A SIMPLE SCALING CHARATERISTICS OF RAINFALL IN TIME AND SPACE TO DERIVE INTENSITY DURATION FREQUENCY RELATIONSHIPS

Size: px
Start display at page:

Download "A SIMPLE SCALING CHARATERISTICS OF RAINFALL IN TIME AND SPACE TO DERIVE INTENSITY DURATION FREQUENCY RELATIONSHIPS"

Transcription

1 Annual Journal of Hyraulic Engineering, JSCE, Vol.51, 27, February A SIMPLE SCALING CHARATERISTICS OF RAINFALL IN TIME AND SPACE TO DERIVE INTENSITY DURATION FREQUENCY RELATIONSHIPS Le Minh NHAT 1, Yasuto TACHIKAWA 2, Takahiro SAYAMA 3 an Kaoru TAKARA 4 1 Stuent Member, Grauate stuent, Dept. of Urban an Environmental Eng., Kyoto University (Kyoto , Japan) nhat@floo.pri.kyoto-u.ac.jp 2 Member of JSCE, Dr. Eng., Associate Professor, DPRI, Kyoto University (Gokasho, Uji , Japan) 3 Member of JSCE, M. Eng., Assistant Professor, DPRI, Kyoto University (Gokasho, Uji , Japan) 4 Fellow of JSCE, Dr. Eng., Professor, DPRI, Kyoto University (Gokasho, Uji , Japan) The properties of time an space scale invariance of rainfall are investigate an applie to Intensity-Duration-Freuency (IDF) relationships. The hypothesis of the simple scaling is examine in time an space in Yoo River basin an the simple scaling properties in time are confirme, which is use to erive IDF relationships for short-uration rainfall of several hours from the statistical characteristics of aily ata only. The erive IDF matches well with the one erive from historical observe ata. Also, the simple scaling properties in space are examine. It is foun that two ranges less than 1 km 2 an more than 1 km 2 show ifferent scale properties. Key Wors: rainfall intensity, scaling invariance, IDF curves, esign rainfall. 1. INTRODUCTION The Intensity Duration Freuency (IDF) relationship of heavy storms is one of the most important hyrologic tools utilize by engineers for esigning floo alleviation an rainage structures in urban an urban areas. Local IDF euations are often estimate on the basis of recors of intensities abstracte from rainfall epths of ifferent urations, observe at a given recoring rainfall gauging station. In some regions, there may exist a number of recoring rainfall gauging stations operating for a time perio sufficiently long to yiel a reliable estimation of the IDF relationships; in many other regions, especially in eveloping countries, however, these stations are either non-existent or their sample sizes are too small. Because aily precipitation ata is the most accessible an abunant source of rainfall information, it seems natural, at least for the regions where ata at higher time resolution are scarce, to evelop an apply methos to erive the IDF characteristics of short-uration events from aily rainfall statistics. Over the last two ecaes, concepts of scale invariance have come to the fore in both moelling an ata analysis in hyrological precipitation research. Gupta an Waymire 1) stuie rainfall spatial variability by introucing the concepts of simple an multiple scaling to characterise the probabilistic structure of the precipitation processes. Kuzuha et al. 2) showe the scaling framework an regional floo freuency analysis. Burlano an Rosso 3) showe that both the simple scaling an multiscaling lognormal moels can be use to erive Depth Duration Freuency (DDF) curves of point precipitation. Menabe et al. 4) evelope a simple scaling methoology to use aily rainfall statistics to infer the IDF curves for rainfall uration less than 1 ay. The scaling hypothesis was verifie by fitting the moel to two ifferent sets of ata (from Australia an South Afric. Yu et al. 5) is an example of methoology in which the theories of scaling properties an employe to infer the IDF characteristics of short-uration rainfall from aily ata. Until now, time scaling characteristics have been stuie by many researchers, while space scaling properties that will link to erivation of Area-Intensity-Duration-Freuency (AIDF), are not well stuie. Thus, in this paper, the properties of time an space scale invariance of rainfall are examine in the Yoo River catchment. Then the IDF relationships for short-uration rainfall from aily ata are erive accoring to Menabe 3) an compare with the obtaine from the traitional metho. The paper is organize as follows: The next

2 section presents the theoretical backgroun as relate to the time an space scale invariance properties of short-uration rainfall. In section 3, these properties are verifie for ata observe at rainfall gauging stations locate in the Yoo River catchment in Japan. The IDF relationship, erive from aily rainfall ata, then compare to the traitional estimate curve in section 4 an conclusions are given in the last section. 2. SIMPLE SCALING CHARATERISTICS OF RAINFALL IN TIME AND SPACE In this section, a general theoretical framework for the simple scaling is introuce. The scaling or scale-invariant moels enable us to transform ata from one temporal or spatial moel to another one, an thus, help to overcome the ifficulty of inaeuate ata. A natural process fulfills the simple scaling property if the unerlying probability istribution of some physical measurements at one scale is ientical to the istribution at another scale, multiplie by a factor that is a power function of the ratio of the two scales. The basic theoretical evelopment of scaling has been investigate by many authors incluing Gupta an Waymire 1) an Kuzuha et al. 2) Let X(t) an X( λ t) enote measurements at two istinct time or spatial scales t an λ t, respectively. Definition of scaling of the probability of the X(t) is ist H X ( t) = λ X ( λt) (1) ist The euality = refers to ientical probability istributions in both sie of the euations, λ enotes a scale factor an H is a scaling exponent. Gupta an Waymire 1) introuce the notions of strict an wie sense simple scaling. The strict sense simple scaling in E.(1) implies that X ( t) an H ( λ X ( λt)) have the same probability istribution. The wie sense simple scaling is expresse as they have the same moments, i.e. H [ X( t) ] λ E[ X( λt ] E ) = (2) The scaling exponent, H can be estimate from the slope of linear regression relationship between the log transforme values of moment, log E [ X (λ t) ] an scale parameters log λ for various orer of moment. This is efinition of a wie sense simple scaling 1). A wie sense simple scaling with t=1 an λ t = λ, is given by H [ X( 1) ] λ E[ X( λ ] E ) = (3) If the scaling exponent H is not constant an changes probabilistically, E.(3) are escribe as ( ) [ (1) EX ] = λ K EX [ ( λ) ] (4) where K() is a function of the moment orer. The proceure to test the suitability of scale invariant moel to escribe the rainfall process is briefly escribe in Fig.1. The moments E [ X (λt) ] are plotte on the logarithmic chart versus the scale λ for ifferent moments orer. The slope K() is plotte on the linear chart versus the moment orer. If the resulting graph is a straight line, the fiel is simple scaling, while in other cases, the multi-scaling approach has to be consiere 1). Log [moment] K () Simple scaling Fig.1 Simple an multiscaling in term of statistical moments. First step, moments of ifferent orers are plotte as function of scale in a log-log plot. From the slope, values of the function K() are obtaine. If K() is linear, the process is simple scaling. If K() is non-linear, the process is multiscaling. (1) Time scaling of rainfall intensity Let the ranom variable I() the maximum annual value of local rainfall intensity over a uration. It is efine as: t+ / 2 1 I( ) = max X ( ξ ) ξ (5) t 1 year t / 2 where X (ξ ) is a time continuous stochastic process representing rainfall intensity an is uration. It is suppose that I() represents the Annual Maximum (AMRI) of uration, efine by the maximum value of moving average of with of the continuous rainfall process. Here, some concepts are introuce about scaling of the probability istribution of ranom functions. A generic ranom function I() is enote by simple scaling properties if it obeys the following: ist H D I( ) = I( D) (6) D is a aggregate time uration, i.e.: 2, 3,..., 24 hours. D Defining the scaling ratio is λ = ist H I ( ) = λ I( λ ) (7) Log [scale] K () Mutil-scaling

3 The E.(7) is rewritten in terms of the moments of orer about the origin, enote by E [ I( ) ]. The resulting expression is: ( ) H E I = λ EI( λ ) (8) [ ] [ ] If one assumes the wie sense simple scaling exists, the istribution of IDF for short-uration of rainfall intensity can be erive from aily rainfall. (2) Space scaling of rainfall intensity Let consier a continuous precipitation process I(, which represents the maximum annual value of average rainfall intensity over a uration, an an area a. It is efine as I(, 1 max t 1 year a t+ / 2 t / 2 a = X ( ξ, ω) ωξ (9) where X ( ξ, ω) is a time-space continuous stochastic process representing rainfall intensity. Since the probability of extreme events is usually examine, the maximum annual rainfall intensity can be efine as the maximum value of a moving average (with area span) in a given year. The concepts are introuce about scaling of the probability istribution of ranom functions. A generic ranom function I(,,with fixe uration, is enote by the simple scaling properties of space if it obeys the following relationship: ist H A a Ia (, ) = IA (, ) a Defining the space scaling ratio is ist λ a = A a (1) Ha Ia (, ) = λa I (, λ (11) This also implies that the moments of any orer are scale-invariance. The resulting expression is (, ) H a E Ia = λ EI (, λ (12) [ ] a [ a ] where enotes the orer of the moment. If one assumes the wie sense simple scaling exists, the AIDF curves can be erive by eveloping a general framework base on the estimation of a common scaling exponent for any freuency level. This approach is use to erive the istribution of the AIDF where ata for the spatial scale of interest oes not exist. 3. SCALE INVARIANCE PROPERTIES OF RAINFALL IN TIME AND SPACE IN YODO RIVER CATCHMENT, JAPAN The scaling properties of rainfall ata was investigate by computing the moment for each uration an area an then by examining the log-log plots of the moments against their uration an area. Fig.2 an Fig.3 illustrate the relationships between moments versus uration (time) an area (space) an a plot of the scaling exponents versus the orer of moments for the Yoo River catchment. In orer to examine the time scale invariance of rainfall in the Yoo River catchment, the four stations Hikone, Hirakata, Ieno an Kamo were selecte from Yoo River catchment. The recor lengths are 21 years an range from 1982 to 22. The analysis was performe on annual maximum rainfall series for storm urations from 1 hour to 24 hours, with λ =1, Fig.2 shows the relationships between the log-transforme values of moment of various orers against values uration at the Hikone station, the slopes of linear regression efine the scaling exponents H. Fig.2b) shows the scaling exponent ecreases with the orer of moment an a linear relationship exists between scaling exponents an orers of moment, which implies that the property of wie sense simple scaling of rainfall intensity exists in this station. In Table 1, the results of the scaling exponent factor H of the four stations in the Yoo River catchment are shown with the high coefficients of etermination for each station ranging from.98 to 1. The result inicates a strong valiity of the simple scaling property of the extreme rainfall in time series. Sample moment of orer 1.E+9 1.E+8 1.E+7 1.E+6 1.E+5 HIKONE Station 1.E+4 6=5 1.E+3 5=4 1.E+2 4=3 3=2 1.E+1 2=1 1=.5 1.E Duration (hour) K() y = -.658x -.13 R 2 =.9999 Hikone Station b) Fig.2 The time scale invariance at the Hikone station, the Yoo catchment, Japan Relationship between moment of orer an uration (hour) b) Relationship between K() an the sample moment orer.

4 M om ent E[I(6,A)] 1.E+8 1.E+7 1.E+6 1.E+5 1.E+4 1.E+3 1.E+2 1.E+1 1.E Area (km 2 ) K() y = x R 2 =.99 A=2.25 to 1 Km 2 y = -.474x R 2 =.99 A=1 to b) Fig.3 The space scale invariance at the Yoo River catchment for 6 hours. Relationship between moment of orer an area A (km 2 ). b) Relationship between K() an the sample moment orer. Table 1. The scaling exponent factor of the four stations in the Yoo River catchment Name of the station No of years recor Scaling exponent H R 2 Hikone Hirakata Ieno Kamo To examine the space scaling invariance, at first hourly ata from 1982 to 22 with 1.5 x 1.5 km spatial resolution, which is generate by AMeDAS rain gauge ata an covers the Yoo River basin are arrange. To obtain spatial mean rainfall intensity the Otorii station is put at the center of the area, an the area is expane in the form of circle with increase raius by.5 km. The ata use for examine spatial scaling factor are annual maximum rainfall series for the area from 2.25 km 2 to km 2, with λ a =1, an fixe uration. In Fig.3 a ifference of the egree of steepness in the slopes for the area (2.25 km 2 to 1 km 2 ) an larger area (1 km 2 to 5 km 2 ) area is foun, which inicates that two ifferent scaling space regimes exist for rainfall space scaling. A steeper slope is foun in the smaller area compare to the lager area. The plots inicate that the relationships between moments an areas are linear having two ifferent slopes with a breaking point at 1 km 2. This property suggests an existence of the two ifferent regimes with a transition in storm ynamics from high variability convective storms with less than 1 km 2 to frontal storms in an area larger than 1 km DERIVATION OF IDF FOR SHORT DURATION All forms of the generalize IDF relationships assume that rainfall epth or intensity is inversely relate to the uration of a storm raise to a power, or scale factor 6). There are several commonly use functions foun in the literature of hyrology applications 7),8),9),1). Koutsoyiannis et al. 11) have moifie the IDF relationship for a given return perio as particular cases, using the following general empirical formula w i = (13) ( +θ) where i enotes the rainfall intensity for uration an w, θ an represent non-negative coefficients. In fact, these arguments justify the formulation of the following general moel for the IDF relationships: a( T ) i = (14) b( ) In Euation (14), b() = ( + θ) with θ> an <<1, whereas a(t) is completely efine by the probability istribution function of the maximum rainfall intensity. The form of Euation (14) is consistent with most IDF empirical euations estimate for many locations 12) : For example Nhat et al. 13) establishe the IDF curves for precipitation in the monsoon area of Vietnam. The ranom variable rainfall intensity I() for uration, has a cumulative probability istribution CDF, which is given by 1 Pr( I( ) i) = F ( i) = 1 (15) T ( i) Accoring to the scaling theory by Menabe et al. 4), the scaling property in a strict sense can be written explicitly using the CDF:

5 H F() i = Fλ [ ] λ i (16) For many parametric forms, left han sie of Euation (16) may be expresse in terms of stanar variant, as in i μ F ( i) = F (17) σ where F (.) is a function inepenent of. Uner this form, it can be euce from Euation (16) that H μ = λ μ λ (18) H σ = λ σ λ (19) Substituting Euations (17), (18) an (19) into Euation (15) an investing with respect to i, one obtains: H H 1 μλ ( ) ( ) (1 1/ ) λ + σλ λ F T it, = (2) H By eualing Euation (2) to the general moel for IDF relationship, given by Euation (13), it is easy to verify that = H (21) θ = (22) b ( ) = (23) at = + F T (24) H H 1 ( ) μλ ( ) ( ) (1 1/ ) λ σλ λ 1 μ + σf (1 1/ T ) i, T = (25) where ( H μ = μλ ) λ an ( H σ = σλ ) λ are constants. It is worthwhile to note that the simple scaling hypothesis leas to the euality between the scale factor an the exponent in the expression relating rainfall intensity an uration. Application of the simple scaling moel for rainfall intensities at the Hikone station, the scale factor can be estimate H =.658. The IDF relationship for a short uration rainfall can be euce from aily ata by Euation (25) with the estimates of μ D an σ with D=24h. From D 24-hour ata collecte at the Hikone recoring station, the sample of 21 years of 24 hours annual maximum rainfall intensity yiels, which can be estimate μ D =24 = an σ D=24 = Back with these estimates an the Gumbel inverse function, the euce IDF relationship for the location of Hikone may be written as Euation (25) with μ = λ μ 24 = an σ = λ σ = then ln( ln(1 1/ T )) i = (26).65 The rainfall Intensity Duration Freuency curves for the Hikone station can be reconstructe by scaling methos with Euation (26). Figure 4 shows well matching of the IDF relationships calculate by Euation (26) an plots obtaine by the historical ata as the return perios from 5 to 1 years. The scale factor H along with the parameters σ an μ, may be interprete as regional climatic characteristics Years return perio Scaling metho Years return perio Scaling metho Years return perio Scaling metho Years return perio Scaling metho Fig.4 The Freuency Curves at the Hikone station, the Yoo Catchments, Japan by the scaling metho. b) c)

6 Rainfall intensity(mm/hr) 7 65 Area=11.25km Year return perio Rainfall intensity(mm/hr) 7 65 b) Area=992.25km Year return perio Fig. 5 The Area Freuency Curves at the Yoo River catchment, Japan by the scaling metho. Area=11.25Km 2 an b)area= km 2. The AIDF curves can be erive by the simple scaling metho. For example, with a fixe area eual to km 2 an a scaling factor H=-.51; μ = λ μ 24 = 25.8; σ = λ σ 24 = 8.22 are foun, the AIDF curves can be erive by: ln( ln(1 1/ T )) i = (27).514 For an area of km 2, the IDF curve can be constructe with a scaling factor H = -.46: ln( ln(1 1/ T )) i = (28).46 The Figure 5 shows a result of the AIDF base on the scaling metho in the Yoo River catchment by the euations (27) an (28). 5. CONCLUSION The major finings of the present stuy can be summarize as follows: The properties of the time an space scale invariance of rainfall uantiles are examine in the Yoo River basin: For time scaling, rainfall properties follows a simple scaling; For space scaling, a simple scaling process with the two ifferent regimes of 2.25 km 2 to 1 km 2 an 1 km 2 to 5 km 2 are foun. Then, accoring to Menabe et al. 4) the rainfall IDF curves for a short uration (hourly) were erive from 24-hour ata. The simple scaling properties are verifie by local ata; the IDF relationships are euce from aily rainfall, which shows goo results in comparison with the IDF curves obtaine from at-site short-uration rainfall ata. Results of this stuy are of significant practical importance because statistical rainfall inferences can be mae with the use of a simple scaling in time an space. Furthermore, aily ata are more wiely available from stanar rain gauge measurements, but ata for short urations are often not available for the reuire site. Further works will focus on a combination between the time scaling an the space scaling an theoretical escription of the AIDF applicable for a less gauge basin. ACKNOWLEDGMENT: This stuy was supporte by Grant-in-Ai for Scientific Research (C) (PI: Assoc. Prof. Y. Tachikawa, Kyoto Univ.). REFERENCES 1) Gupta, V. K. an Waymire, E.: Multiscaling properties of spatial rainfall an river flow istributions. Journal of Geophysical Research, 95(D3): , ) Kuzuha, Y., Komatsu, Y., Tomosugi, K., Kishii, T.: Regional Floo Freuency Analysis, Scaling an PUB, Journal Japan Soc. Hyrol. an Water Resources Vol.18,No.4, pp , 25. 3) Burlano, P. an Rosso, R.: Scaling an multiscaling moels of epth-uration-freuency curves for storm precipitation. Journal of Hyrology, 187, pp , ) Menabe, M., See, A., Pegram, G.: A simple scaling moel for extreme rainfall. Water Resources Research, Vol. 35, No.1, pp , ) Yu, P. S., Yang, T.C. an Lin, C. S.: Regional rainfall intensity formulas base on scaling property of rainfall Journal of Hyrology, 295 (1-4), pp , 24. 6) Chow, V.T., Maiment, D.R. & Mays, L.W: Applie Hyrology, McGraw-Hill, ) Chen, C. L.: Rainfall intensity uration freuency formulas, Journal of Hyraulic Engineering, ASCE, 19(12), pp , ) Hershfie, D. M.: Estimating the Probable Maximum Precipitation, Journal of the Hyraulic Division, Proceeing of the ASCE, HY5, pp , ) Van Nguyen, V. T., Nguyen, T.-D., Ashkar, F.: Regional freuency analysis of extreme rainfalls, Water Sci. Technol. 45(2), pp.75 81, 22. 1) Bell, F. C.: Generalize rainfall uration freuency relationships. Journal of Hyraulic Div., ASCE, 95(1), pp , ) Koutsoyiannis, D., Manetas, A.: A mathematical framework for stuying rainfall intensity uration freuency relationships, Journal of Hyrology, 26, pp , ) Kothyari, U. C. an Grae, R.J.: Rainfall intensity uration freuency formula for Inia, J. Hyr. Eng., ASCE, 118(2), pp , ) Nhat, L. M., Tachikawa, Y., Takara, K.: Establishment of Intensity-Duration-Freuency curves for precipitation in the monsoon area of Vietnam, Annuals of Disas. Prev. Res. Inst., Kyoto Univ., No. 49B, 26. (Receive September 3, 26)

Establishment of Intensity-Duration- Frequency Formula for Precipitation in Puthimari Basin, Assam

Establishment of Intensity-Duration- Frequency Formula for Precipitation in Puthimari Basin, Assam Establishment of Intensity-Duration- Frequency Formula for Precipitation in Puthimari Basin, Assam Tinku Kalita 1, Bipul Talukdar 2 P.G. Student, Department of Civil Engineering, Assam Engineering College,

More information

. Using a multinomial model gives us the following equation for P d. , with respect to same length term sequences.

. Using a multinomial model gives us the following equation for P d. , with respect to same length term sequences. S 63 Lecture 8 2/2/26 Lecturer Lillian Lee Scribes Peter Babinski, Davi Lin Basic Language Moeling Approach I. Special ase of LM-base Approach a. Recap of Formulas an Terms b. Fixing θ? c. About that Multinomial

More information

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013

Survey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013 Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing

More information

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE

THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE Journal of Soun an Vibration (1996) 191(3), 397 414 THE VAN KAMPEN EXPANSION FOR LINKED DUFFING LINEAR OSCILLATORS EXCITED BY COLORED NOISE E. M. WEINSTEIN Galaxy Scientific Corporation, 2500 English Creek

More information

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments

Time-of-Arrival Estimation in Non-Line-Of-Sight Environments 2 Conference on Information Sciences an Systems, The Johns Hopkins University, March 2, 2 Time-of-Arrival Estimation in Non-Line-Of-Sight Environments Sinan Gezici, Hisashi Kobayashi an H. Vincent Poor

More information

d dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1

d dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1 Lecture 5 Some ifferentiation rules Trigonometric functions (Relevant section from Stewart, Seventh Eition: Section 3.3) You all know that sin = cos cos = sin. () But have you ever seen a erivation of

More information

Temporal Distribution of 24-hour Maximum Rainfall

Temporal Distribution of 24-hour Maximum Rainfall International Journal of Engineering Science Invention ISSN (Online): 2319 6734 ISSN (Print): 2319 6726 Volume 6 Issue 7 July 2017 PP. 06-10 Temporal Distribution of 24-hour Maximum Rainfall * Omer Leven

More information

Resilient Modulus Prediction Model for Fine-Grained Soils in Ohio: Preliminary Study

Resilient Modulus Prediction Model for Fine-Grained Soils in Ohio: Preliminary Study Resilient Moulus Preiction Moel for Fine-Graine Soils in Ohio: Preliminary Stuy by Teruhisa Masaa: Associate Professor, Civil Engineering Department Ohio University, Athens, OH 4570 Tel: (740) 59-474 Fax:

More information

Ductility and Failure Modes of Single Reinforced Concrete Columns. Hiromichi Yoshikawa 1 and Toshiaki Miyagi 2

Ductility and Failure Modes of Single Reinforced Concrete Columns. Hiromichi Yoshikawa 1 and Toshiaki Miyagi 2 Ductility an Failure Moes of Single Reinforce Concrete Columns Hiromichi Yoshikawa 1 an Toshiaki Miyagi 2 Key Wors: seismic capacity esign, reinforce concrete column, failure moes, eformational uctility,

More information

Analysis of Storm Pattern for Design Urban Drainage System in the Monsoon Areas of Vietnam

Analysis of Storm Pattern for Design Urban Drainage System in the Monsoon Areas of Vietnam Journal of Environmental Science and Engineering A 7 (218) 49-68 doi:1.17265/2162-5298/218.2.1 D DAVID PUBLISHING Analysis of Storm Pattern for Design Urban Drainage System in the Monsoon Areas of Vietnam

More information

A Modification of the Jarque-Bera Test. for Normality

A Modification of the Jarque-Bera Test. for Normality Int. J. Contemp. Math. Sciences, Vol. 8, 01, no. 17, 84-85 HIKARI Lt, www.m-hikari.com http://x.oi.org/10.1988/ijcms.01.9106 A Moification of the Jarque-Bera Test for Normality Moawa El-Fallah Ab El-Salam

More information

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0. Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?

More information

Differentiability, Computing Derivatives, Trig Review

Differentiability, Computing Derivatives, Trig Review Unit #3 : Differentiability, Computing Derivatives, Trig Review Goals: Determine when a function is ifferentiable at a point Relate the erivative graph to the the graph of an original function Compute

More information

American Society of Agricultural Engineers PAPER NO PRAIRIE RAINFALL,CHARACTERISTICS

American Society of Agricultural Engineers PAPER NO PRAIRIE RAINFALL,CHARACTERISTICS - PAPER NO. 79-2108 PRAIRIE RAINFALL,CHARACTERISTICS G.E. Dyck an D.M. Gray Research Engineer an Chairman Division of Hyrology University of Saskatchewan Saskatoon, Saskatchewan, Canaa For presentation

More information

Sparse Reconstruction of Systems of Ordinary Differential Equations

Sparse Reconstruction of Systems of Ordinary Differential Equations Sparse Reconstruction of Systems of Orinary Differential Equations Manuel Mai a, Mark D. Shattuck b,c, Corey S. O Hern c,a,,e, a Department of Physics, Yale University, New Haven, Connecticut 06520, USA

More information

A Weak First Digit Law for a Class of Sequences

A Weak First Digit Law for a Class of Sequences International Mathematical Forum, Vol. 11, 2016, no. 15, 67-702 HIKARI Lt, www.m-hikari.com http://x.oi.org/10.1288/imf.2016.6562 A Weak First Digit Law for a Class of Sequences M. A. Nyblom School of

More information

EVOLUTION OF PARTICLE SIZE DISTRIBUTION IN AIR IN THE RAINFALL PROCESS VIA THE MOMENT METHOD

EVOLUTION OF PARTICLE SIZE DISTRIBUTION IN AIR IN THE RAINFALL PROCESS VIA THE MOMENT METHOD 137 THERMAL SCIENCE, Year 1, Vol. 16, No. 5, pp. 137-1376 EVOLUTION OF PARTICLE SIZE DISTRIBUTION IN AIR IN THE RAINFALL PROCESS VIA THE MOMENT METHOD by Fu-Jun GAN a an Jian-Zhong LIN a,b * a Department

More information

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0. Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?

More information

This module is part of the. Memobust Handbook. on Methodology of Modern Business Statistics

This module is part of the. Memobust Handbook. on Methodology of Modern Business Statistics This moule is part of the Memobust Hanbook on Methoology of Moern Business Statistics 26 March 2014 Metho: Balance Sampling for Multi-Way Stratification Contents General section... 3 1. Summary... 3 2.

More information

θ x = f ( x,t) could be written as

θ x = f ( x,t) could be written as 9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)

More information

Introduction to the Vlasov-Poisson system

Introduction to the Vlasov-Poisson system Introuction to the Vlasov-Poisson system Simone Calogero 1 The Vlasov equation Consier a particle with mass m > 0. Let x(t) R 3 enote the position of the particle at time t R an v(t) = ẋ(t) = x(t)/t its

More information

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain

Nonlinear Adaptive Ship Course Tracking Control Based on Backstepping and Nussbaum Gain Nonlinear Aaptive Ship Course Tracking Control Base on Backstepping an Nussbaum Gain Jialu Du, Chen Guo Abstract A nonlinear aaptive controller combining aaptive Backstepping algorithm with Nussbaum gain

More information

Energy behaviour of the Boris method for charged-particle dynamics

Energy behaviour of the Boris method for charged-particle dynamics Version of 25 April 218 Energy behaviour of the Boris metho for charge-particle ynamics Ernst Hairer 1, Christian Lubich 2 Abstract The Boris algorithm is a wiely use numerical integrator for the motion

More information

Calculus in the AP Physics C Course The Derivative

Calculus in the AP Physics C Course The Derivative Limits an Derivatives Calculus in the AP Physics C Course The Derivative In physics, the ieas of the rate change of a quantity (along with the slope of a tangent line) an the area uner a curve are essential.

More information

Differentiability, Computing Derivatives, Trig Review. Goals:

Differentiability, Computing Derivatives, Trig Review. Goals: Secants vs. Derivatives - Unit #3 : Goals: Differentiability, Computing Derivatives, Trig Review Determine when a function is ifferentiable at a point Relate the erivative graph to the the graph of an

More information

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation

Thermal conductivity of graded composites: Numerical simulations and an effective medium approximation JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION

LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische

More information

Characterizing Climate-Change Impacts on the 1.5-yr Flood Flow in Selected Basins across the United States: A Probabilistic Approach

Characterizing Climate-Change Impacts on the 1.5-yr Flood Flow in Selected Basins across the United States: A Probabilistic Approach Paper No. 18 Page 1 Copyright Ó 2011, Paper 15-018; 5106 wors, 5 Figures, 0 Animations, 3 Tables. http://earthinteractions.org Characterizing Climate-Change Impacts on the 1.5-yr Floo Flow in Selecte Basins

More information

Make graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides

Make graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides Reference 1: Transformations of Graphs an En Behavior of Polynomial Graphs Transformations of graphs aitive constant constant on the outsie g(x) = + c Make graph of g by aing c to the y-values on the graph

More information

Dot trajectories in the superposition of random screens: analysis and synthesis

Dot trajectories in the superposition of random screens: analysis and synthesis 1472 J. Opt. Soc. Am. A/ Vol. 21, No. 8/ August 2004 Isaac Amiror Dot trajectories in the superposition of ranom screens: analysis an synthesis Isaac Amiror Laboratoire e Systèmes Périphériques, Ecole

More information

Topic 7: Convergence of Random Variables

Topic 7: Convergence of Random Variables Topic 7: Convergence of Ranom Variables Course 003, 2016 Page 0 The Inference Problem So far, our starting point has been a given probability space (S, F, P). We now look at how to generate information

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

Role of parameters in the stochastic dynamics of a stick-slip oscillator

Role of parameters in the stochastic dynamics of a stick-slip oscillator Proceeing Series of the Brazilian Society of Applie an Computational Mathematics, v. 6, n. 1, 218. Trabalho apresentao no XXXVII CNMAC, S.J. os Campos - SP, 217. Proceeing Series of the Brazilian Society

More information

An inductance lookup table application for analysis of reluctance stepper motor model

An inductance lookup table application for analysis of reluctance stepper motor model ARCHIVES OF ELECTRICAL ENGINEERING VOL. 60(), pp. 5- (0) DOI 0.478/ v07-0-000-y An inuctance lookup table application for analysis of reluctance stepper motor moel JAKUB BERNAT, JAKUB KOŁOTA, SŁAWOMIR

More information

Reliability Analysis of Free Jet Scour Below Dams

Reliability Analysis of Free Jet Scour Below Dams Entropy2012, 1, 2578-2588; oi:10.3390/e1122578 Article OPEN ACCESS entropy ISSN 1099-300 www.mpi.com/journal/entropy eliability Analysis of Free Jet Scour Below Dams Chuanqi Li *, Shuai Wang an Wei Wang

More information

LINEAR DIFFERENTIAL EQUATIONS OF ORDER 1. where a(x) and b(x) are functions. Observe that this class of equations includes equations of the form

LINEAR DIFFERENTIAL EQUATIONS OF ORDER 1. where a(x) and b(x) are functions. Observe that this class of equations includes equations of the form LINEAR DIFFERENTIAL EQUATIONS OF ORDER 1 We consier ifferential equations of the form y + a()y = b(), (1) y( 0 ) = y 0, where a() an b() are functions. Observe that this class of equations inclues equations

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,

More information

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs

Lectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent

More information

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21

'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21 Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting

More information

EVALUATION OF LIQUEFACTION RESISTANCE AND LIQUEFACTION INDUCED SETTLEMENT FOR RECLAIMED SOIL

EVALUATION OF LIQUEFACTION RESISTANCE AND LIQUEFACTION INDUCED SETTLEMENT FOR RECLAIMED SOIL 386 EVALUATION OF LIQUEFACTION RESISTANCE AND LIQUEFACTION INDUCED SETTLEMENT FOR RECLAIMED SOIL Lien-Kwei CHIEN 1, Yan-Nam OH 2 An Chih-Hsin CHANG 3 SUMMARY In this stuy, the fille material in Yun-Lin

More information

Lecture 2 Lagrangian formulation of classical mechanics Mechanics

Lecture 2 Lagrangian formulation of classical mechanics Mechanics Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,

More information

A SIMPLE ENGINEERING MODEL FOR SPRINKLER SPRAY INTERACTION WITH FIRE PRODUCTS

A SIMPLE ENGINEERING MODEL FOR SPRINKLER SPRAY INTERACTION WITH FIRE PRODUCTS International Journal on Engineering Performance-Base Fire Coes, Volume 4, Number 3, p.95-3, A SIMPLE ENGINEERING MOEL FOR SPRINKLER SPRAY INTERACTION WITH FIRE PROCTS V. Novozhilov School of Mechanical

More information

Table of Common Derivatives By David Abraham

Table of Common Derivatives By David Abraham Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec

More information

3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes

3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes Fin these erivatives of these functions: y.7 Implicit Differentiation -- A Brief Introuction -- Stuent Notes tan y sin tan = sin y e = e = Write the inverses of these functions: y tan y sin How woul we

More information

Similarity Measures for Categorical Data A Comparative Study. Technical Report

Similarity Measures for Categorical Data A Comparative Study. Technical Report Similarity Measures for Categorical Data A Comparative Stuy Technical Report Department of Computer Science an Engineering University of Minnesota 4-92 EECS Builing 200 Union Street SE Minneapolis, MN

More information

Least-Squares Regression on Sparse Spaces

Least-Squares Regression on Sparse Spaces Least-Squares Regression on Sparse Spaces Yuri Grinberg, Mahi Milani Far, Joelle Pineau School of Computer Science McGill University Montreal, Canaa {ygrinb,mmilan1,jpineau}@cs.mcgill.ca 1 Introuction

More information

OPTIMAL CONTROL PROBLEM FOR PROCESSES REPRESENTED BY STOCHASTIC SEQUENTIAL MACHINE

OPTIMAL CONTROL PROBLEM FOR PROCESSES REPRESENTED BY STOCHASTIC SEQUENTIAL MACHINE OPTIMA CONTRO PROBEM FOR PROCESSES REPRESENTED BY STOCHASTIC SEQUENTIA MACHINE Yaup H. HACI an Muhammet CANDAN Department of Mathematics, Canaale Onseiz Mart University, Canaale, Turey ABSTRACT In this

More information

Hyperbolic Moment Equations Using Quadrature-Based Projection Methods

Hyperbolic Moment Equations Using Quadrature-Based Projection Methods Hyperbolic Moment Equations Using Quarature-Base Projection Methos J. Koellermeier an M. Torrilhon Department of Mathematics, RWTH Aachen University, Aachen, Germany Abstract. Kinetic equations like the

More information

Leaving Randomness to Nature: d-dimensional Product Codes through the lens of Generalized-LDPC codes

Leaving Randomness to Nature: d-dimensional Product Codes through the lens of Generalized-LDPC codes Leaving Ranomness to Nature: -Dimensional Prouct Coes through the lens of Generalize-LDPC coes Tavor Baharav, Kannan Ramchanran Dept. of Electrical Engineering an Computer Sciences, U.C. Berkeley {tavorb,

More information

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems

Construction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu

More information

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k

Robust Forward Algorithms via PAC-Bayes and Laplace Distributions. ω Q. Pr (y(ω x) < 0) = Pr A k A Proof of Lemma 2 B Proof of Lemma 3 Proof: Since the support of LL istributions is R, two such istributions are equivalent absolutely continuous with respect to each other an the ivergence is well-efine

More information

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France

APPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France APPROXIMAE SOLUION FOR RANSIEN HEA RANSFER IN SAIC URBULEN HE II B. Bauouy CEA/Saclay, DSM/DAPNIA/SCM 91191 Gif-sur-Yvette Ceex, France ABSRAC Analytical solution in one imension of the heat iffusion equation

More information

Designing of Acceptance Double Sampling Plan for Life Test Based on Percentiles of Exponentiated Rayleigh Distribution

Designing of Acceptance Double Sampling Plan for Life Test Based on Percentiles of Exponentiated Rayleigh Distribution International Journal of Statistics an Systems ISSN 973-675 Volume, Number 3 (7), pp. 475-484 Research Inia Publications http://www.ripublication.com Designing of Acceptance Double Sampling Plan for Life

More information

18 EVEN MORE CALCULUS

18 EVEN MORE CALCULUS 8 EVEN MORE CALCULUS Chapter 8 Even More Calculus Objectives After stuing this chapter you shoul be able to ifferentiate an integrate basic trigonometric functions; unerstan how to calculate rates of change;

More information

1 The Derivative of ln(x)

1 The Derivative of ln(x) Monay, December 3, 2007 The Derivative of ln() 1 The Derivative of ln() The first term or semester of most calculus courses will inclue the it efinition of the erivative an will work out, long han, a number

More information

TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM

TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM 265 Asian Journal of Control, Vol. 4, No. 3, pp. 265-273, September 22 TRACKING CONTROL OF MULTIPLE MOBILE ROBOTS: A CASE STUDY OF INTER-ROBOT COLLISION-FREE PROBLEM Jurachart Jongusuk an Tsutomu Mita

More information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

YORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics. MATH A Test #2. June 25, 2014 SOLUTIONS

YORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics. MATH A Test #2. June 25, 2014 SOLUTIONS YORK UNIVERSITY Faculty of Science Department of Mathematics an Statistics MATH 505 6.00 A Test # June 5, 04 SOLUTIONS Family Name (print): Given Name: Stuent No: Signature: INSTRUCTIONS:. Please write

More information

A Review of Multiple Try MCMC algorithms for Signal Processing

A Review of Multiple Try MCMC algorithms for Signal Processing A Review of Multiple Try MCMC algorithms for Signal Processing Luca Martino Image Processing Lab., Universitat e València (Spain) Universia Carlos III e Mari, Leganes (Spain) Abstract Many applications

More information

DEGREE DISTRIBUTION OF SHORTEST PATH TREES AND BIAS OF NETWORK SAMPLING ALGORITHMS

DEGREE DISTRIBUTION OF SHORTEST PATH TREES AND BIAS OF NETWORK SAMPLING ALGORITHMS DEGREE DISTRIBUTION OF SHORTEST PATH TREES AND BIAS OF NETWORK SAMPLING ALGORITHMS SHANKAR BHAMIDI 1, JESSE GOODMAN 2, REMCO VAN DER HOFSTAD 3, AND JÚLIA KOMJÁTHY3 Abstract. In this article, we explicitly

More information

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions

Computing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5

More information

Conservation Laws. Chapter Conservation of Energy

Conservation Laws. Chapter Conservation of Energy 20 Chapter 3 Conservation Laws In orer to check the physical consistency of the above set of equations governing Maxwell-Lorentz electroynamics [(2.10) an (2.12) or (1.65) an (1.68)], we examine the action

More information

Polynomial Inclusion Functions

Polynomial Inclusion Functions Polynomial Inclusion Functions E. e Weert, E. van Kampen, Q. P. Chu, an J. A. Muler Delft University of Technology, Faculty of Aerospace Engineering, Control an Simulation Division E.eWeert@TUDelft.nl

More information

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations

Optimized Schwarz Methods with the Yin-Yang Grid for Shallow Water Equations Optimize Schwarz Methos with the Yin-Yang Gri for Shallow Water Equations Abessama Qaouri Recherche en prévision numérique, Atmospheric Science an Technology Directorate, Environment Canaa, Dorval, Québec,

More information

Optimum design of tuned mass damper systems for seismic structures

Optimum design of tuned mass damper systems for seismic structures Earthquake Resistant Engineering Structures VII 175 Optimum esign of tune mass amper systems for seismic structures I. Abulsalam, M. Al-Janabi & M. G. Al-Taweel Department of Civil Engineering, Faculty

More information

ON THE OPTIMALITY SYSTEM FOR A 1 D EULER FLOW PROBLEM

ON THE OPTIMALITY SYSTEM FOR A 1 D EULER FLOW PROBLEM ON THE OPTIMALITY SYSTEM FOR A D EULER FLOW PROBLEM Eugene M. Cliff Matthias Heinkenschloss y Ajit R. Shenoy z Interisciplinary Center for Applie Mathematics Virginia Tech Blacksburg, Virginia 46 Abstract

More information

Estimation of District Level Poor Households in the State of. Uttar Pradesh in India by Combining NSSO Survey and

Estimation of District Level Poor Households in the State of. Uttar Pradesh in India by Combining NSSO Survey and Int. Statistical Inst.: Proc. 58th Worl Statistical Congress, 2011, Dublin (Session CPS039) p.6567 Estimation of District Level Poor Househols in the State of Uttar Praesh in Inia by Combining NSSO Survey

More information

Quantile function expansion using regularly varying functions

Quantile function expansion using regularly varying functions Quantile function expansion using regularly varying functions arxiv:705.09494v [math.st] 9 Aug 07 Thomas Fung a, an Eugene Seneta b a Department of Statistics, Macquarie University, NSW 09, Australia b

More information

On the Surprising Behavior of Distance Metrics in High Dimensional Space

On the Surprising Behavior of Distance Metrics in High Dimensional Space On the Surprising Behavior of Distance Metrics in High Dimensional Space Charu C. Aggarwal, Alexaner Hinneburg 2, an Daniel A. Keim 2 IBM T. J. Watson Research Center Yortown Heights, NY 0598, USA. charu@watson.ibm.com

More information

Outline. Calculus for the Life Sciences II. Introduction. Tides Introduction. Lecture Notes Differentiation of Trigonometric Functions

Outline. Calculus for the Life Sciences II. Introduction. Tides Introduction. Lecture Notes Differentiation of Trigonometric Functions Calculus for the Life Sciences II c Functions Joseph M. Mahaffy, mahaffy@math.ssu.eu Department of Mathematics an Statistics Dynamical Systems Group Computational Sciences Research Center San Diego State

More information

Quantum mechanical approaches to the virial

Quantum mechanical approaches to the virial Quantum mechanical approaches to the virial S.LeBohec Department of Physics an Astronomy, University of Utah, Salt Lae City, UT 84112, USA Date: June 30 th 2015 In this note, we approach the virial from

More information

The Exact Form and General Integrating Factors

The Exact Form and General Integrating Factors 7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily

More information

The Role of Models in Model-Assisted and Model- Dependent Estimation for Domains and Small Areas

The Role of Models in Model-Assisted and Model- Dependent Estimation for Domains and Small Areas The Role of Moels in Moel-Assiste an Moel- Depenent Estimation for Domains an Small Areas Risto Lehtonen University of Helsini Mio Myrsylä University of Pennsylvania Carl-Eri Särnal University of Montreal

More information

Optimization of Geometries by Energy Minimization

Optimization of Geometries by Energy Minimization Optimization of Geometries by Energy Minimization by Tracy P. Hamilton Department of Chemistry University of Alabama at Birmingham Birmingham, AL 3594-140 hamilton@uab.eu Copyright Tracy P. Hamilton, 1997.

More information

arxiv: v1 [physics.class-ph] 20 Dec 2017

arxiv: v1 [physics.class-ph] 20 Dec 2017 arxiv:1712.07328v1 [physics.class-ph] 20 Dec 2017 Demystifying the constancy of the Ermakov-Lewis invariant for a time epenent oscillator T. Pamanabhan IUCAA, Post Bag 4, Ganeshkhin, Pune - 411 007, Inia.

More information

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control

19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control 19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior

More information

Linear First-Order Equations

Linear First-Order Equations 5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)

More information

IPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy

IPA Derivatives for Make-to-Stock Production-Inventory Systems With Backorders Under the (R,r) Policy IPA Derivatives for Make-to-Stock Prouction-Inventory Systems With Backorers Uner the (Rr) Policy Yihong Fan a Benamin Melame b Yao Zhao c Yorai Wari Abstract This paper aresses Infinitesimal Perturbation

More information

The Press-Schechter mass function

The Press-Schechter mass function The Press-Schechter mass function To state the obvious: It is important to relate our theories to what we can observe. We have looke at linear perturbation theory, an we have consiere a simple moel for

More information

Lie symmetry and Mei conservation law of continuum system

Lie symmetry and Mei conservation law of continuum system Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive

More information

The total derivative. Chapter Lagrangian and Eulerian approaches

The total derivative. Chapter Lagrangian and Eulerian approaches Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function

More information

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS

ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS ALGEBRAIC AND ANALYTIC PROPERTIES OF ARITHMETIC FUNCTIONS MARK SCHACHNER Abstract. When consiere as an algebraic space, the set of arithmetic functions equippe with the operations of pointwise aition an

More information

Summary: Differentiation

Summary: Differentiation Techniques of Differentiation. Inverse Trigonometric functions The basic formulas (available in MF5 are: Summary: Differentiation ( sin ( cos The basic formula can be generalize as follows: Note: ( sin

More information

Final Exam Study Guide and Practice Problems Solutions

Final Exam Study Guide and Practice Problems Solutions Final Exam Stuy Guie an Practice Problems Solutions Note: These problems are just some of the types of problems that might appear on the exam. However, to fully prepare for the exam, in aition to making

More information

The maximum sustainable yield of Allee dynamic system

The maximum sustainable yield of Allee dynamic system Ecological Moelling 154 (2002) 1 7 www.elsevier.com/locate/ecolmoel The maximum sustainable yiel of Allee ynamic system Zhen-Shan Lin a, *, Bai-Lian Li b a Department of Geography, Nanjing Normal Uni ersity,

More information

SYNCHRONOUS SEQUENTIAL CIRCUITS

SYNCHRONOUS SEQUENTIAL CIRCUITS CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents

More information

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies

Laplacian Cooperative Attitude Control of Multiple Rigid Bodies Laplacian Cooperative Attitue Control of Multiple Rigi Boies Dimos V. Dimarogonas, Panagiotis Tsiotras an Kostas J. Kyriakopoulos Abstract Motivate by the fact that linear controllers can stabilize the

More information

The Sokhotski-Plemelj Formula

The Sokhotski-Plemelj Formula hysics 24 Winter 207 The Sokhotski-lemelj Formula. The Sokhotski-lemelj formula The Sokhotski-lemelj formula is a relation between the following generalize functions (also calle istributions), ±iǫ = iπ(),

More information

Schrödinger s equation.

Schrödinger s equation. Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of

More information

4.2 First Differentiation Rules; Leibniz Notation

4.2 First Differentiation Rules; Leibniz Notation .. FIRST DIFFERENTIATION RULES; LEIBNIZ NOTATION 307. First Differentiation Rules; Leibniz Notation In this section we erive rules which let us quickly compute the erivative function f (x) for any polynomial

More information

Quantum Stochastic Walks: A Generalization of Classical Random Walks and Quantum Walks

Quantum Stochastic Walks: A Generalization of Classical Random Walks and Quantum Walks Quantum Stochastic Walks: A Generalization of Classical Ranom Walks an Quantum Walks The Harvar community has mae this article openly available. Please share how this access benefits you. Your story matters

More information

Application of Measurement System R&R Analysis in Ultrasonic Testing

Application of Measurement System R&R Analysis in Ultrasonic Testing 17th Worl Conference on Nonestructive Testing, 5-8 Oct 8, Shanghai, China Alication of Measurement System & Analysis in Ultrasonic Testing iao-hai ZHANG, Bing-ya CHEN, Yi ZHU Deartment of Testing an Control

More information

How the potentials in different gauges yield the same retarded electric and magnetic fields

How the potentials in different gauges yield the same retarded electric and magnetic fields How the potentials in ifferent gauges yiel the same retare electric an magnetic fiels José A. Heras a Departamento e Física, E. S. F. M., Instituto Politécnico Nacional, México D. F. México an Department

More information

Lower bounds on Locality Sensitive Hashing

Lower bounds on Locality Sensitive Hashing Lower bouns on Locality Sensitive Hashing Rajeev Motwani Assaf Naor Rina Panigrahy Abstract Given a metric space (X, X ), c 1, r > 0, an p, q [0, 1], a istribution over mappings H : X N is calle a (r,

More information

Applications of First Order Equations

Applications of First Order Equations Applications of First Orer Equations Viscous Friction Consier a small mass that has been roppe into a thin vertical tube of viscous flui lie oil. The mass falls, ue to the force of gravity, but falls more

More information

CONTROL CHARTS FOR VARIABLES

CONTROL CHARTS FOR VARIABLES UNIT CONTOL CHATS FO VAIABLES Structure.1 Introuction Objectives. Control Chart Technique.3 Control Charts for Variables.4 Control Chart for Mean(-Chart).5 ange Chart (-Chart).6 Stanar Deviation Chart

More information

INFLUENCE OF SURFACE ROUGHNESS THROUGH A SERIES OF FLOW FACTORS ON THE PERFORMANCE OF A LONGITUDINALLY ROUGH FINITE SLIDER BEARING

INFLUENCE OF SURFACE ROUGHNESS THROUGH A SERIES OF FLOW FACTORS ON THE PERFORMANCE OF A LONGITUDINALLY ROUGH FINITE SLIDER BEARING ANNALS of Faculty Engineering Huneoara International Journal of Engineering Tome XIV [2016] Fascicule 2 [May] ISSN: 1584-2665 [print; online] ISSN: 1584-2673 [CD-Rom; online] a free-accessmultiisciplinarypublication

More information

Generation of Rainfall Intensity Duration Frequency (IDF) Curves for Ungauged Sites in Arid Region

Generation of Rainfall Intensity Duration Frequency (IDF) Curves for Ungauged Sites in Arid Region Earth Syst Environ (17) 1:8 DOI.07/s41748-017-0008-8 ORIGINAL ARTICLE Generation of Rainfall Intensity Duration Frequency (IDF) Curves for Ungauged Sites in Arid Region Nassir S. Al-Amri 1 Ali M. Subyani

More information

Laplace s Equation in Cylindrical Coordinates and Bessel s Equation (II)

Laplace s Equation in Cylindrical Coordinates and Bessel s Equation (II) Laplace s Equation in Cylinrical Coorinates an Bessel s Equation (II Qualitative properties of Bessel functions of first an secon kin In the last lecture we foun the expression for the general solution

More information