Hong and Shue 2013) containing details of the model. Datmouth

More information

Passivity-Based Control of Saturated Induction Motors

Passivity-Based Control of Saturated Induction Motors Passivity-Base Contol of Satuate Inuction otos Levent U. Gökee, embe, IEEE, awan A. Simaan, Fellow, IEEE, an Chales W. Bice, Senio embe, IEEE Depatment of Electical Engineeing Univesity of South Caolina

More information

General Relativity Homework 5

General Relativity Homework 5 Geneal Relativity Homewok 5. In the pesence of a cosmological constant, Einstein s Equation is (a) Calculate the gavitational potential point souce with = M 3 (). R µ Rg µ + g µ =GT µ. in the Newtonian

More information

2. Radiation Field Basics I. Specific Intensity

2. Radiation Field Basics I. Specific Intensity . Raiation Fiel Basics Rutten:. Basic efinitions of intensity, flux Enegy ensity, aiation pessue E Specific ntensity t Pencil beam of aiation at position, iection n, caying enegy E, pasg though aea, between

More information

of Technology: MIT OpenCourseWare). (accessed MM DD, YYYY). License: Creative Commons Attribution- Noncommercial-Share Alike.

of Technology: MIT OpenCourseWare).   (accessed MM DD, YYYY). License: Creative Commons Attribution- Noncommercial-Share Alike. MIT OpenCouseWae http://ocw.mit.eu 6.013/ESD.013J Electomagnetics an Applications, Fall 005 Please use the following citation fomat: Makus Zahn, Eich Ippen, an Davi Staelin, 6.013/ESD.013J Electomagnetics

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

DPA Modeling in MARS15

DPA Modeling in MARS15 DPA Moeling in MARS15 N. Mokhov (Femilab) NBI2017+RaDIATE IVIL Tokai Japan Septembe 18-22 2017 Outline Intouction DPA Theoetical Moels fo Chage Paticles an High- Enegy Neutons an Databases fo E < 150 MeV

More information

Conservative Averaging Method and its Application for One Heat Conduction Problem

Conservative Averaging Method and its Application for One Heat Conduction Problem Poceedings of the 4th WSEAS Int. Conf. on HEAT TRANSFER THERMAL ENGINEERING and ENVIRONMENT Elounda Geece August - 6 (pp6-) Consevative Aveaging Method and its Application fo One Heat Conduction Poblem

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

arxiv: v2 [physics.data-an] 15 Jul 2015

arxiv: v2 [physics.data-an] 15 Jul 2015 Limitation of the Least Squae Method in the Evaluation of Dimension of Factal Bownian Motions BINGQIANG QIAO,, SIMING LIU, OUDUN ZENG, XIANG LI, and BENZONG DAI Depatment of Physics, Yunnan Univesity,

More information

Multiple Criteria Secretary Problem: A New Approach

Multiple Criteria Secretary Problem: A New Approach J. Stat. Appl. Po. 3, o., 9-38 (04 9 Jounal of Statistics Applications & Pobability An Intenational Jounal http://dx.doi.og/0.785/jsap/0303 Multiple Citeia Secetay Poblem: A ew Appoach Alaka Padhye, and

More information

On a quantity that is analogous to potential and a theorem that relates to it

On a quantity that is analogous to potential and a theorem that relates to it Su une quantité analogue au potential et su un théoème y elatif C R Acad Sci 7 (87) 34-39 On a quantity that is analogous to potential and a theoem that elates to it By R CLAUSIUS Tanslated by D H Delphenich

More information

33. 12, or its reciprocal. or its negative.

33. 12, or its reciprocal. or its negative. Page 6 The Point is Measuement In spite of most of what has been said up to this point, we did not undetake this poject with the intent of building bette themometes. The point is to measue the peson. Because

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

Topic 4a Introduction to Root Finding & Bracketing Methods

Topic 4a Introduction to Root Finding & Bracketing Methods /8/18 Couse Instucto D. Raymond C. Rumpf Office: A 337 Phone: (915) 747 6958 E Mail: cumpf@utep.edu Topic 4a Intoduction to Root Finding & Backeting Methods EE 4386/531 Computational Methods in EE Outline

More information

F-IF Logistic Growth Model, Abstract Version

F-IF Logistic Growth Model, Abstract Version F-IF Logistic Gowth Model, Abstact Vesion Alignments to Content Standads: F-IFB4 Task An impotant example of a model often used in biology o ecology to model population gowth is called the logistic gowth

More information

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution

Central Coverage Bayes Prediction Intervals for the Generalized Pareto Distribution Statistics Reseach Lettes Vol. Iss., Novembe Cental Coveage Bayes Pediction Intevals fo the Genealized Paeto Distibution Gyan Pakash Depatment of Community Medicine S. N. Medical College, Aga, U. P., India

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

2. The Munich chain ladder method

2. The Munich chain ladder method ntoduction ootstapping has become vey popula in stochastic claims eseving because of the simplicity and flexibility of the appoach One of the main easons fo this is the ease with which it can be implemented

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

THE HERMITE POLYNOMIAL & QUANTIZATION OF THE HARMONIC OSCILLATOR

THE HERMITE POLYNOMIAL & QUANTIZATION OF THE HARMONIC OSCILLATOR THE HERMITE POLYNOMIAL & QUANTIZATION OF THE HARMONIC OSCILLATOR TIMOTHY JONES Abstact. The hamonic oscillato possesses a singula place in quantum mechanics. It is use in a wie vaiety of moels. Hee we

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

Hammerstein Model Identification Based On Instrumental Variable and Least Square Methods

Hammerstein Model Identification Based On Instrumental Variable and Least Square Methods Intenational Jounal of Emeging Tends & Technology in Compute Science (IJETTCS) Volume 2, Issue, Januay Febuay 23 ISSN 2278-6856 Hammestein Model Identification Based On Instumental Vaiable and Least Squae

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

Online Appendix Appendix A: Numerical Examples

Online Appendix Appendix A: Numerical Examples Aticle submitte to Management Science; manuscipt no. MS-15-2369 1 Online Appenix Appenix A: Numeical Examples We constuct two instances of the ecycling netwok (RN) base on the EPR implementation in Washington

More information

HW Solutions # MIT - Prof. Please study example 12.5 "from the earth to the moon". 2GmA v esc

HW Solutions # MIT - Prof. Please study example 12.5 from the earth to the moon. 2GmA v esc HW Solutions # 11-8.01 MIT - Pof. Kowalski Univesal Gavity. 1) 12.23 Escaping Fom Asteoid Please study example 12.5 "fom the eath to the moon". a) The escape velocity deived in the example (fom enegy consevation)

More information

Inverse Square Law and Polarization

Inverse Square Law and Polarization Invese Squae Law and Polaization Objectives: To show that light intensity is invesely popotional to the squae of the distance fom a point light souce and to show that the intensity of the light tansmitted

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. descibed the motion of objects using paametes such as the position vecto, velocity and acceleation without any insights as to

More information

r cos, and y r sin with the origin of coordinate system located at

r cos, and y r sin with the origin of coordinate system located at Lectue 3-3 Kinematics of Rotation Duing ou peious lectues we hae consideed diffeent examples of motion in one and seeal dimensions. But in each case the moing object was consideed as a paticle-like object,

More information

That is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton.

That is, the acceleration of the electron is larger than the acceleration of the proton by the same factor the electron is lighter than the proton. PHYS 55 Pactice Test Solutions Fall 8 Q: [] poton an an electon attact each othe electicall so, when elease fom est, the will acceleate towa each othe Which paticle will have a lage acceleation? (Neglect

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

Information Retrieval Advanced IR models. Luca Bondi

Information Retrieval Advanced IR models. Luca Bondi Advanced IR models Luca Bondi Advanced IR models 2 (LSI) Pobabilistic Latent Semantic Analysis (plsa) Vecto Space Model 3 Stating point: Vecto Space Model Documents and queies epesented as vectos in the

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

LET a random variable x follows the two - parameter

LET a random variable x follows the two - parameter INTERNATIONAL JOURNAL OF MATHEMATICS AND SCIENTIFIC COMPUTING ISSN: 2231-5330, VOL. 5, NO. 1, 2015 19 Shinkage Bayesian Appoach in Item - Failue Gamma Data In Pesence of Pio Point Guess Value Gyan Pakash

More information

Macro Theory B. The Permanent Income Hypothesis

Macro Theory B. The Permanent Income Hypothesis Maco Theoy B The Pemanent Income Hypothesis Ofe Setty The Eitan Beglas School of Economics - Tel Aviv Univesity May 15, 2015 1 1 Motivation 1.1 An econometic check We want to build an empiical model with

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

Bifurcation Analysis for the Delay Logistic Equation with Two Delays

Bifurcation Analysis for the Delay Logistic Equation with Two Delays IOSR Jounal of Mathematics (IOSR-JM) e-issn: 78-578, p-issn: 39-765X. Volume, Issue 5 Ve. IV (Sep. - Oct. 05), PP 53-58 www.iosjounals.og Bifucation Analysis fo the Delay Logistic Equation with Two Delays

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

Mobility of atoms and diffusion. Einstein relation.

Mobility of atoms and diffusion. Einstein relation. Mobility of atoms and diffusion. Einstein elation. In M simulation we can descibe the mobility of atoms though the mean squae displacement that can be calculated as N 1 MS ( t ( i ( t i ( 0 N The MS contains

More information

Basic oces an Keple s Laws 1. Two ientical sphees of gol ae in contact with each othe. The gavitational foce of attaction between them is Diectly popotional to the squae of thei aius ) Diectly popotional

More information

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables).

In many engineering and other applications, the. variable) will often depend on several other quantities (independent variables). II PARTIAL DIFFERENTIATION FUNCTIONS OF SEVERAL VARIABLES In man engineeing and othe applications, the behaviou o a cetain quantit dependent vaiable will oten depend on seveal othe quantities independent

More information

4. Some Applications of first order linear differential

4. Some Applications of first order linear differential August 30, 2011 4-1 4. Some Applications of fist ode linea diffeential Equations The modeling poblem Thee ae seveal steps equied fo modeling scientific phenomena 1. Data collection (expeimentation) Given

More information

Lead field theory and the spatial sensitivity of scalp EEG Thomas Ferree and Matthew Clay July 12, 2000

Lead field theory and the spatial sensitivity of scalp EEG Thomas Ferree and Matthew Clay July 12, 2000 Lead field theoy and the spatial sensitivity of scalp EEG Thomas Feee and Matthew Clay July 12, 2000 Intoduction Neuonal population activity in the human cotex geneates electic fields which ae measuable

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

Do not turn over until you are told to do so by the Invigilator.

Do not turn over until you are told to do so by the Invigilator. UNIVERSITY OF EAST ANGLIA School of Mathematics Main Seies UG Examination 2015 16 FLUID DYNAMICS WITH ADVANCED TOPICS MTH-MD59 Time allowed: 3 Hous Attempt QUESTIONS 1 and 2, and THREE othe questions.

More information

New problems in universal algebraic geometry illustrated by boolean equations

New problems in universal algebraic geometry illustrated by boolean equations New poblems in univesal algebaic geomety illustated by boolean equations axiv:1611.00152v2 [math.ra] 25 Nov 2016 Atem N. Shevlyakov Novembe 28, 2016 Abstact We discuss new poblems in univesal algebaic

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

MEASURING CHINESE RISK AVERSION

MEASURING CHINESE RISK AVERSION MEASURING CHINESE RISK AVERSION --Based on Insuance Data Li Diao (Cental Univesity of Finance and Economics) Hua Chen (Cental Univesity of Finance and Economics) Jingzhen Liu (Cental Univesity of Finance

More information

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism

Physics 2020, Spring 2005 Lab 5 page 1 of 8. Lab 5. Magnetism Physics 2020, Sping 2005 Lab 5 page 1 of 8 Lab 5. Magnetism PART I: INTRODUCTION TO MAGNETS This week we will begin wok with magnets and the foces that they poduce. By now you ae an expet on setting up

More information

APPLICATIONS OF LUMPED PARAMETER MODELS FOR SIMULATION OF LOW-TEMPERATURE GEOTHERMAL RESERVOIRS

APPLICATIONS OF LUMPED PARAMETER MODELS FOR SIMULATION OF LOW-TEMPERATURE GEOTHERMAL RESERVOIRS PROCEEDINGS, Twenty-Eighth Wokshop on Geothemal Resevoi Engineeing Stanfod Univesity, Stanfod, Califonia, Januay 27-29, 23 SGP-TR-173 APPLICATIONS OF LUMPED PARAMETER MODELS FOR SIMULATION OF LOW-TEMPERATURE

More information

Estimation of the Correlation Coefficient for a Bivariate Normal Distribution with Missing Data

Estimation of the Correlation Coefficient for a Bivariate Normal Distribution with Missing Data Kasetsat J. (Nat. Sci. 45 : 736-74 ( Estimation of the Coelation Coefficient fo a Bivaiate Nomal Distibution with Missing Data Juthaphon Sinsomboonthong* ABSTRACT This study poposes an estimato of the

More information

CHAPTER 3 DIODES. NTUEE Electronics L. H. Lu 3-1

CHAPTER 3 DIODES. NTUEE Electronics L. H. Lu 3-1 CHAPER 3 OE Chapte Outline 3.1 he eal ioe 3.2 eminal Chaacteistics of Junction ioes 3.3 Moeling the ioe Fowa Chaacteistics 3.4 Opeation in the Reese Beakown Region ene ioes 3.5 Rectifie Cicuits 3.6 Limiting

More information

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D.

Research Design - - Topic 17 Multiple Regression & Multiple Correlation: Two Predictors 2009 R.C. Gardner, Ph.D. Reseach Design - - Topic 7 Multiple Regession & Multiple Coelation: Two Pedictos 009 R.C. Gadne, Ph.D. Geneal Rationale and Basic Aithmetic fo two pedictos Patial and semipatial coelation Regession coefficients

More information

6 PROBABILITY GENERATING FUNCTIONS

6 PROBABILITY GENERATING FUNCTIONS 6 PROBABILITY GENERATING FUNCTIONS Cetain deivations pesented in this couse have been somewhat heavy on algeba. Fo example, detemining the expectation of the Binomial distibution (page 5.1 tuned out to

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

To Feel a Force Chapter 7 Static equilibrium - torque and friction

To Feel a Force Chapter 7 Static equilibrium - torque and friction To eel a oce Chapte 7 Chapte 7: Static fiction, toque and static equilibium A. Review of foce vectos Between the eath and a small mass, gavitational foces of equal magnitude and opposite diection act on

More information

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE

LINEAR AND NONLINEAR ANALYSES OF A WIND-TUNNEL BALANCE LINEAR AND NONLINEAR ANALYSES O A WIND-TUNNEL INTRODUCTION BALANCE R. Kakehabadi and R. D. Rhew NASA LaRC, Hampton, VA The NASA Langley Reseach Cente (LaRC) has been designing stain-gauge balances fo utilization

More information