Effects of Spatial Variability on Annual Average Water Balance

Size: px
Start display at page:

Download "Effects of Spatial Variability on Annual Average Water Balance"

Transcription

1 WATER RESOURCES RESEARCH, VOL. 23, NO. 11, PAGES , NOVEMBER 1987 Effects f Spatial Variability n Annual Average Water Balance P. C. D. M!LLY Department f Civil Engineering, Water Resurces Prgram, Princetn University, Princetn, New Jersey P.S. EAGLESON Department f Civil Engineering, Massachusetts Institute f Technlgy, Cambridge Spatial variability f sil and vegetatin causes spatial variability f the water balance. Fr an area in which the water balance is nt affected by lateral water flw, the frequency distributins f strm surface runff, evaptranspiratin, and drainage t grundwater are derivable frm distributins f sil hydraulic parameters by means f a pint water balance mdel and lcal applicatin f the vegetal equilibrium hypthesis. Means and variances f the cmpnents f the budget can be fund by Mnte Carl simulatin r by apprximate lcal expansins. Fr a fixed set f mean sil parameters, sil spatial variability may induce significant changes in the areal mean water balance, particularly if strm surface runff ccurs. Variability f the pre size distributin index and permeability has a much larger effect than that f effective prsity n the means and variances f water balance variables. The imprtance f the pre size distributin index implies that the micrscpic similarity assumptin may underestimate the effects f sil spatial variability. In general, the presence f sil variability reduces the sensitivity f water balance t mean prperties. Fr small levels f sil variability, there exists a unique equivalent hmgeneus sil type that reprduces the budget cmpnents and the mean sil misture saturatin f an inhmgeneus area. INTRODUCTION The lcal hydrlgic respnse f the land surface t atmspheric frcing (precipitatin, slar and atmspheric radiatin, etc.) is determined by the prperties f the surface and by the frcing. Bth f these factrs may vary significantly at spatial scales smaller than the scale f practical hydrlgic analyses. Since analyses f small-scale physical prcesses in catchments suggest that the lcal respnse is a nnlinear functin f these variables, we infer that the prblem f spatial integratin t the catchment scale is nt trivial. It is nt at all clear, fr example, under what cnditins a ne-dimensinal mdel f the sil bundary layer, grunded in sil water hydrdynamics, can represent the average behavir f a spatially variable natural catchment. This prblem f lcal variability has been ne f the majr impediments t the successful applicatin f Darcy scale physical thery t explain hydrlgic respnse at catchment scales. Variability f atmspheric frcing is mst apparent in the hetergeneity f rainfall fields. Individual strms have significant internal spatial and tempral structure and are generally in mtin relative t the grund. The result is that rainfall intensity histries, and even aggregate quantities such as ttal strm depth, are smetimes variable at scales smaller than thse f the catchment f interest. With increasingly large averaging perids (i.e., many strms), the spatial crrelatin naturally increases. Hwever, the shrt-term hydrlgic respnse is nt necessarily determined uniquely by such lngtime averages, whse unifrmity is therefre nt especially helpful in the analysis f single events. On the ther hand, the time average water balance can be parameterized in terms f rainfall statistics that are quite unifrm spatially. Variability f the land surface (itself, the sil texture and Cpyright 1987 by the American Gephysical Unin. Paper number 7W /87/007W structure, the vegetatin type and density, and gemrphlgical parameters), is the secnd majr surce f variability f hydrlgic fluxes. Sil prperties affect the ability f the sil surface bundary layer t transmit water int r frm the sil. The vegetatin alternately enhances r hinders the transmissin prcess. Gemrphlgical factrs f imprtance include thse inducing lateral subsurface flws, which cmplicate (and ften gvern) the direct runff generatin prcess. The spatial variability f the surface, unlike that f the frcing, is a factr that cannt be eliminated by averaging in time; surface prperties f untilled sils are s persistent in time as t be effectively static. In this paper we examine the effect f spatial variability f sil and vegetatin n water balance. In particular, we are cncerned with the extent t which their areal variatins affect the tempral-spatial averages f the majr hydrlgic fluxes. We are als interested in the questin f the existence f an equivalent hmgeneus sil capable f reprducing the average behavir f an inhmgeneus area. Theretical analyses f water balance n spatially variable sils have been described by Peck et al. [1977] and by Sharma and Luxmre [1979]. They emplyed dynamic simulatin mdels in analyses f the water balance f a particular catchment n a mnthly time scale, accunting fr strage changes. Sil spatial variability was represented using the cncept f micrscpic scale similarity. Sharma and Luxmre demnstrated the imprtance f sil variability and nted the difficulty f making generalizatins in light f the dependence f results n the sil-plant-weather cmbinatin. They bserved that their neglect f variatins f vegetatin prperties assciated with sil variability was unrealistic. Our treatment fllws the basic apprach first laid dwn by Peck et al. [1977-1, but ffers several new insights, primarily as a result f ur different apprach t the pint water balance. By restricting ur attentin t the annual average water balance, we are able t emply the results f Eaglesn [1978a, b, 2135

2 2136 MILLY AND EAGLESON: EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE c, d, e, f, g], which cncisely express the majr cmpnents f the water balance as functins f sil and atmspheric parameters and which accunt fr the dependence f equilibrium vegetatin densities n sil prperties. The cmputatinal simplicity f the water balance mdel allws us t btain detailed results regarding the sensitivity f average hydrlgic fluxes t the variance f sil parameters fr a wide range f sil types and climatic cnditins. It als permits us t examine the effect f departures frm micrscpic similarity in the analysis. Just as imprtant, the parametric frugality f the mdel allws us t infer frm thse results sme relatively general cnclusins regarding the effects f sil spatial variability. In what fllws the term "water balance" will refer t the annual average water balance, which will be further averaged here in space. FRAMEWORK Climate Parameters d, average rate f ptential evapratin; mt mean time between strms; mtr mean strm duratin; m mean duratin f rainy seasn; mpa mean annual rainfall; c parameter f gamma distributin f strm depth' a mean annual air temperature. Other Parameters h 0 surface retentin capacity; Z effective depth t water table; k v ptential transpiratin efficiency; M vegetal canpy density. Given these parameters, the water balance mdel yields expected values f the fllwing variables' We suppse that an inhmgeneus area A may be repre- S average sil misture saturatin; sented, t first rder, as a battery f parallel, independent, ETA annual evaptranspiratin; ne-dimensinal sil clumns, each described by a deterministic mdel yielding utputs as functins f lcal inputs and RsA annual surface runff; Rg A annual recharge t grundwater. parameters. In rder t derive the areal average water balance, Furthermre, invcatin f the vegetal equilibrium hypthesis we integrate the pint water balance ver the regin A, using [Eaglesn, 1978f-] allws us t slve the water balance withthe jint density functin f the sil prperties as a weighting ut specifying M;in that case, the water balance mdel als functin. Thus if y is any utput dependent n the sil prperprvides the value f M as an utput. Accrding t the equities t with jint frequency distributin f(t) in A, then the librium hypthesis, natural systems f vegetatin evlve areal average (y), defined by tward a canpy density that maximizes the average sil misture saturatin. dx (1) With respect climate, nly certain lng-term statistics are prescribed; the mdel implicitly perfrms a time average f is given by the dynamics [Eaglesn, 1978a, b, c, d, e, f, g]. In cntrast, cnstant sil parameters are specified, with the implicatin that the mdel is based n a physical cnceptin f hmge- (Y) =, g( )f( ) d (2) neity within the mdeled area. Direct applicatin f the mdel t a hetergeneus area implicitly requires an assumptin that in which x is the spatial crdinate, g( ) is the utput func- "effective" sil parameters may be defined. This assumptin is tin relating t t y, and fl is the set f all t fund in A. examined in a later sectin f this paper. (Ntatin fllws the main text f this paper.) One f the critical assumptins underlying the ne- In principle, the areal integratin shuld include nt nly dimensinal water balance mdel used here is that surface the sil parameters, but als the inputs, such as rainfall and runff is generated nly by the infiltratin-excess mechanism. ptential evapratin rate. While these may be highly variable There is n prvisin fr runff prduced at riparian seepage in space at any time, it is nly climatic statistics that enter the faces. Our cnclusins are therefre limited t catchments fr water balance mdel we use t represent g( ). These statistics which this assumptin is valid r t thse prtins f catchexhibit cnsiderably greater crrelatin in space than the in- ments in which the water table des nt apprach the surface. stantane s values, but, f curse, may als have significant spatial variability. We are therefre ignring such temprally JOINT DENSITY OF SOIL PARAMETERS cnstant, spatially variable effects as rgraphic influences n In rder t prceed within the prpsed framewrk, we rainfall statistics, tpgraphic influences n net radiatin, and require a statistical descriptin f the distributins and crres frth. latins f the three independent sil parameters n e, k(1), and m, which we dente cllectively by. The nature f the jint POINT WATER BALANCE We emply the statistical-dynamic water balance mdel f Eaglesn a, b, c, d, e, f, g] t explain, t first rder, the transfrmatin f lcal hydrlgic inputs and surface prperties t hydrlgic fluxes. The input parameters t the mdel are defined as fllws. Sil Parameters variability f these parameters has nt been well-defined and is an area f nging research. The marginal distributins f sme hydraulic parameters have been studied, either directly r indirectly, by a number f investigatrs. The analyses are mainly f tw basic types. In the first, data are cllected frm numerus surces f wide gegraphic rigin and gruped by sil textural classificatin. The resulting statistics characterize variability within a texture class ver the set f all sils. Such ne effective prsity f sil; analyses have been reprted by Clapp and Hrnberger [19783, k(1) sil permeability; by Brakensiek et al. [1981], and by Rawls et al. [1982]. The m pre size distributin index f sil. secnd type f analysis uses a large set f data frm a single

3 MILLY AND EAGLESON: EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE 2137 lcatin, field, r watershed t develp the densities, and therefre seems mre relevant t the current analysis. Warrick and Nielsen [1980] prvide a review f the earlier wrk in this area, and numerus wrks have been published subsequently, particularly in the sil science literature. It is rather well-established that the hydraulic cnductivity, and hence the intrinsic permeability, is ften lgnrmally distributed in the field. Effective prsity is sufficiently wellrepresented by the nrmal distributin. The parameter m, which is the expnent in the Brks-Crey [Brks and Crey, 1964] equatin fr the sil misture characteristic, was fund t be lgnrmal by Brakensiek et al. [1981] within a textural class, but its lcal variability within a field r a catchment has nt received much attentin. Our investigatins f available sil misture retentin data supprt the use f the lgnrmal distributin at the lcal scale. On the basis f the freging, we adpt the multivariate nrmal distributin t describe sil variability in this wrk. We treat he, In [k(1)], and In (m) as the three variates, dented by IO)il [1 ne ] 1 [ln(m)_] m = r 2 = n [k(1) (3) Then the jint density functin f m is f(t) = (2zr)3/2[Q[ /2 exp [-«(t -- III)TQ - (0}-- IIl)] (4) (T (0.6) BYERS AND STEPHENS (1983) x TRANSECT (I.2)... ANDERSON AND CASSEL (1986) (I. I) A HORIZON COELHO (1974) 300 mm DEPTH (0.8) AHUJA et l. (1984) O- 150mm DEPTH (0.9) NIELSEN et l. (1973) (I.8) 305mm LOAMY SAND DEPTH "] _ (2'0)(2 )7) SANDY LOAM [ LOAM,,,, (2.1). CLAY LOAM m (2.._5_) SlLTY CLAY [ ua (2.1) / SILTY CLAY LOAM) (2.5) ALL TEXTURES -2, IO -,5 tn[k(i),mm 2] Fig. 1. Fitted lgnrmal frequency distributins f k(1). Parenthetical numbers at left are values f a. in which (5) Q = EE(t - p)(t - p)r] (6) a a a2p 2 '10'3p 1 g3 lp31 g392p32 32 The vectr g is the mean value f, the matrix Q is the cvariance f, a is the standard deviatin f w, and Pu is the crrelatin f w and w. Fr cnvenience, we scale the standard deviatins by a parameter a, creases with the hrizntal dimensin, but there are bviusly ther imprtant factrs determining the sil variability. The data prvided by Brakensiek et al. [1981] can be prcessed t yield an estimate f a equal t 2.5 fr the entire United States f America. The hypthetical extreme case f an area having a bimdal sil distributin with permeabilities differing by a factr f 1000 yields a value f abut 3.5. Fr areas f interest fr the water balance prblem, it seems reasnable t fcus n values f ain the range frm abut WATER BALANCE SENSITIVITY TO THE SOIL VARIANCE ffi = ffo i= 1, 2, 3 (8) Mnte Carl Analysis f the Means The evaluatin f (2) is cmplicated by the fact that g( ) is We set f2 equal t unity, s a is equivalent t the standard nt knwn as an explicit functin; a numerical integratin deviatin f the lgarithm f permeability. We fix the values scheme is required. Since t is three-dimensinal and the ff and f3 as cnstants fr the entire investigatin. Based n evaluatin f g( ) is nt simple, a straightfrward disur interpretatin f sme f the limited available data, we cretizatin methd is cmputatinally unattractive. We intake f t be 0.05 and f3 t be 0.4. These shuld be cnsidered stead emply a Mnte Carl technique fr evaluatin f (2). as representative values with n universal significance. The We use a randm sampling scheme t generate numerus parameter a is used as an indicatr f the level f variability equally prbable values f t. With a set f N t i values s in the sil parameters. generated, we apprximate (2) accrding t It is helpful t cnsider the range f values that a may assume. Typical fitted frequency distributins f the lgarithm f permeability are pltted in Figure 1 fr representative textural classes and fr selected field sites; Table 1 summarizes the experimental findings f sme investigatrs. Fr sites Fr all results reprted in this paper, we used N equal t 500, whse characteristic hrizntal dimensin is 1000 m r less, the value f a typically ranges frm 0.5 t 1.0, but may becme even larger. Fr instance, Nielsen et al. [1973] fund which was fund thrugh numerus sensitivity analyses t be sufficient fr accurate estimatin f the means. We als examined the variances f the utputs, estimated accrding t the smaller values n a relatively hmgeneus field, while 1 N Andersn and Cassel [1986] fund values as high as 2.6, which O'y i 1 [ ](O)/) they speculated may have been caused by the presence f tree rt channels in the lwer sil hrizns. In general, a in- We have chsen the tw climatic data sets used by Eaglesn 1 N <y> =, a(t,) (9) -- <y>]2 (10)

4 2138 MILLY AND EAGLESON: EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE TABLE 1. Representative Values f S, the Standard Deviatin fln [k(1)] Characteristic Hrizntal Length f Site, Estimated Surce f Data m Sil a Byers and Stephens [1983] 15 fluival sand Cassel [1983] 60 Nrflk lamy sand Bresler et al. [1984] 90 Hamra Red Mediterranean Ahuja et al. [1984] 300 three silt lams Andersn and Cassel [1986] 500 Prtsmuth sandy lam Celh [1974] 1000 Pima clay lam Nielsen et al. [1973] 1500 Panche sil series Brakensiek et al. [1981] 5 x USDA texture classes Brakensiek et al. [1981] 5 x 106 all textures cmbined 2.5 [1978f]; the data fr Clintn, Massachusetts, and fr Santa mean value f In [k(1)], with n e and In (m) remaining fixed. Paula, Califrnia, are summarized in Table 2. Fr the sil parameters, the mean values!s are assigned the values given by Eaglesn ['1978e] as typical fr each f fur textural classes f sil; these are given in Table 3. We cnsider the case where there is n crss-crrelatin amng the sil parameters. We cnsider nly the case when the surface retentin capacity is negligible and the water table is s deep that there is n capillary rise t the surface. We take k v t be unity, and we Figure 4 shws, fr the Clintn climate, the sensitivity f the water balance t In [k(1)] fr a hmgeneus sil and fr a sil with a - equal t 6. Nt nly is the sensitivity f the balance t the mean generally reduced by inhmgeneity, but additinally the curves fr the inhmgeneus case are remarkably linear ver the range f pssible means. Several similar calculatins revealed that the effect f averaging is similar fr In (m) and fr the ther sil-climate cmbinatins. emply the vegetal equilibrium hypthesis t evaluate M. Figure 2 displays the slutins fr mean sil water satu- Mnte Carl Analysis f the Variances ratin s f the fur sils at bth lcatins. The parameter s We calculated the variances f the varius water balance is pltted as a functin f variability f sil type. One striking feature f these plts is the relatively small dependence f s utputs accrding t (10). In ur discussin f the results, we shall fcus n the cases f sandy lam and clay lam sils n the sil variance. The secnd remarkable feature is the with the Clintn climate; the first is qualitatively representative f all cases with sandy lam r silt lam sils, while the secnd is representative f all cases with clay lam r clay sils. small sensitivity t climate in cmparisn with the larger sensitivity t sil type. This is apparently explained by the fact that sil parameters such as permeability vary ver a wider range than the climatic parameters such as precipitatin and ptential evapratin. Figure 3 shws the majr water balance cmpnents fr each sil-climate cmbinatin as functins f sil variability. All pltted quantities are nrmalized by average precipitatin. As is seen in Figure 2, the effect f sil type dminates that f climate. In cntrast t Figure 2, significant sensitivity t a is visible. In general, it may be said that variability tends t equalize the magnitudes f the three cmpnents. Fr example, surface runff appears in the case f sandy lam and silt lam as a 2 grws frm 0 t 6. In cntrast, it decreases frm a very large fractin in the case f clay. Whereas nly the clay and the clay lam sils yield strm surface runff in the hmgeneus case, all inhmgeneus sils prduce it. A cnsequence f the behavir nted abve is that there is less sensitivity f the water balance t the average sil type when sil variability is cnsidered. We illustrate this mre directly by cnsidering ur clay lam sil and varying the TABLE 2. Climatic Parameters Figure 5 shws variances f s as functins f a - fr the tw cases. The relatins are rughly linear. In all cases examined, the standard deviatin f s was between 0.03 and 0.1 when 6 2 was unity. Figure 6 shws variances f the nrmalized cmpnents f the water balance as functins f a 2. In the case f the sandy lam, variances are quite small fr a 2 less than unity. This seems t be assciated with the virtual absence f surface runff in this regin; in all f ur results, flux variances are disprprtinately small when the surface runff cmpnent is very small. This suggests that much f the variability in fluxes induced by sil variance is cntrlled by strm surface runff. In the case f the clay lam sil, variances are much larger and apprach maximum values asympttically. The rder f magnitude f the maxima can be estimated by cnsidering the hypthetical case where variability f a particular flux is s great that the flux is unifrmly distributed between zer and ne. In that situatin, the variance wuld be abut This is cnsistent with Figure 6 and ther calculatins nt reprted here. Parameter Clintn Santa Paula,,, mm s-1 mtb, S mr, S mpa, mm mt, S K 1.74 x x x x 10? x x x x 10? TABLE 3. Mean Sil Parameters Clay Silt Sandy Clay Lam Lam Lam n e k(1), mm x x x x 10-7 m

5 . MILLY AND EAGLESON: EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE <S > 0.6- O,4- CLAY CLAY LOAM SILT LOAM 08 2 =6 0.2 ø'' SANDYLOAM CLINTON SANTA PAULA Fig. 2. Areal means f s as functins f %2 fr varius sils and climates. Apprximate Analysis f the Means It is difficult t infer frm applicatin f (9) the manner in which individual sil parameters affect the average water balance. Furthermre, the effects f crrelatin are nt easily discerned. In this sectin we prduce an alternative expressin fr (y) that shws the interactin f parameters explicitly, albeit nly apprximately. Assuming that sil variability is small, we develp secnd-rder apprximatins fr the mean values f the utput variables f the water balance. We expand the utput y in a Taylr series arund the mean pa- rameter set y = g( ) = g( ) + ( - )' -d g( ) ( ) Taking the expected value, and nececting terms fr which n is 3 r greater, we find (Y) = g( ) + i=t, % Qu ( 2) E 0.2 /!E[Rga ]/mpa k(i),mm 2 Fig. 4. Water balance as functin f mean In [k(1)] fr the clay lam sil with Clintn climate. r (Y) = g(p) + a 2,63-2 f r _2 f r32 f3 2 +,,0,02 f,f, 2 + 0, ] f2f3p23)] (13) + &2& in which all partial derivatives are taken at m equal t p. This equatin tells us, t a first apprximatin, that the effect f sil spatial variability f any input parameter n any utput variable is directly prprtinal bth t the variance f the parameter and t the secnd derivative f the utput with SANDY LOAM () SILT LOAM CLINTON SANTA PAULA CLINTON - SANTA PAULA I.O 0.8 C LAY LOAM I, ( c ) _ It E [ETa ]/mp A CLAY (d) 0.6 O.4 II E[Rsa ]/mpa CLINTON SANTA PAULA I 0.2 -, E[R a]/mpa I Fig. 3. Areal averagexpected water balance cmpnents as functins f a 2 fr variu sils and climates.

6 2140 MILLY AND EAGLESON' EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE s% 0.02 SANDY LOAM CLAY LOAM TABLE 4. Sensitivity f Mean Evaptranspiratin t Sil Variability 1 02 g. 1 02g 1 02g 2 0(_D22 2 0c032 Sil Type 2 &0 x 2 fx 2 f22 --' f32 Clintn Sandy lam Silt lam Clay lam Clay O.OI I I I I Santa Paula Sandy lam Silt lam Clay lam Clay Fig. 5. Variance f s as functin f a 2 fr tw sils with Clintn climate. respect t the parameter. Effects may als arise due t the interactin f tw parameters when they are crrelated with each ther Fr each Of the cmbinatins f sil and climate already discussed, and fr each f the majr utput variables, we have cmputed the terms (32g/3i3j)f f. Table 4 summarizes the results fr evaptranspiratin. These numbers are representative f results fr all ther utputs, which are therefre nt presented here. Each term in Table 4 represents the change in the mean utput resulting frm a particular term in (13) when a 0 is unity. In assessing the imprtance f a given term, it is helpful t recall that each f the utputs cnsidered is dimensinless and is cnfined t the interval [0, 1]. The relative imprtance f the different terms in (13) varies frm case t case, but sme generalizatins can be made. Let us cnsider first the terms assciated directly with the variances f the three parameters. Fr the cases in which n sur c O.lO SANDY LOAM E [ETA ]/mpa _ E [RsAi/mpA [] E i i I CLAY LOAM OOA A I ( 2 I i 4 i I. 6 Fig. 6. Variances f nrmalized water balance fluxes as functins f a 2 fr tw sils with Clintn climate. - A A Sil Type &x 0092 fzf2 Owz flf Clintn Sandy lam Silt lam Clay lam Clay Santa Paula Sandy lam Silt lam Clay lam Clay Nte {fx, r 2, c03} = {ne, In [k(1)], In (m)}. face runff is generated in the hmgeneus situatin, the effect f spatial variability f any f these parameters is minimal. This is cnsistent with ur earlier bservatin that strm surface runff is an imprtant surce f variability. Fr the sils f finer texture, variability f m is mst effective in changing the utputs, and variability f k(1) als has a significant effect. The effect f variability f ti e is negligible. The imprtance f the terms that cntain the crss derivatives will depend n the magnitude f the crrelatin between parameters, but generally appears t be minimal. The table entries represent the maximal effect, which ccurs when tw parameters are perfectly crrelated. In any case, the tie- k(1) term is cnsistently small. The tie- m term is generally smewhat larger, yielding abslute changes f the utputs ptentially (fr IP 31-1) as high as 3% fr the situatins in which surface runff ccurs. The,largest crss-derivative term is the m - k(1) term. The apprximatin implied by (12) crrespnds t straight lines that are tangent t the curves in Figure 3 at zer variance; this crrespndence was verified numerically in the curse f ur wrk as a check n the cnsistency f the calculatins. The range f validity f the apprximatin (12) is nt, hwever, readily apparent frm Figure 3 fr all cases, since the plts d nt reslve sme f the changes in slpe fr small variance. In summary, this apprximate analysis suggests that sil spatial variability has a significant effect n the areal average water balance nly fr cases in which surface runff is generated. In thse cases, the utput is mst strngly affected by variability f m, next by that f k(1), and nly slightly by variability f tie' Crss-crrelatin f parameters is unimpr- tant.

7 MILLY AND EAGLESON' EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE 2141 Apprximate Analysis f the Variances As in the case f the mean, we may use (11) t derive an apprximate result fr the variance that ffers insights absent frm the Mnte Carl apprach. Fr sufficiently small values f a 2 we find r i= = 3 &øi & Qu (14) by gk( ), then the requirement fr equivalence is <yk> = gt,( e) k = 1, 2,.'-, K (17) If e satisfies (17), then we may say that is an equivalent parameter set with respect t the K utputs. Several questins naturally arise cncerning the existence and uniqueness f, as well as its functinal dependence n f( ) and ther parameters. These questins are mst directly addressed by viewing (17) as a system f equatins defining %. Direct, exact slutin f (17) fr any useful set f gn des nt appear feasible, given the cmplex nature f the equatins. In this sectin we cnsider nly an apprximate case, the case where a 0 is small. We apprximate the left side f (17) using (12), and represent the right side f (17) using (11), in bth cases replacing g by gn, 1 c32g Q0 = g,(p) = j= in which the partial derivatives are evaluated at equal t It. We see, t a first apprximatin, that the variance f any water balance utput variable is directly prprtinal t a0 e. = k = 1, 2,..., K (18) We emplyed (15) t estimate the relative cntributins f each f the three sil parameters t variance f water balance Fr a sufficiently small, will be clse enugh t It that we cmpnents. The findings parallel the bservatins made in may drp all but the leading term in the infinite sum. This discussin f Table 4. In brief, variance f In (m) cntributes yields a new system f equatins fr e the mst t utput variance, and variance f In [k(1)] cntributes the bulk f the remainder. 1 02g, Qij The range f validity f (15) is variable; departures frm i=1 j=l prprtinality in the relatin between a0 e and ay e are indica- tive f failure f (15). Referring t Figure 6, we see that the apprximatin is nt bad fr the balance cmpnents in the case f sandy lam when a02 is less than unity, mainly be- Ocøic% (O,)e It). g (19) k= 1,2,...,K where derivatives are evaluated using the mean sil. This is a set f K linear equatins fr the three unknwn cmpnents cause there is n surface runff and hence n variability f f ) e. In the case where K is 3 and the matrix Og/3 is fluxes. Hwever, in the case f clay lam, the range f validity nnsingular, there exists a uniquequivalent sil parameter vectr is much smaller. Fr the variance f s, the situatin is similar. Fr sandy lam, (15) is accurate up t a e near 2, as can be me -- It -[- Qij (20) seen in Figure 5. Less apparent in Figure 5 is the inadequacy f (15) fr the clay lam' the slpe is quite small at the rigin, but increases several times ver near the rigin. ON THE EXISTENCE OF AN EQUIVALENT HOMOGENEOUS SOIL TYPE We have shwn that the areal average water balance depends n spatial variability f sil parameters. In applicatins f the water balance mdel, hwever, it is usually desirable t wrk with a single hmgeneusil type. In such a situatin, it is ften argued that the single ne-dimensinal clumn may capture the essential dynamics and that the sil type used is an "effective" sil type, functinally dependent upn the distributin f actual sil types within the mdeled area. In this sectin we prpse a precise definitin f an equivalent hm- geneus sil and explre the cnditins fr its existence in the case f lw sil variance. The general idea f an equivalent hmgeneus sil is that it shuld yield the same respnse as the spatially variable ensemble f sils. If we take the measure f respnse t be the areally averaged utput y, then we require that the equivalent sil type have sil parameters.} e satisfying (16) Typically, we are cncerned with a set f K utputs yn (k - 1, 2,..-, K). If the crrespnding utput functins are dented If / is singular r if K is 1 r 2 then there is an infinite set f equivalent parameter sets. If K is reater than 3 and t ere is n redundancy in (l ), then there can be n equivalent param- eter set. The value f K equal t 3 seems t be especially relevant here. Of the three nrmalized water balance fluxes (evaptranspiratin, surface runff, grundwater recharge), nly tw f them yield independent cnditins n e since their sum is precipitatin, which is independent f. A third independent utput is the mean sil misture saturatin. Equatin (20) can therefre be used, fr a 0 small, t cnstruct the equivalent hmgeneus sil with respect t the three water balance fluxes and the mean sil misture saturatin. We nte that the equivalent sil depends nt nly n the density functin fr the sil parameters, but als n the climate parameters. SUMMARY AND CONCLUSIONS Our study explres sme effects f sil spatial variability n annual average water balance. We use idealized dynamic mdel, and ur findings shuld be interpreted in light f the simplifying assumptins made. The mst imprtant f these are the fllwing. 1. The spatially variable land area behaves as a battery f parallel hmgeneus sil clumns withut dynamic interac-

8 2142 MILLY AND EAGLESON' EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE tin. Excess infiltratin capacity at ne lcatin cannt cm- M vegetal canpy density. pensate fr a deficiency elsewhere. m pre size distributin index f sil. 2. The spatial variability f climate is negligible within the mpa mean annual precipitatin. mdeled area. 3. The annual average water balance at a pint in th e area mtb mean time between strms. mr, mean strm duratin. is described by the mdel f Eaglesn [1978a, b, c, d, e, f, g], m, mean duratin f wet seasn. the majr assumptins f which are summarized by Eaglesn N number f samples in Mnte Carl cmputatins. [1978a]. n e effective prsity f sil. 4. The vegetal equilibrium hypthesis f Eaglesn [1978f] Q Cvariance f t. applies. 5. The effective prsity, the lgarithm f permeability, Rg A annual recharge t grundwater. RsA annual surface runff. and the lgarithm f the pre size distributin irldex f the s time average sil misture saturatin. sil fllw a jint nrmal distributin. 'a mean annual temperature. 6. The water table is deep, the surface retentin capacity is x lcatin vectr in A. negligible, and the ptential transpiratin efficiency is unity. Keeping in mind these limitatins f the study, we have the fllwing cnclusins. y a set f water balance variables. y any water balance variable. yk kth cmpnent f y. 1. The areal mean f the time average sil misture s is Z depth t water table. insensitive i the variance f the sil hydraulic parameters, parameter f gamma distributin f strm depth. despite its strng dependence n the mean sil parameters. is mean f t. 2. The average divisin f precipitatin amng surface Pij crss crrelatin f ci and runff, grundwater recharge, and evhptranspiratin may be a standard deviatin f In [k(1)]. significantly affected by the variance f sil prperties. The a standard deviatin f significance f the effect depends upn the mean sil parame- as standardeviatin f s. ters. Sils f high average permeability exhibit a slight in- ay standardeviatin f y. crease in surface runff due t sil variance, while thse f lw fl set f all t values fund in A. average permeability exhibit decreased surface runff and in- t sil parameter vectr {tie, In [k(1)], In (m)}. creasedrainage t grundwater. As a general rule, increased t ith sample value f t used in Mnte Carl runs. variance f sil type tends t equalize the magnitudes f the c ith cmpnent f t. three majr water balance cmpnents. ( ) areal average n A. 3. A crllary f 2 is that the sensitivity f the water bal- El- ] expected value at a pint in A. ance t the mean sil prperties is markedly reduced by the presence f spatial variability. Acknwledgments. This wrk was supprted by the Natinal Science Fundatin under grants ATM , ATM , and 4. When the sil hydraulic prperties are parameterized in CEE terms f effective prsity, permeability, and pre size distributin index, variability f the first has a negligibleffect n the average water balance relative t variability f the ther tw. REFERENCES Ahuja, L. R., J. W. Naney, and D. R. Nielsen, Scaling sil water prperties and infiltratin mdeling, Sil $ci. $c. Am. J., 48(5), 5. The significant effect f the pre size distributin index , n the means and variances suggests that departures frm Andersn, S. H., and D. K. Cassel, Statistical and autregressive analysis f sil physical prperties f Prtsmuth sandy lam, Sil micrscpic similarity in the sil are imprtant. $ci. $c. Am. J., 50(5), , , The bulk f the variance f water balance variables is Brakensiek, D. L., R. L. Engleman, and W. J. RawIs, Variatin within explained by variance f permeability and pre size distri- texture classes f sil water prperties, Trans. Am. $c. Agric. Eng., butin index. 24(2), , Bresler, E., G. Dagan, R. J. Wagenet, and A. Laufer, Statistical analy- 7. Fr sufficiently small variance f the sil parameters, sis f salinity and texture effects n spatial variability f sil hythere exists a unique equivalent hmgeneus sil type that draulic cnductivity, Sil $ci. $c. Am. J., 48(1), 16-25, yields the same mean sil misture saturatin and the same Brks, R. H., and A. T. Crey, Hydraulic prperties f prus mean water balance cmpnents as an inhmgeneus sil. media, Hydrl. Pap. 3, Cl. State Univ., Frt Cllins, Byers, E., and D. B. Stephens, Statistical and stchastic analyses f NOTATION hydrauli cnductivity and particle-size in a fluvial sand, Sil Sci. A mdeled area. $c. Am. J., 47(6), , Cassel, D. K., Spatial and tempral variability f sil physical prper- ErA annual evaptranspiratin. ties fllwing tillage f Nrflk lamy sand, Sil $ci. $c. Am. J., 47(2), , average rate f ptential evapratin. Clapp, R. B., and G. M. Hrnberger, Empirical equatins lbr sme f( ) jint density f t. sil hydraulic prperties, Water Resur. Res., 14(4), , f/ rati f ai t a. Celh, M. A., Spatial variability f water related sil physical g( ) functin transfrming t t y. prperties, Ph.D. dissertatin, Dep. f Sils, Water, and Eng., Univ. g( ) functin transfrming t t y. f Ariz., Tucsn, Eaglesn, P.S., Climate, sil, and vegetatin, 1, Intrductin t water gk( ) functin transfrming t t Ykbalance dynamics, Water Resur. Res., 14(5), , 1978a. h sil surface retentin capacity. Eaglesn, P.S., Climate, sil, and vegetatin, 2, The distributin f K number f elements in y. annual precipitatin derived frm bserved strm sequences, Water k(1) sil permeability. Resur. Res., 14(5), , 1978b. k v ptential transpiratin efficiency. Eaglesn, P.S., Climate, sil, and vegetatin, 3, A simplified mdel f

9 MILLY AND EAGLESON: EFFECTS OF SPATIAL VARIABILITY ON ANNUAL AVERAGE WATER BALANCE 2143 sil misture mvement in the liquid phase, Water Resur. Res., water prperties, Trans. Am. Sc. Agric. Eng., 25(2), , 14(5), , 1978c Eaglesn, P.S., Climate, sil, and vegetatin, 4, The expected value f Sharma, M. L., and R. J. Luxmre, Sil spatial variability and its annual evaptranspiratin, Water Resur. Res., 14(5), , cnsequences n simulated water balance, Water Resur. Res., 1978d. 15(6), , Eaglesn, P.S., Climate, sil, and vegetatin, 5, A derived distributin Warrick, A. W., and D. R. Nielsen, Spatial variability f sil physical f strm surface runff, Water Resur. Res., 14(5), , 1978e. prperties in the field, edited by D. Hillel, in Applicatins f Sil Eaglesn, P.S., Climate, sil, and vegetatin, 6, Dynamics f the Physics, Academic, Orland, Fla., annual water balance, Water Resur. Res., 14(5), , 1978f Eaglesn, P.S., Climate, sil, and vegetatin, 7, A derived distributin P.S. Eaglesn, Department f Civil Engineering, Massachusetts f annual water yield, Water Resur. Res., 14(5), , 1978g. Institute f Technlgy, Cambridge, MA Nielsen, D. R., J. W. Biggar, and K. T. Erh, Spatial variability f P. C. D. Milly, Water Resurces Prgram, Department f Civil field-measured sil-water prperties, Hilgardia, 42(7), , Engineering, Princetn University, Princetn, NJ Peck, A. J., R. J. Luxmre, and J. L. Stlzy, Effects f spatial variability f sil hydraulic prperties in water budget mdeling, Water Resur. Res., 3(2), , Rawls, W. J., D. L. Brakensiek, and K. E. Saxtn, Estimatin f sil (Received May 1, 1987; revised August 3, 1987; accepted August 4, 1987.)

, which yields. where z1. and z2

, which yields. where z1. and z2 The Gaussian r Nrmal PDF, Page 1 The Gaussian r Nrmal Prbability Density Functin Authr: Jhn M Cimbala, Penn State University Latest revisin: 11 September 13 The Gaussian r Nrmal Prbability Density Functin

More information

Module 4: General Formulation of Electric Circuit Theory

Module 4: General Formulation of Electric Circuit Theory Mdule 4: General Frmulatin f Electric Circuit Thery 4. General Frmulatin f Electric Circuit Thery All electrmagnetic phenmena are described at a fundamental level by Maxwell's equatins and the assciated

More information

ENSC Discrete Time Systems. Project Outline. Semester

ENSC Discrete Time Systems. Project Outline. Semester ENSC 49 - iscrete Time Systems Prject Outline Semester 006-1. Objectives The gal f the prject is t design a channel fading simulatr. Upn successful cmpletin f the prject, yu will reinfrce yur understanding

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 4: Mdel checing fr ODE mdels In Petre Department f IT, Åb Aademi http://www.users.ab.fi/ipetre/cmpmd/ Cntent Stichimetric matrix Calculating the mass cnservatin relatins

More information

(1.1) V which contains charges. If a charge density ρ, is defined as the limit of the ratio of the charge contained. 0, and if a force density f

(1.1) V which contains charges. If a charge density ρ, is defined as the limit of the ratio of the charge contained. 0, and if a force density f 1.0 Review f Electrmagnetic Field Thery Selected aspects f electrmagnetic thery are reviewed in this sectin, with emphasis n cncepts which are useful in understanding magnet design. Detailed, rigrus treatments

More information

FIELD QUALITY IN ACCELERATOR MAGNETS

FIELD QUALITY IN ACCELERATOR MAGNETS FIELD QUALITY IN ACCELERATOR MAGNETS S. Russenschuck CERN, 1211 Geneva 23, Switzerland Abstract The field quality in the supercnducting magnets is expressed in terms f the cefficients f the Furier series

More information

Bootstrap Method > # Purpose: understand how bootstrap method works > obs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(obs) >

Bootstrap Method > # Purpose: understand how bootstrap method works > obs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(obs) > Btstrap Methd > # Purpse: understand hw btstrap methd wrks > bs=c(11.96, 5.03, 67.40, 16.07, 31.50, 7.73, 11.10, 22.38) > n=length(bs) > mean(bs) [1] 21.64625 > # estimate f lambda > lambda = 1/mean(bs);

More information

Distributions, spatial statistics and a Bayesian perspective

Distributions, spatial statistics and a Bayesian perspective Distributins, spatial statistics and a Bayesian perspective Dug Nychka Natinal Center fr Atmspheric Research Distributins and densities Cnditinal distributins and Bayes Thm Bivariate nrmal Spatial statistics

More information

Lecture 17: Free Energy of Multi-phase Solutions at Equilibrium

Lecture 17: Free Energy of Multi-phase Solutions at Equilibrium Lecture 17: 11.07.05 Free Energy f Multi-phase Slutins at Equilibrium Tday: LAST TIME...2 FREE ENERGY DIAGRAMS OF MULTI-PHASE SOLUTIONS 1...3 The cmmn tangent cnstructin and the lever rule...3 Practical

More information

Study Group Report: Plate-fin Heat Exchangers: AEA Technology

Study Group Report: Plate-fin Heat Exchangers: AEA Technology Study Grup Reprt: Plate-fin Heat Exchangers: AEA Technlgy The prblem under study cncerned the apparent discrepancy between a series f experiments using a plate fin heat exchanger and the classical thery

More information

Math Foundations 20 Work Plan

Math Foundations 20 Work Plan Math Fundatins 20 Wrk Plan Units / Tpics 20.8 Demnstrate understanding f systems f linear inequalities in tw variables. Time Frame December 1-3 weeks 6-10 Majr Learning Indicatrs Identify situatins relevant

More information

A Matrix Representation of Panel Data

A Matrix Representation of Panel Data web Extensin 6 Appendix 6.A A Matrix Representatin f Panel Data Panel data mdels cme in tw brad varieties, distinct intercept DGPs and errr cmpnent DGPs. his appendix presents matrix algebra representatins

More information

Kinetic Model Completeness

Kinetic Model Completeness 5.68J/10.652J Spring 2003 Lecture Ntes Tuesday April 15, 2003 Kinetic Mdel Cmpleteness We say a chemical kinetic mdel is cmplete fr a particular reactin cnditin when it cntains all the species and reactins

More information

22.54 Neutron Interactions and Applications (Spring 2004) Chapter 11 (3/11/04) Neutron Diffusion

22.54 Neutron Interactions and Applications (Spring 2004) Chapter 11 (3/11/04) Neutron Diffusion .54 Neutrn Interactins and Applicatins (Spring 004) Chapter (3//04) Neutrn Diffusin References -- J. R. Lamarsh, Intrductin t Nuclear Reactr Thery (Addisn-Wesley, Reading, 966) T study neutrn diffusin

More information

1 The limitations of Hartree Fock approximation

1 The limitations of Hartree Fock approximation Chapter: Pst-Hartree Fck Methds - I The limitatins f Hartree Fck apprximatin The n electrn single determinant Hartree Fck wave functin is the variatinal best amng all pssible n electrn single determinants

More information

February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA

February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA February 28, 2013 COMMENTS ON DIFFUSION, DIFFUSIVITY AND DERIVATION OF HYPERBOLIC EQUATIONS DESCRIBING THE DIFFUSION PHENOMENA Mental Experiment regarding 1D randm walk Cnsider a cntainer f gas in thermal

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 2: Mdeling change. In Petre Department f IT, Åb Akademi http://users.ab.fi/ipetre/cmpmd/ Cntent f the lecture Basic paradigm f mdeling change Examples Linear dynamical

More information

7 TH GRADE MATH STANDARDS

7 TH GRADE MATH STANDARDS ALGEBRA STANDARDS Gal 1: Students will use the language f algebra t explre, describe, represent, and analyze number expressins and relatins 7 TH GRADE MATH STANDARDS 7.M.1.1: (Cmprehensin) Select, use,

More information

[COLLEGE ALGEBRA EXAM I REVIEW TOPICS] ( u s e t h i s t o m a k e s u r e y o u a r e r e a d y )

[COLLEGE ALGEBRA EXAM I REVIEW TOPICS] ( u s e t h i s t o m a k e s u r e y o u a r e r e a d y ) (Abut the final) [COLLEGE ALGEBRA EXAM I REVIEW TOPICS] ( u s e t h i s t m a k e s u r e y u a r e r e a d y ) The department writes the final exam s I dn't really knw what's n it and I can't very well

More information

SAMPLING DYNAMICAL SYSTEMS

SAMPLING DYNAMICAL SYSTEMS SAMPLING DYNAMICAL SYSTEMS Melvin J. Hinich Applied Research Labratries The University f Texas at Austin Austin, TX 78713-8029, USA (512) 835-3278 (Vice) 835-3259 (Fax) hinich@mail.la.utexas.edu ABSTRACT

More information

Determining the Accuracy of Modal Parameter Estimation Methods

Determining the Accuracy of Modal Parameter Estimation Methods Determining the Accuracy f Mdal Parameter Estimatin Methds by Michael Lee Ph.D., P.E. & Mar Richardsn Ph.D. Structural Measurement Systems Milpitas, CA Abstract The mst cmmn type f mdal testing system

More information

Numerical Simulation of the Thermal Resposne Test Within the Comsol Multiphysics Environment

Numerical Simulation of the Thermal Resposne Test Within the Comsol Multiphysics Environment Presented at the COMSOL Cnference 2008 Hannver University f Parma Department f Industrial Engineering Numerical Simulatin f the Thermal Respsne Test Within the Cmsl Multiphysics Envirnment Authr : C. Crradi,

More information

Computational modeling techniques

Computational modeling techniques Cmputatinal mdeling techniques Lecture 11: Mdeling with systems f ODEs In Petre Department f IT, Ab Akademi http://www.users.ab.fi/ipetre/cmpmd/ Mdeling with differential equatins Mdeling strategy Fcus

More information

Comparison of two variable parameter Muskingum methods

Comparison of two variable parameter Muskingum methods Extreme Hydrlgical Events: Precipitatin, Flds and Drughts (Prceedings f the Ykhama Sympsium, July 1993). IAHS Publ. n. 213, 1993. 129 Cmparisn f tw variable parameter Muskingum methds M. PERUMAL Department

More information

Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax

Revision: August 19, E Main Suite D Pullman, WA (509) Voice and Fax .7.4: Direct frequency dmain circuit analysis Revisin: August 9, 00 5 E Main Suite D Pullman, WA 9963 (509) 334 6306 ice and Fax Overview n chapter.7., we determined the steadystate respnse f electrical

More information

We can see from the graph above that the intersection is, i.e., [ ).

We can see from the graph above that the intersection is, i.e., [ ). MTH 111 Cllege Algebra Lecture Ntes July 2, 2014 Functin Arithmetic: With nt t much difficulty, we ntice that inputs f functins are numbers, and utputs f functins are numbers. S whatever we can d with

More information

ROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS

ROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS Particle Acceleratrs, 1986, Vl. 19, pp. 99-105 0031-2460/86/1904-0099/$15.00/0 1986 Grdn and Breach, Science Publishers, S.A. Printed in the United States f America ROUNDING ERRORS IN BEAM-TRACKING CALCULATIONS

More information

CAUSAL INFERENCE. Technical Track Session I. Phillippe Leite. The World Bank

CAUSAL INFERENCE. Technical Track Session I. Phillippe Leite. The World Bank CAUSAL INFERENCE Technical Track Sessin I Phillippe Leite The Wrld Bank These slides were develped by Christel Vermeersch and mdified by Phillippe Leite fr the purpse f this wrkshp Plicy questins are causal

More information

A mathematical model for complete stress-strain curve prediction of permeable concrete

A mathematical model for complete stress-strain curve prediction of permeable concrete A mathematical mdel fr cmplete stress-strain curve predictin f permeable cncrete M. K. Hussin Y. Zhuge F. Bullen W. P. Lkuge Faculty f Engineering and Surveying, University f Suthern Queensland, Twmba,

More information

NAME TEMPERATURE AND HUMIDITY. I. Introduction

NAME TEMPERATURE AND HUMIDITY. I. Introduction NAME TEMPERATURE AND HUMIDITY I. Intrductin Temperature is the single mst imprtant factr in determining atmspheric cnditins because it greatly influences: 1. The amunt f water vapr in the air 2. The pssibility

More information

MATHEMATICS SYLLABUS SECONDARY 5th YEAR

MATHEMATICS SYLLABUS SECONDARY 5th YEAR Eurpean Schls Office f the Secretary-General Pedaggical Develpment Unit Ref. : 011-01-D-8-en- Orig. : EN MATHEMATICS SYLLABUS SECONDARY 5th YEAR 6 perid/week curse APPROVED BY THE JOINT TEACHING COMMITTEE

More information

Methods for Determination of Mean Speckle Size in Simulated Speckle Pattern

Methods for Determination of Mean Speckle Size in Simulated Speckle Pattern 0.478/msr-04-004 MEASUREMENT SCENCE REVEW, Vlume 4, N. 3, 04 Methds fr Determinatin f Mean Speckle Size in Simulated Speckle Pattern. Hamarvá, P. Šmíd, P. Hrváth, M. Hrabvský nstitute f Physics f the Academy

More information

Verification of Quality Parameters of a Solar Panel and Modification in Formulae of its Series Resistance

Verification of Quality Parameters of a Solar Panel and Modification in Formulae of its Series Resistance Verificatin f Quality Parameters f a Slar Panel and Mdificatin in Frmulae f its Series Resistance Sanika Gawhane Pune-411037-India Onkar Hule Pune-411037- India Chinmy Kulkarni Pune-411037-India Ojas Pandav

More information

On Huntsberger Type Shrinkage Estimator for the Mean of Normal Distribution ABSTRACT INTRODUCTION

On Huntsberger Type Shrinkage Estimator for the Mean of Normal Distribution ABSTRACT INTRODUCTION Malaysian Jurnal f Mathematical Sciences 4(): 7-4 () On Huntsberger Type Shrinkage Estimatr fr the Mean f Nrmal Distributin Department f Mathematical and Physical Sciences, University f Nizwa, Sultanate

More information

Technical Bulletin. Generation Interconnection Procedures. Revisions to Cluster 4, Phase 1 Study Methodology

Technical Bulletin. Generation Interconnection Procedures. Revisions to Cluster 4, Phase 1 Study Methodology Technical Bulletin Generatin Intercnnectin Prcedures Revisins t Cluster 4, Phase 1 Study Methdlgy Release Date: Octber 20, 2011 (Finalizatin f the Draft Technical Bulletin released n September 19, 2011)

More information

Perfrmance f Sensitizing Rules n Shewhart Cntrl Charts with Autcrrelated Data Key Wrds: Autregressive, Mving Average, Runs Tests, Shewhart Cntrl Chart

Perfrmance f Sensitizing Rules n Shewhart Cntrl Charts with Autcrrelated Data Key Wrds: Autregressive, Mving Average, Runs Tests, Shewhart Cntrl Chart Perfrmance f Sensitizing Rules n Shewhart Cntrl Charts with Autcrrelated Data Sandy D. Balkin Dennis K. J. Lin y Pennsylvania State University, University Park, PA 16802 Sandy Balkin is a graduate student

More information

Lead/Lag Compensator Frequency Domain Properties and Design Methods

Lead/Lag Compensator Frequency Domain Properties and Design Methods Lectures 6 and 7 Lead/Lag Cmpensatr Frequency Dmain Prperties and Design Methds Definitin Cnsider the cmpensatr (ie cntrller Fr, it is called a lag cmpensatr s K Fr s, it is called a lead cmpensatr Ntatin

More information

CHAPTER 4 DIAGNOSTICS FOR INFLUENTIAL OBSERVATIONS

CHAPTER 4 DIAGNOSTICS FOR INFLUENTIAL OBSERVATIONS CHAPTER 4 DIAGNOSTICS FOR INFLUENTIAL OBSERVATIONS 1 Influential bservatins are bservatins whse presence in the data can have a distrting effect n the parameter estimates and pssibly the entire analysis,

More information

Emphases in Common Core Standards for Mathematical Content Kindergarten High School

Emphases in Common Core Standards for Mathematical Content Kindergarten High School Emphases in Cmmn Cre Standards fr Mathematical Cntent Kindergarten High Schl Cntent Emphases by Cluster March 12, 2012 Describes cntent emphases in the standards at the cluster level fr each grade. These

More information

Surface and Contact Stress

Surface and Contact Stress Surface and Cntact Stress The cncept f the frce is fundamental t mechanics and many imprtant prblems can be cast in terms f frces nly, fr example the prblems cnsidered in Chapter. Hwever, mre sphisticated

More information

OF SIMPLY SUPPORTED PLYWOOD PLATES UNDER COMBINED EDGEWISE BENDING AND COMPRESSION

OF SIMPLY SUPPORTED PLYWOOD PLATES UNDER COMBINED EDGEWISE BENDING AND COMPRESSION U. S. FOREST SERVICE RESEARCH PAPER FPL 50 DECEMBER U. S. DEPARTMENT OF AGRICULTURE FOREST SERVICE FOREST PRODUCTS LABORATORY OF SIMPLY SUPPORTED PLYWOOD PLATES UNDER COMBINED EDGEWISE BENDING AND COMPRESSION

More information

CHAPTER 24: INFERENCE IN REGRESSION. Chapter 24: Make inferences about the population from which the sample data came.

CHAPTER 24: INFERENCE IN REGRESSION. Chapter 24: Make inferences about the population from which the sample data came. MATH 1342 Ch. 24 April 25 and 27, 2013 Page 1 f 5 CHAPTER 24: INFERENCE IN REGRESSION Chapters 4 and 5: Relatinships between tw quantitative variables. Be able t Make a graph (scatterplt) Summarize the

More information

Thermodynamics Partial Outline of Topics

Thermodynamics Partial Outline of Topics Thermdynamics Partial Outline f Tpics I. The secnd law f thermdynamics addresses the issue f spntaneity and invlves a functin called entrpy (S): If a prcess is spntaneus, then Suniverse > 0 (2 nd Law!)

More information

AP Statistics Notes Unit Two: The Normal Distributions

AP Statistics Notes Unit Two: The Normal Distributions AP Statistics Ntes Unit Tw: The Nrmal Distributins Syllabus Objectives: 1.5 The student will summarize distributins f data measuring the psitin using quartiles, percentiles, and standardized scres (z-scres).

More information

CS 477/677 Analysis of Algorithms Fall 2007 Dr. George Bebis Course Project Due Date: 11/29/2007

CS 477/677 Analysis of Algorithms Fall 2007 Dr. George Bebis Course Project Due Date: 11/29/2007 CS 477/677 Analysis f Algrithms Fall 2007 Dr. Gerge Bebis Curse Prject Due Date: 11/29/2007 Part1: Cmparisn f Srting Algrithms (70% f the prject grade) The bjective f the first part f the assignment is

More information

Electric Current and Resistance

Electric Current and Resistance Electric Current and Resistance Electric Current Electric current is the rate f flw f charge thrugh sme regin f space The SI unit f current is the ampere (A) 1 A = 1 C / s The symbl fr electric current

More information

Modeling the Nonlinear Rheological Behavior of Materials with a Hyper-Exponential Type Function

Modeling the Nonlinear Rheological Behavior of Materials with a Hyper-Exponential Type Function www.ccsenet.rg/mer Mechanical Engineering Research Vl. 1, N. 1; December 011 Mdeling the Nnlinear Rhelgical Behavir f Materials with a Hyper-Expnential Type Functin Marc Delphin Mnsia Département de Physique,

More information

Modelling of Clock Behaviour. Don Percival. Applied Physics Laboratory University of Washington Seattle, Washington, USA

Modelling of Clock Behaviour. Don Percival. Applied Physics Laboratory University of Washington Seattle, Washington, USA Mdelling f Clck Behaviur Dn Percival Applied Physics Labratry University f Washingtn Seattle, Washingtn, USA verheads and paper fr talk available at http://faculty.washingtn.edu/dbp/talks.html 1 Overview

More information

3. Mass Transfer with Chemical Reaction

3. Mass Transfer with Chemical Reaction 8 3. Mass Transfer with Chemical Reactin 3. Mass Transfer with Chemical Reactin In the fllwing, the fundamentals f desrptin with chemical reactin, which are applied t the prblem f CO 2 desrptin in ME distillers,

More information

General Chemistry II, Unit I: Study Guide (part I)

General Chemistry II, Unit I: Study Guide (part I) 1 General Chemistry II, Unit I: Study Guide (part I) CDS Chapter 14: Physical Prperties f Gases Observatin 1: Pressure- Vlume Measurements n Gases The spring f air is measured as pressure, defined as the

More information

Lecture 23: Lattice Models of Materials; Modeling Polymer Solutions

Lecture 23: Lattice Models of Materials; Modeling Polymer Solutions Lecture 23: 12.05.05 Lattice Mdels f Materials; Mdeling Plymer Slutins Tday: LAST TIME...2 The Bltzmann Factr and Partitin Functin: systems at cnstant temperature...2 A better mdel: The Debye slid...3

More information

Resampling Methods. Chapter 5. Chapter 5 1 / 52

Resampling Methods. Chapter 5. Chapter 5 1 / 52 Resampling Methds Chapter 5 Chapter 5 1 / 52 1 51 Validatin set apprach 2 52 Crss validatin 3 53 Btstrap Chapter 5 2 / 52 Abut Resampling An imprtant statistical tl Pretending the data as ppulatin and

More information

I. Analytical Potential and Field of a Uniform Rod. V E d. The definition of electric potential difference is

I. Analytical Potential and Field of a Uniform Rod. V E d. The definition of electric potential difference is Length L>>a,b,c Phys 232 Lab 4 Ch 17 Electric Ptential Difference Materials: whitebards & pens, cmputers with VPythn, pwer supply & cables, multimeter, crkbard, thumbtacks, individual prbes and jined prbes,

More information

Internal vs. external validity. External validity. This section is based on Stock and Watson s Chapter 9.

Internal vs. external validity. External validity. This section is based on Stock and Watson s Chapter 9. Sectin 7 Mdel Assessment This sectin is based n Stck and Watsn s Chapter 9. Internal vs. external validity Internal validity refers t whether the analysis is valid fr the ppulatin and sample being studied.

More information

3. Design of Channels General Definition of some terms CHAPTER THREE

3. Design of Channels General Definition of some terms CHAPTER THREE CHAPTER THREE. Design f Channels.. General The success f the irrigatin system depends n the design f the netwrk f canals. The canals may be excavated thrugh the difference types f sils such as alluvial

More information

3.4 Shrinkage Methods Prostate Cancer Data Example (Continued) Ridge Regression

3.4 Shrinkage Methods Prostate Cancer Data Example (Continued) Ridge Regression 3.3.4 Prstate Cancer Data Example (Cntinued) 3.4 Shrinkage Methds 61 Table 3.3 shws the cefficients frm a number f different selectin and shrinkage methds. They are best-subset selectin using an all-subsets

More information

CHAPTER 3 INEQUALITIES. Copyright -The Institute of Chartered Accountants of India

CHAPTER 3 INEQUALITIES. Copyright -The Institute of Chartered Accountants of India CHAPTER 3 INEQUALITIES Cpyright -The Institute f Chartered Accuntants f India INEQUALITIES LEARNING OBJECTIVES One f the widely used decisin making prblems, nwadays, is t decide n the ptimal mix f scarce

More information

Thermodynamics and Equilibrium

Thermodynamics and Equilibrium Thermdynamics and Equilibrium Thermdynamics Thermdynamics is the study f the relatinship between heat and ther frms f energy in a chemical r physical prcess. We intrduced the thermdynamic prperty f enthalpy,

More information

Drought damaged area

Drought damaged area ESTIMATE OF THE AMOUNT OF GRAVEL CO~TENT IN THE SOIL BY A I R B O'RN EMS S D A T A Y. GOMI, H. YAMAMOTO, AND S. SATO ASIA AIR SURVEY CO., l d. KANAGAWA,JAPAN S.ISHIGURO HOKKAIDO TOKACHI UBPREFECTRAl OffICE

More information

Analysis of Curved Bridges Crossing Fault Rupture Zones

Analysis of Curved Bridges Crossing Fault Rupture Zones Analysis f Curved Bridges Crssing Fault Rupture Znes R.K.Gel, B.Qu & O.Rdriguez Dept. f Civil and Envirnmental Engineering, Califrnia Plytechnic State University, San Luis Obisp, CA 93407, USA SUMMARY:

More information

David HORN and Irit OPHER. School of Physics and Astronomy. Raymond and Beverly Sackler Faculty of Exact Sciences

David HORN and Irit OPHER. School of Physics and Astronomy. Raymond and Beverly Sackler Faculty of Exact Sciences Cmplex Dynamics f Neurnal Threshlds David HORN and Irit OPHER Schl f Physics and Astrnmy Raymnd and Beverly Sackler Faculty f Exact Sciences Tel Aviv University, Tel Aviv 69978, Israel hrn@neurn.tau.ac.il

More information

EXPERIMENTAL STUDY ON DISCHARGE COEFFICIENT OF OUTFLOW OPENING FOR PREDICTING CROSS-VENTILATION FLOW RATE

EXPERIMENTAL STUDY ON DISCHARGE COEFFICIENT OF OUTFLOW OPENING FOR PREDICTING CROSS-VENTILATION FLOW RATE EXPERIMENTAL STUD ON DISCHARGE COEFFICIENT OF OUTFLOW OPENING FOR PREDICTING CROSS-VENTILATION FLOW RATE Tmnbu Gt, Masaaki Ohba, Takashi Kurabuchi 2, Tmyuki End 3, shihik Akamine 4, and Tshihir Nnaka 2

More information

IN a recent article, Geary [1972] discussed the merit of taking first differences

IN a recent article, Geary [1972] discussed the merit of taking first differences The Efficiency f Taking First Differences in Regressin Analysis: A Nte J. A. TILLMAN IN a recent article, Geary [1972] discussed the merit f taking first differences t deal with the prblems that trends

More information

Phys. 344 Ch 7 Lecture 8 Fri., April. 10 th,

Phys. 344 Ch 7 Lecture 8 Fri., April. 10 th, Phys. 344 Ch 7 Lecture 8 Fri., April. 0 th, 009 Fri. 4/0 8. Ising Mdel f Ferrmagnets HW30 66, 74 Mn. 4/3 Review Sat. 4/8 3pm Exam 3 HW Mnday: Review fr est 3. See n-line practice test lecture-prep is t

More information

arxiv:hep-ph/ v1 2 Jun 1995

arxiv:hep-ph/ v1 2 Jun 1995 WIS-95//May-PH The rati F n /F p frm the analysis f data using a new scaling variable S. A. Gurvitz arxiv:hep-ph/95063v1 Jun 1995 Department f Particle Physics, Weizmann Institute f Science, Rehvt 76100,

More information

NGSS High School Physics Domain Model

NGSS High School Physics Domain Model NGSS High Schl Physics Dmain Mdel Mtin and Stability: Frces and Interactins HS-PS2-1: Students will be able t analyze data t supprt the claim that Newtn s secnd law f mtin describes the mathematical relatinship

More information

More Tutorial at

More Tutorial at Answer each questin in the space prvided; use back f page if extra space is needed. Answer questins s the grader can READILY understand yur wrk; nly wrk n the exam sheet will be cnsidered. Write answers,

More information

A study on GPS PDOP and its impact on position error

A study on GPS PDOP and its impact on position error IndianJurnalfRadi& SpacePhysics V1.26,April1997,pp. 107-111 A study n GPS and its impact n psitin errr P Banerjee,AnindyaBse& B SMathur TimeandFrequencySectin,NatinalPhysicalLabratry,NewDelhi110012 Received19June

More information

Pressure And Entropy Variations Across The Weak Shock Wave Due To Viscosity Effects

Pressure And Entropy Variations Across The Weak Shock Wave Due To Viscosity Effects Pressure And Entrpy Variatins Acrss The Weak Shck Wave Due T Viscsity Effects OSTAFA A. A. AHOUD Department f athematics Faculty f Science Benha University 13518 Benha EGYPT Abstract:-The nnlinear differential

More information

Engineering Approach to Modelling Metal THz Structures

Engineering Approach to Modelling Metal THz Structures Terahertz Science and Technlgy, ISSN 1941-7411 Vl.4, N.1, March 11 Invited Paper ngineering Apprach t Mdelling Metal THz Structures Stepan Lucyszyn * and Yun Zhu Department f, Imperial Cllege Lndn, xhibitin

More information

Sequential Allocation with Minimal Switching

Sequential Allocation with Minimal Switching In Cmputing Science and Statistics 28 (1996), pp. 567 572 Sequential Allcatin with Minimal Switching Quentin F. Stut 1 Janis Hardwick 1 EECS Dept., University f Michigan Statistics Dept., Purdue University

More information

Least Squares Optimal Filtering with Multirate Observations

Least Squares Optimal Filtering with Multirate Observations Prc. 36th Asilmar Cnf. n Signals, Systems, and Cmputers, Pacific Grve, CA, Nvember 2002 Least Squares Optimal Filtering with Multirate Observatins Charles W. herrien and Anthny H. Hawes Department f Electrical

More information

Aircraft Performance - Drag

Aircraft Performance - Drag Aircraft Perfrmance - Drag Classificatin f Drag Ntes: Drag Frce and Drag Cefficient Drag is the enemy f flight and its cst. One f the primary functins f aerdynamicists and aircraft designers is t reduce

More information

7.0 Heat Transfer in an External Laminar Boundary Layer

7.0 Heat Transfer in an External Laminar Boundary Layer 7.0 Heat ransfer in an Eternal Laminar Bundary Layer 7. Intrductin In this chapter, we will assume: ) hat the fluid prperties are cnstant and unaffected by temperature variatins. ) he thermal & mmentum

More information

Chapter 2 GAUSS LAW Recommended Problems:

Chapter 2 GAUSS LAW Recommended Problems: Chapter GAUSS LAW Recmmended Prblems: 1,4,5,6,7,9,11,13,15,18,19,1,7,9,31,35,37,39,41,43,45,47,49,51,55,57,61,6,69. LCTRIC FLUX lectric flux is a measure f the number f electric filed lines penetrating

More information

Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals of Diffusion

Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals of Diffusion Materials Engineering 272-C Fall 2001, Lecture 7 & 8 Fundamentals f Diffusin Diffusin: Transprt in a slid, liquid, r gas driven by a cncentratin gradient (r, in the case f mass transprt, a chemical ptential

More information

ANALYTICAL SOLUTIONS TO THE PROBLEM OF EDDY CURRENT PROBES

ANALYTICAL SOLUTIONS TO THE PROBLEM OF EDDY CURRENT PROBES ANALYTICAL SOLUTIONS TO THE PROBLEM OF EDDY CURRENT PROBES CONSISTING OF LONG PARALLEL CONDUCTORS B. de Halleux, O. Lesage, C. Mertes and A. Ptchelintsev Mechanical Engineering Department Cathlic University

More information

THE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS. Chapter 8. This work extends chapter 6 titled, "Field Mass Generation and Control", while

THE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS. Chapter 8. This work extends chapter 6 titled, Field Mass Generation and Control, while 133 THE FLUXOID QUANTUM AND ELECTROGRAVITATIONAL DYNAMICS Chapter 8 This wrk extends chapter 6 titled, "Field Mass Generatin and Cntrl", while als develping a new cnceptual apprach t mass-field vehicle

More information

AP Statistics Practice Test Unit Three Exploring Relationships Between Variables. Name Period Date

AP Statistics Practice Test Unit Three Exploring Relationships Between Variables. Name Period Date AP Statistics Practice Test Unit Three Explring Relatinships Between Variables Name Perid Date True r False: 1. Crrelatin and regressin require explanatry and respnse variables. 1. 2. Every least squares

More information

1996 Engineering Systems Design and Analysis Conference, Montpellier, France, July 1-4, 1996, Vol. 7, pp

1996 Engineering Systems Design and Analysis Conference, Montpellier, France, July 1-4, 1996, Vol. 7, pp THE POWER AND LIMIT OF NEURAL NETWORKS T. Y. Lin Department f Mathematics and Cmputer Science San Jse State University San Jse, Califrnia 959-003 tylin@cs.ssu.edu and Bereley Initiative in Sft Cmputing*

More information

z = Geometric height (m)

z = Geometric height (m) 13 Z = Geptential height (m) = Lapse rate (6.5 K km -1 ) R = Gas cnstant fr dry air (287 Jkg -1 K) g = Acceleratin f gravity (9.8 ms -2 ) TS = Surface Temperature (K) p = Initial air pressure (Assumptin:

More information

The Destabilization of Rossby Normal Modes by Meridional Baroclinic Shear

The Destabilization of Rossby Normal Modes by Meridional Baroclinic Shear The Destabilizatin f Rssby Nrmal Mdes by Meridinal Barclinic Shear by Jseph Pedlsky Wds Hle Oceangraphic Institutin Wds Hle, MA 0543 Abstract The Rssby nrmal mdes f a tw-layer fluid in a meridinal channel

More information

Coalition Formation and Data Envelopment Analysis

Coalition Formation and Data Envelopment Analysis Jurnal f CENTRU Cathedra Vlume 4, Issue 2, 20 26-223 JCC Jurnal f CENTRU Cathedra Calitin Frmatin and Data Envelpment Analysis Rlf Färe Oregn State University, Crvallis, OR, USA Shawna Grsspf Oregn State

More information

Learning to Control an Unstable System with Forward Modeling

Learning to Control an Unstable System with Forward Modeling 324 Jrdan and Jacbs Learning t Cntrl an Unstable System with Frward Mdeling Michael I. Jrdan Brain and Cgnitive Sciences MIT Cambridge, MA 02139 Rbert A. Jacbs Cmputer and Infrmatin Sciences University

More information

A New Evaluation Measure. J. Joiner and L. Werner. The problems of evaluation and the needed criteria of evaluation

A New Evaluation Measure. J. Joiner and L. Werner. The problems of evaluation and the needed criteria of evaluation III-l III. A New Evaluatin Measure J. Jiner and L. Werner Abstract The prblems f evaluatin and the needed criteria f evaluatin measures in the SMART system f infrmatin retrieval are reviewed and discussed.

More information

Admissibility Conditions and Asymptotic Behavior of Strongly Regular Graphs

Admissibility Conditions and Asymptotic Behavior of Strongly Regular Graphs Admissibility Cnditins and Asympttic Behavir f Strngly Regular Graphs VASCO MOÇO MANO Department f Mathematics University f Prt Oprt PORTUGAL vascmcman@gmailcm LUÍS ANTÓNIO DE ALMEIDA VIEIRA Department

More information

Comparing Several Means: ANOVA. Group Means and Grand Mean

Comparing Several Means: ANOVA. Group Means and Grand Mean STAT 511 ANOVA and Regressin 1 Cmparing Several Means: ANOVA Slide 1 Blue Lake snap beans were grwn in 12 pen-tp chambers which are subject t 4 treatments 3 each with O 3 and SO 2 present/absent. The ttal

More information

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics

Chapters 29 and 35 Thermochemistry and Chemical Thermodynamics Chapters 9 and 35 Thermchemistry and Chemical Thermdynamics 1 Cpyright (c) 011 by Michael A. Janusa, PhD. All rights reserved. Thermchemistry Thermchemistry is the study f the energy effects that accmpany

More information

Bed-load Transport of Mixed-size Sediment: Fractional Transport Rates, Bed Forms, and the Development of a Coarse Bed-surface Layer

Bed-load Transport of Mixed-size Sediment: Fractional Transport Rates, Bed Forms, and the Development of a Coarse Bed-surface Layer Utah State University DigitalCmmns@USU Watershed Sciences Faculty Publicatins Watershed Sciences 1-1-1989 Bed-lad Transprt f Mixed-size Sediment: Fractinal Transprt Rates, Bed Frms, and the Develpment

More information

Chapter 3: Cluster Analysis

Chapter 3: Cluster Analysis Chapter 3: Cluster Analysis } 3.1 Basic Cncepts f Clustering 3.1.1 Cluster Analysis 3.1. Clustering Categries } 3. Partitining Methds 3..1 The principle 3.. K-Means Methd 3..3 K-Medids Methd 3..4 CLARA

More information

Ray tracing equations in transversely isotropic media Cosmin Macesanu and Faruq Akbar, Seimax Technologies, Inc.

Ray tracing equations in transversely isotropic media Cosmin Macesanu and Faruq Akbar, Seimax Technologies, Inc. Ray tracing equatins in transversely istrpic media Csmin Macesanu and Faruq Akbar, Seimax Technlgies, Inc. SUMMARY We discuss a simple, cmpact apprach t deriving ray tracing equatins in transversely istrpic

More information

Chem 115 POGIL Worksheet - Week 8 Thermochemistry (Continued), Electromagnetic Radiation, and Line Spectra

Chem 115 POGIL Worksheet - Week 8 Thermochemistry (Continued), Electromagnetic Radiation, and Line Spectra Chem 115 POGIL Wrksheet - Week 8 Thermchemistry (Cntinued), Electrmagnetic Radiatin, and Line Spectra Why? As we saw last week, enthalpy and internal energy are state functins, which means that the sum

More information

Preparation work for A2 Mathematics [2017]

Preparation work for A2 Mathematics [2017] Preparatin wrk fr A2 Mathematics [2017] The wrk studied in Y12 after the return frm study leave is frm the Cre 3 mdule f the A2 Mathematics curse. This wrk will nly be reviewed during Year 13, it will

More information

2. Precipitation Chemistry Data

2. Precipitation Chemistry Data STIMATING TH ATMSPHRIC INT A WATRSH INPUT F PLLUTANTS PRRY J. SAMSN epartment f Atmspheric and ceanic Science, University f Michigan, Ann Arbr, All 4819-2143, U.S.A. (Received June 2, 1986; revised March

More information

Supporting information

Supporting information Electrnic Supplementary Material (ESI) fr Physical Chemistry Chemical Physics This jurnal is The wner Scieties 01 ydrgen perxide electrchemistry n platinum: twards understanding the xygen reductin reactin

More information

Lecture 10, Principal Component Analysis

Lecture 10, Principal Component Analysis Principal Cmpnent Analysis Lecture 10, Principal Cmpnent Analysis Ha Helen Zhang Fall 2017 Ha Helen Zhang Lecture 10, Principal Cmpnent Analysis 1 / 16 Principal Cmpnent Analysis Lecture 10, Principal

More information

20 Faraday s Law and Maxwell s Extension to Ampere s Law

20 Faraday s Law and Maxwell s Extension to Ampere s Law Chapter 20 Faraday s Law and Maxwell s Extensin t Ampere s Law 20 Faraday s Law and Maxwell s Extensin t Ampere s Law Cnsider the case f a charged particle that is ming in the icinity f a ming bar magnet

More information

BASD HIGH SCHOOL FORMAL LAB REPORT

BASD HIGH SCHOOL FORMAL LAB REPORT BASD HIGH SCHOOL FORMAL LAB REPORT *WARNING: After an explanatin f what t include in each sectin, there is an example f hw the sectin might lk using a sample experiment Keep in mind, the sample lab used

More information

THE TOPOLOGY OF SURFACE SKIN FRICTION AND VORTICITY FIELDS IN WALL-BOUNDED FLOWS

THE TOPOLOGY OF SURFACE SKIN FRICTION AND VORTICITY FIELDS IN WALL-BOUNDED FLOWS THE TOPOLOGY OF SURFACE SKIN FRICTION AND VORTICITY FIELDS IN WALL-BOUNDED FLOWS M.S. Chng Department f Mechanical Engineering The University f Melburne Victria 3010 AUSTRALIA min@unimelb.edu.au J.P. Mnty

More information

COMP 551 Applied Machine Learning Lecture 5: Generative models for linear classification

COMP 551 Applied Machine Learning Lecture 5: Generative models for linear classification COMP 551 Applied Machine Learning Lecture 5: Generative mdels fr linear classificatin Instructr: Herke van Hf (herke.vanhf@mail.mcgill.ca) Slides mstly by: Jelle Pineau Class web page: www.cs.mcgill.ca/~hvanh2/cmp551

More information