mslumped-parameter (zero-dimensions!) groundwater model of Bangladesh
|
|
- Amos Phelps
- 5 years ago
- Views:
Transcription
1 mslumed-pmete (zeo-dimensions!) goundwte model of Bngldesh You gol in this oblem set is to develo bucket model fo the hydology of ou study site in Bngldesh. Using this model, you will investigte how the develoment of dy-seson iigted gicultue in Bngldesh my hve ffected its goundwte hydology. Figue 1 is concetul eesenttion of ou study site. We e inteested in modeling the hydology of the sndy quife, which undelies ou entie study site nd is confined by eltively imemeble cly lye. The fction of the quife e coveed by ech of the onds (f ), ice fields (f g ), nd ives (f ) is: f =0.1 f =0.02 f g =0.65 H, H, H efe to the heds of the quife, ond, nd ive esectively. In this model, you cn ssume tht tees t ou site hve shllow oots tht do not extend ll the wy into the quife. So, by efeence to Figue 1, ET tee, which is the flux out of the quife due tee tnsition, is equl to zeo. The couled equtions fo the tes of chnge of H nd H e: dh = k * ( H H ) E Eqution 1 dh S * = f * k * ( H H ) + f * k * ( H H ) qi Eqution 2 In Eqution 1, E is the te of evotion fom the ond e unit ond e. In Eqution 2, q i is the net flux out of the quife esulting fom the iigtion of ice fields, e unit quife e. The following questions will hel you develo models fo E nd q i. The sediments between the ond nd quife hve conductnce of k =0.01 dy -1. The sediments ccumulted t the ive bottom hve highe conductnce of k =0.1 dy -1. The stotivity (S) of the quife is S=0.01. The units of [Length/Time]. dh nd dh e Figue 1 The heds in the ives t ou site e contolled by the wte levels in the Gnges ive, nd e not ffected by the quife hed. So, the evolution of H duing the dy seson is indeendent of H. Field dt fo H s function of time e lotted in ed in Figue 2. 1
2 Figue 2: Dt on Aquife (geen nd bown), Rive (ed), nd Pond (blue) heds t ou study site. Assume tht the only significnt flows into nd out of the quife occu duing the dy seson, since duing the iny seson (lso efeed to s the monsoon seson o the flooding seson), the heds of the quife, ives nd onds e equl so tht no flows occu between them. You gol is to model the evolution of H nd H ove the dution of the dy seson. Bsed on Figue 2, the dy seson extends oximtely between Novembe 1 st nd My 31 st. At its beginning, following the flooding seson, the heds in the ives, onds, nd quife e ll t 4m. The following execises nd questions will guide you though develoing you model nd undestnding you esults. ) The ive hed, H, ffects the quife hed H (see Eqution 2). Howeve, H itself isn t ffected by H since the Gnges Rive contols it. We will wok with H s known inut into Eqution 2. This cn be done by secifying the vlues of H t diffeent times in the dy seson bsed on collected field dt (Figue 2). Altentively, we cn use simlified eesenttion of the H dt shown in Figue 2 by modeling H (t) s Sine function of time t, so tht the esulting function esembles the collected dt. t H = H m * Sin * π + π + 4 Eqution 3 (in metes) tsn H m is the mlitude of H (t), H m = 2.5 m tsn is the dution of the dy seson. 1. Check tht this eqution fo H (t) gives oite vlues of H fo t=0, t=tsn, nd t=0.5*(tsn). t 2. Show tht nothe equivlent eqution fo H (t) is H = H m * Sin * π + 4 (in metes). tsn b) Evotion t ou study site cn be modeled with efeence to the evotion t the neest meteoologicl sttion in Munshigonj (with the cystl bll). Figue 3 shows the estimted evotion t Munshigonj, which will be efeed to s the efeence evotion (Eo). Eo is usully 2
3 exessed s flow e unit e of the evoting sufce with units of [Length/Time]. In Figue 3, the units of Eo e mm/month. Figue 3 Eo dt is collected egully nd elibly, so it is useful to estimte evotion t ou site in eltion to Eo. The ctul evotion te of the onds t ou site (e unit ond e) cn be modeled s E = C *E o C is coefficient estimted emiiclly, by collecting field dt on the evotion tes of the onds nd elting them to E o. C ws found to be 1.4. Similly, the ctul tnsition te of ice lnts in the gicultul fields t ou site (e unit field e) cn be modeled s E g = C g *E o. C g ws found to be 1.1. Using dt fom Figue 3, estimte the men vlue of E o duing the dy seson. You will need to convet you esult into units of metes/dy, since it will be n inut into you equtions fo dh / nd dh /. c) Assume tht the fmes um out wte fom the quife to iigte thei ice fields t te. The ice co tnsies some of the wte lied to the fields, nd the est ecoltes bck though the cly lye into the quife. 1- If you ignoe the lg between the times when wte is lied to the fields nd when it eches the quife, wht is the net flux out of the quife tht esults fom iigtion (lbeled q i in the eqution fo dh /)? Use the eqution fo E g in t (b) to exess q i in tems of known quntities. Mke sue you exess it e unit quife e, since it will be one of the fluxes in Eqution 2 tht detemine dh /. 2- Figue 2 shows tht the fmes do not iigte thei cos duing the entie dy seson. Wite simle model fo q i (t), using you nswe to t (c) nd infomtion on the stt nd end of the iigting eiod fom Figue 2. 3
4 d) Code the system of equtions fo dh / nd dh / into Mtlb function M-file, which defines you diffeentil equtions nd is n inut file fo the ode45 function. The quife hed nd ond hed should be the only unknowns in you equtions, in ddition to you indeendent vible t. Mke sue you define ll othe vibles nd metes you include in you equtions. Solve fo you quife nd ond heds using the ode45 function. ode45 oututs the solutions (H (t) nd H (t)), s well s the vecto of time oints (t) fo which H nd H e solved. Click on the button Woksce on the left side of you Mtlb window to see these oututs (Figue 4). Figue 4 In the Woksce window, double click on the vecto of time oints nd on the mtix of heds to see thei vlues. Wht e the two columns of the hed mtix? 1- Plot the ode45 solutions fo H (t) nd H (t). Figue out how to lot H (t) setely: to etieve the vlues fo H (t) setely fom the hed mtix outut by ode45, you need to secify which ows nd which column of the hed mtix you e inteested in. 2- Ovely on you lot of H (t) nd H (t) the lot fo ive hed H (t). To do this, you will need to e-define the eqution fo H (t) t the commnd omt, even though you ve defined it in you initil function M-file. This is becuse ny vible o mete you define in you function M-file is intenl to tht function. The only oututs into you Woksce e the ode45 solutions, i.e. you quife nd ond heds nd the vecto of time oints t. Confim tht once you define H t the commnd omt, it shows u in you Woksce. How mny ows does the H vecto hve? Why? To ovely the H (t) cuve on to of you lot fo H (t) nd H (t), tye hold on t the commnd omt befoe enteing the lot (t,h) commnd. e) Inteet you esulting lot. How does the onset of iigtion ffect H (t), H (t) nd H (t)? Come you lot to the dt esented in Figue 2. 4
5 f) Think bout how you might imove you model so tht it bette eflects the conditions t ou study site. As you elbote you model, un it nd lot the solutions fo H (t) nd H (t), then ovely the cuve fo H (t). See if you modifictions to the model oduce esults tht gee bette with the dt in Figue 2. Below e coule of suggestions fo imoving you model. The fist suggested modifiction is equied, the second is otionl, nd you cn come u with othe ossible modifictions. If you hve n ide fo imoving you model, Hnn cn hel you with the coding. 1- In t b, you secified E o to be constnt vlue equl to the vege vlue of E o ove the dy seson. Bsed on the dt in Figue 3, fomulte bette model fo E o (t) nd code it into you function M-file. 2- (OPTIONAL, but oduces nice esults) The q i flux you descibed in (c-1) is the mximum flux when ll the ice fields e being iigted. Howeve, this mximum flux isn t mintined duing the whole iigting eiod, since mny fields e iigted fo only otion of this eiod. To ccount fo this, include fcto i in you eqution fo dh /, which multilies q i nd secifies the fction of gicultul e tht is ctully iigted t ny time t. Define i (t) s Sine function of t, vying fom 0.5 t the stt of the iigting eiod, to 1 in the middle of this eiod, nd bck to 0.5 t its end. This model fo i (t) imlies tht hlf the ice fields e ctully iigted initilly, nd this fction inceses with time until ll the fields e being iigted, nd then oceeds to decline bck to 0.5 t the end of the iigting eiod. i (t) must be secified s zeo outside the iigting eiod. Refe to (c-2) fo infomtion on the extent of the iigting eiod, nd to t () to emind youself how to model vible s Sine function of time. g) So f, you ve been looking t the solutions fo the quife nd ond heds. These e evolving in time due to the fluxes between the diffeent wte bodies. In the next few questions you will be investigting these fluxes. 1- Define the eqution fo FluxP(t), the flux between the quife nd the ond e unit e of quife. In you eqution, when is the esult fo FluxP ositive, nd would tht imly echge to o dischge fom the quife? If needed, djust the signs in you eqution so tht ositive FluxP indictes echge to the quife, i.e. flow fom the ond to the quife. 2- Similly, define the eqution fo FluxR(t), the flux between the quife nd the ive e unit e of quife. In you eqution, when is FluxR ositive, nd would tht imly echge to o dischge fom the quife? If needed, djust the signs in you eqution so tht ositive FluxR indictes echge to the quife. 3- Cete new Mtlb M-file, in which you code the equtions fo FluxP(t) nd FluxR(t). Mke sue you nme the vibles defined by these equtions: FluxP nd FluxR (you ll soon see why this is necessy). You will be unning this scit fte you un ode45, so it will use the solutions fo H (t) nd H (t) tht ode45 oduces. As in t (d-1), to etieve the solutions fo H (t) setely, you need to secify which ows nd which column of you outut hed mtix you e inteested in. Similly fo H (t). You scit will lso use the vecto of t vlues (time oints) oduced by ode45. Remembe tht you need to define ny othe metes o vibles used in you equtions fo FluxP(t) nd FluxR(t) (such s H, k, k, f nd f ), even though you ve defined them in you initil function M-file. This is becuse these vibles nd metes e intenl to you function, nd so en t sved by Mtlb into you Woksce when you un ode45 (this is exlined in t d). 5
6 4- The net flux out of the quife due to iigtion, e unit quife e, is FluxI(t)= i (t)*q i (t) o simly q i (t), deending on whethe o not you comleted the otionl t (f-2). Add the eqution fo FluxI(t) to you new M-file. Nme the vible defined by this eqution: FluxI. Remembe you will need to define ny vible o mete you use in this eqution tht is not n outut of ode45. Use the models fo q i (t) nd E o (t) tht you ceted in ts (c-2) nd (f-1), esectively. Since q i (t) nd E o (t) hve diffeent vlues deending on the time eiod (fo exmle, q i (t) is zeo outside of the iigting eiod), you need fo loo tht secifies these vibles fo evey time oint in the t vecto outut by ode45. Instuctions to hel you wite the code fo FluxI(t) e vilble on stell unde Mteils, in the document FluxI.doc. Does you eqution oduce ositive o negtive vlues fo FluxI(t)? Does FluxI(t) constitute dischge fom o echge to the quife? i) Run you new scit by tying its filenme t the commnd omt, to obtin solutions fo FluxP(t), FluxR(t), nd FluxI(t). Remembe tht FluxP(t) nd FluxR(t) e functions of H (t) nd H (t), so you need to hve un ode45 fist to obtin the solutions fo the quife nd ond heds. Plot these fluxes nd inteet you esults. Note esecilly chnges in sign in FluxP(t) nd FluxR(t). Wht do they men? Ae they consistent with you lot fo H (t), H (t) nd H (t)? Also inteet chnges in the sloes of these flux cuves. j) Fom the Mteils section of the stell website, downlod the Mtlb scit TotlFluxes.m nd sve it into you cuent diectoy, whee you e sving you othe scits. Run it to obtin solutions fo the vibles: totldischgep, totlechgep, totldischger, totlechger, nd totldischgei. The TotlFluxes.m scit uses you esults fo FluxP(t), FluxR(t), nd FluxI(t). Tht is why you hd to give secific nmes to the vectos contining the solutions fo these fluxes. The TotlFluxes.m scit integtes these fluxes ove the dution of the dy seson to comute the vibles: totldischgep: The totl dischge fom the quife to the ond e unit quife e ove the dy seson. totlechgep: The totl echge fom the ond to the quife e unit quife e ove the dy seson. totldischger: The totl dischge fom the quife to the ive e unit quife e ove the dy seson. totlechger: The totl echge fom the ive to the quife e unit quife e ove the dy seson. totldischgei: The totl flow out of the quife due to iigtion e unit quife e ove the dy seson. Once you un the scit, Mtlb sves these vibles nd thei vlues into you Woksce. Confim tht the vibles eesenting flows out of the quife hve negtive vlues, while those eesenting flows into the quife hve ositive vlues. 1- Wht is the totl flow out of the quife e unit quife e ove the dy seson? Wht is the totl flow into the quife e unit quife e ove the dy seson? 2- Wht is the net chnge in quife hed ove the dy seson (efe to you lot fo H, H, nd H o lot H (t) gin)? Given tht S=0.01, wht chnge in volume of wte e unit quife e does this coesond to? 3- Bsed on you nswes to (j-1) nd (j-2): does you model fo the quife hed conseve mss? 6
7 k) The quife t ou study site hs deth D=100m, nd vege oosity Ө = 0.25 (25%). 1- Wht is the volume of wte contined in the quife? 2- Assume tht ove ye, the only flows into nd out of the quife t ou site occu duing the dy seson. Using you nswes to (j-1) nd (k-1), clculte the esidence time of wte in the quife. If you find tht the totl outflows fom nd inflows into the quife e not equivlent, tke thei vege. l) Use you model to figue out how the quife s wte budget ws chnged s esult of the develoment of iigted gicultue in Bngldesh. 1- Adjust you model so tht no wte is extcted fom the quife fo iigtion. You cn do this by chnging the vlue of f g to 0 in you initil function M-file tht defines you system of equtions fo dh / nd dh /. 2- Run ode45, nd lot H (t) nd H (t). Ovely the lot of H (t). Come you lot fo H (t), H (t) nd H (t) in the bsence iigted gicultue to the lot of these heds tht you oduced when you ccounted fo iigtion in you model. 3- Run the M-file scit you wote tht solves fo FluxP(t), FluxR(t), nd FluxI(t). Plot these fluxes. Agin, come these esults, in the bsence of iigtion, to the esults of the model in which you ccounted fo iigtion. 4- Run the scit you downloded, TotlFluxes.m. Comute the esidence time of wte in the quife in the bsence of uming fo iigtion. Come it to the esidence time tht you comuted in (k-2). 7
Language Processors F29LP2, Lecture 5
Lnguge Pocessos F29LP2, Lectue 5 Jmie Gy Feuy 2, 2014 1 / 1 Nondeteministic Finite Automt (NFA) NFA genelise deteministic finite utomt (DFA). They llow sevel (0, 1, o moe thn 1) outgoing tnsitions with
More information4.2 Boussinesq s Theory. Contents
00477 Pvement Stuctue 4. Stesses in Flexible vement Contents 4. Intoductions to concet of stess nd stin in continuum mechnics 4. Boussinesq s Theoy 4. Bumiste s Theoy 4.4 Thee Lye System Weekset Sung Chte
More informationHomework 3 MAE 118C Problems 2, 5, 7, 10, 14, 15, 18, 23, 30, 31 from Chapter 5, Lamarsh & Baratta. The flux for a point source is:
. Homewok 3 MAE 8C Poblems, 5, 7, 0, 4, 5, 8, 3, 30, 3 fom Chpte 5, msh & Btt Point souces emit nuetons/sec t points,,, n 3 fin the flux cuent hlf wy between one sie of the tingle (blck ot). The flux fo
More informationPreviously. Extensions to backstepping controller designs. Tracking using backstepping Suppose we consider the general system
436-459 Advnced contol nd utomtion Extensions to bckstepping contolle designs Tcking Obseves (nonline dmping) Peviously Lst lectue we looked t designing nonline contolles using the bckstepping technique
More information10 m, so the distance from the Sun to the Moon during a solar eclipse is. The mass of the Sun, Earth, and Moon are = =
Chpte 1 nivesl Gvittion 11 *P1. () The un-th distnce is 1.4 nd the th-moon 8 distnce is.84, so the distnce fom the un to the Moon duing sol eclipse is 11 8 11 1.4.84 = 1.4 The mss of the un, th, nd Moon
More informationWeek 8. Topic 2 Properties of Logarithms
Week 8 Topic 2 Popeties of Logithms 1 Week 8 Topic 2 Popeties of Logithms Intoduction Since the esult of ithm is n eponent, we hve mny popeties of ithms tht e elted to the popeties of eponents. They e
More informationOptimization. x = 22 corresponds to local maximum by second derivative test
Optimiztion Lectue 17 discussed the exteme vlues of functions. This lectue will pply the lesson fom Lectue 17 to wod poblems. In this section, it is impotnt to emembe we e in Clculus I nd e deling one-vible
More informationRadial geodesics in Schwarzschild spacetime
Rdil geodesics in Schwzschild spcetime Spheiclly symmetic solutions to the Einstein eqution tke the fom ds dt d dθ sin θdϕ whee is constnt. We lso hve the connection components, which now tke the fom using
More informationSPA7010U/SPA7010P: THE GALAXY. Solutions for Coursework 1. Questions distributed on: 25 January 2018.
SPA7U/SPA7P: THE GALAXY Solutions fo Cousewok Questions distibuted on: 25 Jnuy 28. Solution. Assessed question] We e told tht this is fint glxy, so essentilly we hve to ty to clssify it bsed on its spectl
More informationTopics for Review for Final Exam in Calculus 16A
Topics fo Review fo Finl Em in Clculus 16A Instucto: Zvezdelin Stnkov Contents 1. Definitions 1. Theoems nd Poblem Solving Techniques 1 3. Eecises to Review 5 4. Chet Sheet 5 1. Definitions Undestnd the
More informationRELATIVE KINEMATICS. q 2 R 12. u 1 O 2 S 2 S 1. r 1 O 1. Figure 1
RELAIVE KINEMAICS he equtions of motion fo point P will be nlyzed in two diffeent efeence systems. One efeence system is inetil, fixed to the gound, the second system is moving in the physicl spce nd the
More information( ) D x ( s) if r s (3) ( ) (6) ( r) = d dr D x
SIO 22B, Rudnick dpted fom Dvis III. Single vile sttistics The next few lectues e intended s eview of fundmentl sttistics. The gol is to hve us ll speking the sme lnguge s we move to moe dvnced topics.
More informationQuality control. Final exam: 2012/1/12 (Thur), 9:00-12:00 Q1 Q2 Q3 Q4 Q5 YOUR NAME
Qulity contol Finl exm: // (Thu), 9:-: Q Q Q3 Q4 Q5 YOUR NAME NOTE: Plese wite down the deivtion of you nswe vey clely fo ll questions. The scoe will be educed when you only wite nswe. Also, the scoe will
More information9.4 The response of equilibrium to temperature (continued)
9.4 The esponse of equilibium to tempetue (continued) In the lst lectue, we studied how the chemicl equilibium esponds to the vition of pessue nd tempetue. At the end, we deived the vn t off eqution: d
More informationFI 2201 Electromagnetism
FI 1 Electomgnetism Alexnde A. Isknd, Ph.D. Physics of Mgnetism nd Photonics Resech Goup Electosttics ELECTRIC PTENTIALS 1 Recll tht we e inteested to clculte the electic field of some chge distiution.
More informationClass Summary. be functions and f( D) , we define the composition of f with g, denoted g f by
Clss Summy.5 Eponentil Functions.6 Invese Functions nd Logithms A function f is ule tht ssigns to ech element D ectly one element, clled f( ), in. Fo emple : function not function Given functions f, g:
More informationLecture 10. Solution of Nonlinear Equations - II
Fied point Poblems Lectue Solution o Nonline Equtions - II Given unction g : R R, vlue such tht gis clled ied point o the unction g, since is unchnged when g is pplied to it. Whees with nonline eqution
More information(a) Counter-Clockwise (b) Clockwise ()N (c) No rotation (d) Not enough information
m m m00 kg dult, m0 kg bby. he seesw stts fom est. Which diection will it ottes? ( Counte-Clockwise (b Clockwise ( (c o ottion ti (d ot enough infomtion Effect of Constnt et oque.3 A constnt non-zeo toque
More informationWeek 10: DTMC Applications Ranking Web Pages & Slotted ALOHA. Network Performance 10-1
Week : DTMC Alictions Rnking Web ges & Slotted ALOHA etwok efonce - Outline Aly the theoy of discete tie Mkov chins: Google s nking of web-ges Wht ge is the use ost likely seching fo? Foulte web-gh s Mkov
More information1 Using Integration to Find Arc Lengths and Surface Areas
Novembe 9, 8 MAT86 Week Justin Ko Using Integtion to Find Ac Lengths nd Sufce Aes. Ac Length Fomul: If f () is continuous on [, b], then the c length of the cuve = f() on the intevl [, b] is given b s
More informationNS-IBTS indices calculation procedure
ICES Dt Cente DATRAS 1.1 NS-IBTS indices 2013 DATRAS Pocedue Document NS-IBTS indices clcultion pocedue Contents Genel... 2 I Rw ge dt CA -> Age-length key by RFA fo defined ge nge ALK... 4 II Rw length
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 3 Due on Sep. 14, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More information7.5-Determinants in Two Variables
7.-eteminnts in Two Vibles efinition of eteminnt The deteminnt of sque mti is el numbe ssocited with the mti. Eve sque mti hs deteminnt. The deteminnt of mti is the single ent of the mti. The deteminnt
More informationCHAPTER 18: ELECTRIC CHARGE AND ELECTRIC FIELD
ollege Physics Student s Mnul hpte 8 HAPTR 8: LTRI HARG AD LTRI ILD 8. STATI LTRIITY AD HARG: OSRVATIO O HARG. ommon sttic electicity involves chges nging fom nnocoulombs to micocoulombs. () How mny electons
More informationThe Area of a Triangle
The e of Tingle tkhlid June 1, 015 1 Intodution In this tile we will e disussing the vious methods used fo detemining the e of tingle. Let [X] denote the e of X. Using se nd Height To stt off, the simplest
More informationFluids & Bernoulli s Equation. Group Problems 9
Goup Poblems 9 Fluids & Benoulli s Eqution Nme This is moe tutoil-like thn poblem nd leds you though conceptul development of Benoulli s eqution using the ides of Newton s 2 nd lw nd enegy. You e going
More informationThis immediately suggests an inverse-square law for a "piece" of current along the line.
Electomgnetic Theoy (EMT) Pof Rui, UNC Asheville, doctophys on YouTube Chpte T Notes The iot-svt Lw T nvese-sque Lw fo Mgnetism Compe the mgnitude of the electic field t distnce wy fom n infinite line
More informationAnswers to test yourself questions
Answes to test youself questions opic Descibing fields Gm Gm Gm Gm he net field t is: g ( d / ) ( 4d / ) d d Gm Gm Gm Gm Gm Gm b he net potentil t is: V d / 4d / d 4d d d V e 4 7 9 49 J kg 7 7 Gm d b E
More informationPhysics 505 Fall 2005 Midterm Solutions. This midterm is a two hour open book, open notes exam. Do all three problems.
Physics 55 Fll 5 Midtem Solutions This midtem is two hou open ook, open notes exm. Do ll thee polems. [35 pts] 1. A ectngul ox hs sides of lengths, nd c z x c [1] ) Fo the Diichlet polem in the inteio
More informationπ,π is the angle FROM a! TO b
Mth 151: 1.2 The Dot Poduct We hve scled vectos (o, multiplied vectos y el nume clled scl) nd dded vectos (in ectngul component fom). Cn we multiply vectos togethe? The nswe is YES! In fct, thee e two
More informationGeneral Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface
Genel Physics II Chpte 3: Guss w We now wnt to quickly discuss one of the moe useful tools fo clculting the electic field, nmely Guss lw. In ode to undestnd Guss s lw, it seems we need to know the concept
More informationChapter 7. Kleene s Theorem. 7.1 Kleene s Theorem. The following theorem is the most important and fundamental result in the theory of FA s:
Chpte 7 Kleene s Theoem 7.1 Kleene s Theoem The following theoem is the most impotnt nd fundmentl esult in the theoy of FA s: Theoem 6 Any lnguge tht cn e defined y eithe egul expession, o finite utomt,
More informationU>, and is negative. Electric Potential Energy
Electic Potentil Enegy Think of gvittionl potentil enegy. When the lock is moved veticlly up ginst gvity, the gvittionl foce does negtive wok (you do positive wok), nd the potentil enegy (U) inceses. When
More information10 Statistical Distributions Solutions
Communictions Engineeing MSc - Peliminy Reding 1 Sttisticl Distiutions Solutions 1) Pove tht the vince of unifom distiution with minimum vlue nd mximum vlue ( is ) 1. The vince is the men of the sques
More informationSection 35 SHM and Circular Motion
Section 35 SHM nd Cicul Motion Phsics 204A Clss Notes Wht do objects do? nd Wh do the do it? Objects sometimes oscillte in simple hmonic motion. In the lst section we looed t mss ibting t the end of sping.
More informationA CYLINDRICAL CONTACT MODEL FOR TWO DIMENSIONAL MULTIASPERITY PROFILES
Poceedings of 003 STLE/ASME Intentionl Joint Tibology Confeence Ponte Ved Bech, loid USA, Octobe 6 9, 003 003TIB-69 A CYLINDICAL CONTACT MODEL O TWO DIMENSIONAL MULTIASPEITY POILES John J. Jgodnik nd Sinn
More informationKepler s problem gravitational attraction
Kele s oblem gavitational attaction Summay of fomulas deived fo two-body motion Let the two masses be m and m. The total mass is M = m + m, the educed mass is µ = m m /(m + m ). The gavitational otential
More informationSolutions to Midterm Physics 201
Solutions to Midtem Physics. We cn conside this sitution s supeposition of unifomly chged sphee of chge density ρ nd dius R, nd second unifomly chged sphee of chge density ρ nd dius R t the position of
More informationSchool of Electrical and Computer Engineering, Cornell University. ECE 303: Electromagnetic Fields and Waves. Fall 2007
School of Electicl nd Compute Engineeing, Conell Univesity ECE 303: Electomgnetic Fields nd Wves Fll 007 Homewok 4 Due on Sep. 1, 007 by 5:00 PM Reding Assignments: i) Review the lectue notes. ii) Relevnt
More informationMark Scheme (Results) January 2008
Mk Scheme (Results) Jnuy 00 GCE GCE Mthemtics (6679/0) Edecel Limited. Registeed in Englnd nd Wles No. 4496750 Registeed Office: One90 High Holbon, London WCV 7BH Jnuy 00 6679 Mechnics M Mk Scheme Question
More informationChapter 6 Notes, Larson/Hostetler 3e
Contents 6. Antiderivtives nd the Rules of Integrtion.......................... 6. Are nd the Definite Integrl.................................. 6.. Are............................................ 6. Reimnn
More informationOnline-routing on the butterfly network: probabilistic analysis
Online-outing on the buttefly netwok: obabilistic analysis Andey Gubichev 19.09.008 Contents 1 Intoduction: definitions 1 Aveage case behavio of the geedy algoithm 3.1 Bounds on congestion................................
More informationSTD: XI MATHEMATICS Total Marks: 90. I Choose the correct answer: ( 20 x 1 = 20 ) a) x = 1 b) x =2 c) x = 3 d) x = 0
STD: XI MATHEMATICS Totl Mks: 90 Time: ½ Hs I Choose the coect nswe: ( 0 = 0 ). The solution of is ) = b) = c) = d) = 0. Given tht the vlue of thid ode deteminnt is then the vlue of the deteminnt fomed
More informationOn the Eötvös effect
On the Eötvös effect Mugu B. Răuţ The im of this ppe is to popose new theoy bout the Eötvös effect. We develop mthemticl model which loud us bette undestnding of this effect. Fom the eqution of motion
More informationFamilies of Solutions to Bernoulli ODEs
In the fmily of solutions to the differentil eqution y ry dx + = it is shown tht vrition of the initil condition y( 0 = cuses horizontl shift in the solution curve y = f ( x, rther thn the verticl shift
More informationTwo dimensional polar coordinate system in airy stress functions
I J C T A, 9(9), 6, pp. 433-44 Intentionl Science Pess Two dimensionl pol coodinte system in iy stess functions S. Senthil nd P. Sek ABSTRACT Stisfy the given equtions, boundy conditions nd bihmonic eqution.in
More informationAlgebra Based Physics. Gravitational Force. PSI Honors universal gravitation presentation Update Fall 2016.notebookNovember 10, 2016
Newton's Lw of Univesl Gvittion Gvittionl Foce lick on the topic to go to tht section Gvittionl Field lgeb sed Physics Newton's Lw of Univesl Gvittion Sufce Gvity Gvittionl Field in Spce Keple's Thid Lw
More informationPhysics 111. Uniform circular motion. Ch 6. v = constant. v constant. Wednesday, 8-9 pm in NSC 128/119 Sunday, 6:30-8 pm in CCLIR 468
ics Announcements dy, embe 28, 2004 Ch 6: Cicul Motion - centipetl cceletion Fiction Tension - the mssless sting Help this week: Wednesdy, 8-9 pm in NSC 128/119 Sundy, 6:30-8 pm in CCLIR 468 Announcements
More informationEECE 260 Electrical Circuits Prof. Mark Fowler
EECE 60 Electicl Cicuits Pof. Mk Fowle Complex Numbe Review /6 Complex Numbes Complex numbes ise s oots of polynomils. Definition of imginy # nd some esulting popeties: ( ( )( ) )( ) Recll tht the solution
More informationSt Andrew s Academy Mathematics Department Higher Mathematics VECTORS
St ndew s cdemy Mthemtics etment Highe Mthemtics VETORS St ndew's cdemy Mths et 0117 1 Vectos sics 1. = nd = () Sketch the vectos nd. () Sketch the vectos nd. (c) Given u = +, sketch the vecto u. (d) Given
More informationn f(x i ) x. i=1 In section 4.2, we defined the definite integral of f from x = a to x = b as n f(x i ) x; f(x) dx = lim i=1
The Fundmentl Theorem of Clculus As we continue to study the re problem, let s think bck to wht we know bout computing res of regions enclosed by curves. If we wnt to find the re of the region below the
More informationAP Calculus AB Exam Review Sheet B - Session 1
AP Clcls AB Em Review Sheet B - Session Nme: AP 998 # Let e the nction given y e.. Find lim nd lim.. Find the solte minimm vle o. Jstiy tht yo nswe is n solte minimm. c. Wht is the nge o? d. Conside the
More information4 7x =250; 5 3x =500; Read section 3.3, 3.4 Announcements: Bell Ringer: Use your calculator to solve
Dte: 3/14/13 Objective: SWBAT pply properties of exponentil functions nd will pply properties of rithms. Bell Ringer: Use your clcultor to solve 4 7x =250; 5 3x =500; HW Requests: Properties of Log Equtions
More informationInternational Journal of Pure and Applied Sciences and Technology
Int. J. Pue l. Sci. Technol. () (0). -6 Intentionl Jounl of Pue nd lied Sciences nd Technology ISSN 9-607 vilble online t www.ijost.in Resech Pe Rdil Vibtions in Mico-Isotoic Mico-Elstic Hollow Shee R.
More informationDIRECT CURRENT CIRCUITS
DRECT CURRENT CUTS ELECTRC POWER Consider the circuit shown in the Figure where bttery is connected to resistor R. A positive chrge dq will gin potentil energy s it moves from point to point b through
More informationr a + r b a + ( r b + r c)
AP Phsics C Unit 2 2.1 Nme Vectos Vectos e used to epesent quntities tht e chcteized b mgnitude ( numeicl vlue with ppopite units) nd diection. The usul emple is the displcement vecto. A quntit with onl
More informationRead section 3.3, 3.4 Announcements:
Dte: 3/1/13 Objective: SWBAT pply properties of exponentil functions nd will pply properties of rithms. Bell Ringer: 1. f x = 3x 6, find the inverse, f 1 x., Using your grphing clcultor, Grph 1. f x,f
More informationDiscrete Model Parametrization
Poceedings of Intentionl cientific Confeence of FME ession 4: Automtion Contol nd Applied Infomtics Ppe 9 Discete Model Pmetition NOKIEVIČ, Pet Doc,Ing,Cc Deptment of Contol ystems nd Instumenttion, Fculty
More informationMichael Rotkowitz 1,2
Novembe 23, 2006 edited Line Contolles e Unifomly Optiml fo the Witsenhusen Counteexmple Michel Rotkowitz 1,2 IEEE Confeence on Decision nd Contol, 2006 Abstct In 1968, Witsenhusen intoduced his celebted
More informationMath 4318 : Real Analysis II Mid-Term Exam 1 14 February 2013
Mth 4318 : Rel Anlysis II Mid-Tem Exm 1 14 Febuy 2013 Nme: Definitions: Tue/Flse: Poofs: 1. 2. 3. 4. 5. 6. Totl: Definitions nd Sttements of Theoems 1. (2 points) Fo function f(x) defined on (, b) nd fo
More informationDEPARTMENT OF CIVIL AND ENVIRONMENTAL ENGINEERING FLUID MECHANICS III Solutions to Problem Sheet 3
DEPATMENT OF CIVIL AND ENVIONMENTAL ENGINEEING FLID MECHANICS III Solutions to Poblem Sheet 3 1. An tmospheic vote is moelle s combintion of viscous coe otting s soli boy with ngul velocity Ω n n iottionl
More informationProperties of Integrals, Indefinite Integrals. Goals: Definition of the Definite Integral Integral Calculations using Antiderivatives
Block #6: Properties of Integrls, Indefinite Integrls Gols: Definition of the Definite Integrl Integrl Clcultions using Antiderivtives Properties of Integrls The Indefinite Integrl 1 Riemnn Sums - 1 Riemnn
More informationElectronic Supplementary Material
Electonic Supplementy Mteil On the coevolution of socil esponsiveness nd behvioul consistency Mx Wolf, G Snde vn Doon & Fnz J Weissing Poc R Soc B 78, 440-448; 0 Bsic set-up of the model Conside the model
More informationThe Atwood Machine OBJECTIVE INTRODUCTION APPARATUS THEORY
The Atwood Mchine OBJECTIVE To derive the ening of Newton's second lw of otion s it pplies to the Atwood chine. To explin how ss iblnce cn led to the ccelertion of the syste. To deterine the ccelertion
More informationProblem Set 3 SOLUTIONS
Univesity of Albm Deptment of Physics nd Astonomy PH 10- / LeCli Sping 008 Poblem Set 3 SOLUTIONS 1. 10 points. Remembe #7 on lst week s homewok? Clculte the potentil enegy of tht system of thee chges,
More informationHomework: Study 6.2 #1, 3, 5, 7, 11, 15, 55, 57
Gols: 1. Undestnd volume s the sum of the es of n infinite nume of sufces. 2. Be le to identify: the ounded egion the efeence ectngle the sufce tht esults fom evolution of the ectngle ound n xis o foms
More informationElectric Potential. and Equipotentials
Electic Potentil nd Euipotentils U Electicl Potentil Review: W wok done y foce in going fom to long pth. l d E dl F W dl F θ Δ l d E W U U U Δ Δ l d E W U U U U potentil enegy electic potentil Potentil
More informationSo, if we are finding the amount of work done over a non-conservative vector field F r, we do that long ur r b ur =
3.4 Geen s Theoem Geoge Geen: self-taught English scientist, 793-84 So, if we ae finding the amount of wok done ove a non-consevative vecto field F, we do that long u b u 3. method Wok = F d F( () t )
More informationMultiplying and Dividing Rational Expressions
Lesson Peview Pt - Wht You ll Len To multipl tionl epessions To divide tionl epessions nd Wh To find lon pments, s in Eecises 0 Multipling nd Dividing Rtionl Epessions Multipling Rtionl Epessions Check
More informationChapter 28 Sources of Magnetic Field
Chpte 8 Souces of Mgnetic Field - Mgnetic Field of Moving Chge - Mgnetic Field of Cuent Element - Mgnetic Field of Stight Cuent-Cying Conducto - Foce Between Pllel Conductos - Mgnetic Field of Cicul Cuent
More informationChapter 21: Electric Charge and Electric Field
Chpte 1: Electic Chge nd Electic Field Electic Chge Ancient Gees ~ 600 BC Sttic electicit: electic chge vi fiction (see lso fig 1.1) (Attempted) pith bll demonsttion: inds of popeties objects with sme
More informationChapter Direct Method of Interpolation More Examples Mechanical Engineering
Chpte 5 iect Method o Intepoltion Moe Exmples Mechnicl Engineeing Exmple Fo the pupose o shinking tunnion into hub, the eduction o dimete o tunnion sht by cooling it though tempetue chnge o is given by
More informationFriedmannien equations
..6 Fiedmnnien equtions FLRW metic is : ds c The metic intevl is: dt ( t) d ( ) hee f ( ) is function which detemines globl geometic l popety of D spce. f d sin d One cn put it in the Einstein equtions
More information11.1 Balanced Three Phase Voltage Sources
BAANCED THREE- PHASE CIRCUITS C.T. Pn 1 CONTENT 11.1 Blnced Thee-Phse Voltge Souces 11.2 Blnced Thee-Phse ods 11.3 Anlysis of the Wye-WyeCicuits 11.4 Anlysis of the Wye-Delt Cicuits 11.5 Powe Clcultions
More informationOperations with Polynomials
38 Chpter P Prerequisites P.4 Opertions with Polynomils Wht you should lern: How to identify the leding coefficients nd degrees of polynomils How to dd nd subtrct polynomils How to multiply polynomils
More informationITI Introduction to Computing II
ITI 1121. Intoduction to Computing II Mcel Tucotte School of Electicl Engineeing nd Compute Science Abstct dt type: Stck Stck-bsed lgoithms Vesion of Febuy 2, 2013 Abstct These lectue notes e ment to be
More information7.2 The Definite Integral
7.2 The Definite Integrl the definite integrl In the previous section, it ws found tht if function f is continuous nd nonnegtive, then the re under the grph of f on [, b] is given by F (b) F (), where
More informationConservation Law. Chapter Goal. 5.2 Theory
Chpter 5 Conservtion Lw 5.1 Gol Our long term gol is to understnd how mny mthemticl models re derived. We study how certin quntity chnges with time in given region (sptil domin). We first derive the very
More informations c s (b) Hence, show that the entropy for rubber-like materials must have the separable form
EN: Continuum Mechnics Homewok 6: Aliction of continuum mechnics to elstic solids Due Decembe th, School of Engineeing Bown Univesity. Exeiments show tht ubbe-like mteils hve secific intenl enegy ( ) nd
More informationCHAPTER 7 Applications of Integration
CHAPTER 7 Applitions of Integtion Setion 7. Ae of Region Between Two Cuves.......... Setion 7. Volume: The Disk Method................. Setion 7. Volume: The Shell Method................ Setion 7. A Length
More informationSUMMER KNOWHOW STUDY AND LEARNING CENTRE
SUMMER KNOWHOW STUDY AND LEARNING CENTRE Indices & Logrithms 2 Contents Indices.2 Frctionl Indices.4 Logrithms 6 Exponentil equtions. Simplifying Surds 13 Opertions on Surds..16 Scientific Nottion..18
More informationELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:
LCTROSTATICS. Quntiztion of Chge: Any chged body, big o smll, hs totl chge which is n integl multile of e, i.e. = ± ne, whee n is n intege hving vlues,, etc, e is the chge of electon which is eul to.6
More informationData Structures. Element Uniqueness Problem. Hash Tables. Example. Hash Tables. Dana Shapira. 19 x 1. ) h(x 4. ) h(x 2. ) h(x 3. h(x 1. x 4. x 2.
Element Uniqueness Poblem Dt Stuctues Let x,..., xn < m Detemine whethe thee exist i j such tht x i =x j Sot Algoithm Bucket Sot Dn Shpi Hsh Tbles fo (i=;i
More informationPhysics 604 Problem Set 1 Due Sept 16, 2010
Physics 64 Polem et 1 Due ept 16 1 1) ) Inside good conducto the electic field is eo (electons in the conducto ecuse they e fee to move move in wy to cncel ny electic field impessed on the conducto inside
More informationELECTRO - MAGNETIC INDUCTION
NTRODUCTON LCTRO - MAGNTC NDUCTON Whenee mgnetic flu linked with cicuit chnges, n e.m.f. is induced in the cicuit. f the cicuit is closed, cuent is lso induced in it. The e.m.f. nd cuent poduced lsts s
More informationEnergy Dissipation Gravitational Potential Energy Power
Lectue 4 Chpte 8 Physics I 0.8.03 negy Dissiption Gvittionl Potentil negy Powe Couse wesite: http://fculty.uml.edu/andiy_dnylov/teching/physicsi Lectue Cptue: http://echo360.uml.edu/dnylov03/physicsfll.html
More information2.4 Linear Inequalities and Interval Notation
.4 Liner Inequlities nd Intervl Nottion We wnt to solve equtions tht hve n inequlity symol insted of n equl sign. There re four inequlity symols tht we will look t: Less thn , Less thn or
More information(A) 6.32 (B) 9.49 (C) (D) (E) 18.97
Univesity of Bhin Physics 10 Finl Exm Key Fll 004 Deptment of Physics 13/1/005 8:30 10:30 e =1.610 19 C, m e =9.1110 31 Kg, m p =1.6710 7 Kg k=910 9 Nm /C, ε 0 =8.8410 1 C /Nm, µ 0 =4π10 7 T.m/A Pt : 10
More informationSOLUTIONS TO CONCEPTS CHAPTER 11
SLUTINS T NEPTS HPTE. Gvittionl fce of ttction, F.7 0 0 0.7 0 7 N (0.). To clculte the gvittionl fce on t unline due to othe ouse. F D G 4 ( / ) 8G E F I F G ( / ) G ( / ) G 4G 4 D F F G ( / ) G esultnt
More information1 Probability Density Functions
Lis Yn CS 9 Continuous Distributions Lecture Notes #9 July 6, 28 Bsed on chpter by Chris Piech So fr, ll rndom vribles we hve seen hve been discrete. In ll the cses we hve seen in CS 9, this ment tht our
More informationProbabilistic Retrieval
CS 630 Lectue 4: 02/07/2006 Lectue: Lillin Lee Scibes: Pete Bbinski, Dvid Lin Pobbilistic Retievl I. Nïve Beginnings. Motivtions b. Flse Stt : A Pobbilistic Model without Vition? II. Fomultion. Tems nd
More information3.1 Magnetic Fields. Oersted and Ampere
3.1 Mgnetic Fields Oested nd Ampee The definition of mgnetic induction, B Fields of smll loop (dipole) Mgnetic fields in mtte: ) feomgnetism ) mgnetiztion, (M ) c) mgnetic susceptiility, m d) mgnetic field,
More informationLecture 3. In this lecture, we will discuss algorithms for solving systems of linear equations.
Lecture 3 3 Solving liner equtions In this lecture we will discuss lgorithms for solving systems of liner equtions Multiplictive identity Let us restrict ourselves to considering squre mtrices since one
More informationAntiderivatives Introduction
Antierivtives 0. Introuction So fr much of the term hs been sent fining erivtives or rtes of chnge. But in some circumstnces we lrey know the rte of chnge n we wish to etermine the originl function. For
More informationH5 Gas meter calibration
H5 Gas mete calibation Calibation: detemination of the elation between the hysical aamete to be detemined and the signal of a measuement device. Duing the calibation ocess the measuement equiment is comaed
More informationRiemann Integrals and the Fundamental Theorem of Calculus
Riemnn Integrls nd the Fundmentl Theorem of Clculus Jmes K. Peterson Deprtment of Biologicl Sciences nd Deprtment of Mthemticl Sciences Clemson University September 16, 2013 Outline Grphing Riemnn Sums
More informationChapter 6 Thermoelasticity
Chpte 6 Themoelsticity Intoduction When theml enegy is dded to n elstic mteil it expnds. Fo the simple unidimensionl cse of b of length L, initilly t unifom tempetue T 0 which is then heted to nonunifom
More informationImproper Integrals, and Differential Equations
Improper Integrls, nd Differentil Equtions October 22, 204 5.3 Improper Integrls Previously, we discussed how integrls correspond to res. More specificlly, we sid tht for function f(x), the region creted
More informationElectric Field F E. q Q R Q. ˆ 4 r r - - Electric field intensity depends on the medium! origin
1 1 Electic Field + + q F Q R oigin E 0 0 F E ˆ E 4 4 R q Q R Q - - Electic field intensity depends on the medium! Electic Flux Density We intoduce new vecto field D independent of medium. D E So, electic
More informationReview of Mathematical Concepts
ENEE 322: Signls nd Systems view of Mthemticl Concepts This hndout contins ief eview of mthemticl concepts which e vitlly impotnt to ENEE 322: Signls nd Systems. Since this mteil is coveed in vious couses
More information