not to be republished NCERT MATHEMATICAL MODELLING Appendix 2 A.2.1 Introduction A.2.2 Why Mathematical Modelling?

Size: px
Start display at page:

Download "not to be republished NCERT MATHEMATICAL MODELLING Appendix 2 A.2.1 Introduction A.2.2 Why Mathematical Modelling?"

Transcription

1 256 MATHEMATICS A.2.1 Inroducion In class XI, we have learn abou mahemaical modelling as an aemp o sudy some par (or form) of some real-life problems in mahemaical erms, i.e., he conversion of a physical siuaion ino mahemaics using some suiable condiions. Roughly speaking mahemaical modelling is an aciviy in which we make models o describe he behaviour of various phenomenal aciviies of our ineres in many ways using words, drawings or skeches, compuer programs, mahemaical formulae ec. In earlier classes, we have observed ha soluions o many problems, involving applicaions of various mahemaical conceps, involve mahemaical modelling in one way or he oher. Therefore, i is imporan o sudy mahemaical modelling as a separae opic. In his chaper, we shall furher sudy mahemaical modelling of some real-life problems using echniques/resuls from marix, calculus and linear programming. A.2.2 Why Mahemaical Modelling? Sudens are aware of he soluion of word problems in arihmeic, algebra, rigonomery and linear programming ec. Someimes we solve he problems wihou going ino he physical insigh of he siuaional problems. Siuaional problems need physical insigh ha is inroducion of physical laws and some symbols o compare he mahemaical resuls obained wih pracical values. To solve many problems faced by us, we need a echnique and his is wha is known as mahemaical modelling. Le us consider he following problems: (i) (ii) (iii) (iv) To find he widh of a river (paricularly, when i is difficul o cross he river). To find he opimal angle in case of sho-pu (by considering he variables such as : he heigh of he hrower, resisance of he media, acceleraion due o graviy ec.). To find he heigh of a ower (paricularly, when i is no possible o reach he op of he ower). To find he emperaure a he surface of he Sun. Appendix 2 MATHEMATICAL MODELLING

2 (v) (vi) MATHEMATICAL MODELLING 257 Why hear paiens are no allowed o use lif? (wihou knowing he physiology of a human being). To find he mass of he Earh. (vii) Esimae he yield of pulses in India from he sanding crops (a person is no allowed o cu all of i). (viii) Find he volume of blood inside he body of a person (a person is no allowed o bleed compleely). (ix) Esimae he populaion of India in he year 2020 (a person is no allowed o wai ill hen). All of hese problems can be solved and infac have been solved wih he help of Mahemaics using mahemaical modelling. In fac, you migh have sudied he mehods for solving some of hem in he presen exbook iself. However, i will be insrucive if you firs ry o solve hem yourself and ha oo wihou he help of Mahemaics, if possible, you will hen appreciae he power of Mahemaics and he need for mahemaical modelling. A.2.3 Principles of Mahemaical Modelling Mahemaical modelling is a principled aciviy and so i has some principles behind i. These principles are almos philosophical in naure. Some of he basic principles of mahemaical modelling are lised below in erms of insrucions: (i) Idenify he need for he model. (for wha we are looking for) (ii) Lis he parameers/variables which are required for he model. (iii) Idenify he available releven daa. (wha is given?) (iv) Idenify he circumsances ha can be applied (assumpions) (v) Idenify he governing physical principles. (vi) Idenify (a) he equaions ha will be used. (b) he calculaions ha will be made. (c) he soluion which will follow. (vii) Idenify ess ha can check he (a) consisency of he model. (b) uiliy of he model. (viii) Idenify he parameer values ha can improve he model.

3 258 MATHEMATICS The above principles of mahemaical modelling lead o he following: seps for mahemaical modelling. Sep 1: Idenify he physical siuaion. Sep 2: Conver he physical siuaion ino a mahemaical model by inroducing parameers / variables and using various known physical laws and symbols. Sep 3: Find he soluion of he mahemaical problem. Sep 4: Inerpre he resul in erms of he original problem and compare he resul wih observaions or experimens. Sep 5: If he resul is in good agreemen, hen accep he model. Oherwise modify he hypoheses / assumpions according o he physical siuaion and go o Sep 2. The above seps can also be viewed hrough he following diagram: Fig A.2.1 Example 1 Find he heigh of a given ower using mahemaical modelling. Soluion Sep 1 Given physical siuaion is o find he heigh of a given ower. Sep 2 Le AB be he given ower (Fig A.2.2). Le PQ be an observer measuring he heigh of he ower wih his eye a P. Le PQ = h and le heigh of ower be H. Le α be he angle of elevaion from he eye of he observer o he op of he ower. Fig A.2.2

4 MATHEMATICAL MODELLING 259 Le l = PC = QB Now an α = AC H h = PC l or H = h + l an α... (1) Sep 3 Noe ha he values of he parameers h, l and α (using sexan) are known o he observer and so (1) gives he soluion of he problem. Sep 4 In case, if he foo of he ower is no accessible, i.e., when l is no known o he observer, le β be he angle of depression from P o he foo B of he ower. So from ΔPQB, we have PQ h anβ = = or l = h co β QB l Sep 5 is no required in his siuaion as exac values of he parameers h, l, α and β are known. Example 2 Le a business firm produces hree ypes of producs P 1, P 2 and P 3 ha uses hree ypes of raw maerials R 1 and R 3. Le he firm has purchase orders from wo cliens F 1 and F 2. Considering he siuaion ha he firm has a limied quaniy of R 1 and R 3, respecively, prepare a model o deermine he quaniies of he raw maerial R 1 and R 3 required o mee he purchase orders. Soluion Sep 1 The physical siuaion is well idenified in he problem. Sep 2 Le A be a marix ha represens purchase orders from he wo cliens F 1 and F 2. Then, A is of he form P1 P2 P3 F = 1 A F 2 Le B be he marix ha represens he amoun of raw maerials R 1 and R 3, required o manufacure each uni of he producs P 1, P 2 and P 3. Then, B is of he form R1R2R3 P1 B= P 2 P 3

5 260 MATHEMATICS Sep 3 Noe ha he produc (which in his case is well defined) of marices A and B is given by he following marix R1R2R3 F = 1 AB F 2 which in fac gives he desired quaniies of he raw maerials R 1 and R 3 o fulfill he purchase orders of he wo cliens F 1 and F 2. Example 3 Inerpre he model in Example 2, in case A=, B = and he available raw maerials are 330 unis of R 1, 455 unis of R 2 and 140 unis of R 3. Soluion Noe ha AB = R1 R 2 R3 F = F This clearly shows ha o mee he purchase order of F 1 and F 2, he raw maerial required is 335 unis of R 1, 467 unis of R 2 and 147 unis of R 3 which is much more han he available raw maerial. Since he amoun of raw maerial required o manufacure each uni of he hree producs is fixed, we can eiher ask for an increase in he available raw maerial or we may ask he cliens o reduce heir orders. Remark If we replace A in Example 3 by A 1 given by A 1 = i.e., if he cliens agree o reduce heir purchase orders, hen A 1 B =

6 MATHEMATICAL MODELLING 261 This requires 311 unis of R 1, 436 unis of R 2 and 138 unis of R 3 which are well below he available raw maerials, i.e., 330 unis of R 1, 455 unis of R 2 and 140 unis of R 3. Thus, if he revised purchase orders of he cliens are given by A 1, hen he firm can easily supply he purchase orders of he wo cliens. Noe One may furher modify A so as o make full use of he available raw maerial. Query Can we make a mahemaical model wih a given B and wih fixed quaniies of he available raw maerial ha can help he firm owner o ask he cliens o modify heir orders in such a way ha he firm makes he full use of is available raw maerial? The answer o his query is given in he following example: Example 4 Suppose P 1, P 2, P 3 and R 1, R 3 are as in Example 2. Le he firm has 330 unis of R 1, 455 unis of R 2 and 140 unis of R 3 available wih i and le he amoun of raw maerials R 1 and R 3 required o manufacure each uni of he hree producs is given by R1 R2 R3 P B= P P How many unis of each produc is o be made so as o uilise he full available raw maerial? Soluion Sep 1 The siuaion is easily idenifiable. Sep 2 Suppose he firm produces x unis of P 1, y unis of P 2 and z unis of P 3. Since produc P 1 requires 3 unis of R 1, P 2 requires 7 unis of R 1 and P 3 requires 5 unis of R 1 (observe marix B) and he oal number of unis, of R 1, available is 330, we have Similarly, we have 3x + 7y + 5z = 330 (for raw maerial R 1 ) 4x + 9y + 12z = 455 (for raw maerial R 2 ) and 3y + 7z = 140 (for raw maerial R 3 ) This sysem of equaions can be expressed in marix form as x y z 140

7 262 MATHEMATICS Sep 3 Using elemenary row operaions, we obain x y This gives x = 20, y = 35 and z = 5. Thus, he firm can produce 20 unis of P 1, 35 unis of P 2 and 5 unis of P 3 o make full use of is available raw maerial. Remark One may observe ha if he manufacurer decides o manufacure according o he available raw maerial and no according o he purchase orders of he wo cliens F 1 and F 2 (as in Example 3), he/she is unable o mee hese purchase orders as F 1 demanded 6 unis of P 3 where as he manufacurer can make only 5 unis of P 3. Example 5 A manufacurer of medicines is preparing a producion plan of medicines M 1 and M 2. There are sufficien raw maerials available o make boles of M 1 and boles of M 2, bu here are only boles ino which eiher of he medicines can be pu. Furher, i akes 3 hours o prepare enough maerial o fill 1000 boles of M 1, i akes 1 hour o prepare enough maerial o fill 1000 boles of M 2 and here are 66 hours available for his operaion. The profi is Rs 8 per bole for M 1 and Rs 7 per bole for M 2. How should he manufacurer schedule his/her producion in order o maximise profi? Soluion Sep 1 To find he number of boles of M 1 and M 2 in order o maximise he profi under he given hypoheses. Sep 2 Le x be he number of boles of ype M 1 medicine and y be he number of boles of ype M 2 medicine. Since profi is Rs 8 per bole for M 1 and Rs 7 per bole for M 2, herefore he objecive funcion (which is o be maximised) is given by Z Z (x, y) = 8x + 7y The objecive funcion is o be maximised subjec o he consrains (Refer Chaper 12 on Linear Programming) x y x y z x y x 0, y (1) Sep 3 The shaded region OPQRST is he feasible region for he consrains (1) (Fig A.2.3). The co-ordinaes of verices O, P, Q, R, S and T are (0, 0), (20000, 0), (20000, 6000), (10500, 34500), (5000, 40000) and (0, 40000), respecively.

8 MATHEMATICAL MODELLING 263 Noe ha Z a P (0, 0) = 0 Fig A.2.3 Z a P (20000, 0) = = Z a Q (20000, 6000) = = Z a R (10500, 34500) = = Z a S = (5000, 40000) = = Z a T = (0, 40000) = = Now observe ha he profi is maximum a x = and y = and he maximum profi is Rs Hence, he manufacurer should produce boles of M 1 medicine and boles of M 2 medicine in order o ge maximum profi of Rs Example 6 Suppose a company plans o produce a new produc ha incur some coss (fixed and variable) and le he company plans o sell he produc a a fixed price. Prepare a mahemaical model o examine he profiabiliy. Soluion Sep 1 Siuaion is clearly idenifiable.

9 264 MATHEMATICS Sep 2 Formulaion: We are given ha he coss are of wo ypes: fixed and variable. The fixed coss are independen of he number of unis produced (e.g., ren and raes), while he variable coss increase wih he number of unis produced (e.g., maerial). Iniially, we assume ha he variable coss are direcly proporional o he number of unis produced his should simplify our model. The company earn a cerain amoun of money by selling is producs and wans o ensure ha i is maximum. For convenience, we assume ha all unis produced are sold immediaely. The mahemaical model Le x = number of unis produced and sold C = oal cos of producion (in rupees) I = income from sales (in rupees) P = profi (in rupees) Our assumpions above sae ha C consiss of wo pars: (i) fixed cos = a (in rupees), (ii) variable cos = b (rupees/uni produced). Then C = a + bx... (1) Also, income I depends on selling price s (rupees/uni) Thus I = sx... (2) The profi P is hen he difference beween income and coss. So P = I C = sx (a + bx) =(s b) x a... (3) We now have a mahemaical model of he relaionships (1) o (3) beween he variables x, C, I, P, a, b, s. These variables may be classified as: independen x dependen C, I, P parameers a, b, s The manufacurer, knowing x, a, b, s can deermine P. Sep 3 From (3), we can observe ha for he break even poin (i.e., make neiher profi a nor loss), he mus have P = 0, i.e., x unis. s b Seps 4 and 5 In view of he break even poin, one may conclude ha if he company a produces few unis, i.e., less han x unis, hen he company will suffer loss s b

10 MATHEMATICAL MODELLING 265 and if i produces large number of unis, i.e., much more han a s b unis, hen i can make huge profi. Furher, if he break even poin proves o be unrealisic, hen anoher model could be ried or he assumpions regarding cash flow may be modified. Remark From (3), we also have d P s b dx = This means ha rae of change of P wih respec o x depends on he quaniy s b, which is he difference of selling price and he variable cos of each produc. Thus, in order o gain profi, his should be posiive and o ge large gains, we need o produce large quaniy of he produc and a he same ime ry o reduce he variable cos. Example 7 Le a ank conains 1000 lires of brine which conains 250 g of sal per lire. Brine conaining 200 g of sal per lire flows ino he ank a he rae of 25 lires per minue and he mixure flows ou a he same rae. Assume ha he mixure is kep uniform all he ime by sirring. Wha would be he amoun of sal in he ank a any ime? Soluion Sep 1 The siuaion is easily idenifiable. Sep 2 Le y = y () denoe he amoun of sal (in kg) in he ank a ime (in minues) afer he inflow, ouflow sars. Furher assume ha y is a differeniable funcion. When = 0, i.e., before he inflow ouflow of he brine sars, y = 250 g 1000 = 250 kg Noe ha he change in y occurs due o he inflow, ouflow of he mixure. Now he inflow of brine brings sal ino he ank a he rae of 5 kg per minue (as g = 5 kg) and he ouflow of brine akes sal ou of he ank a he rae of y y y 25 kg per minue (as a ime, he sal in he ank is kg) Thus, he rae of change of sal wih respec o is given by or dy y = 5 d 40 (Why?) dy 1 y d + = 5... (1) 40

11 266 MATHEMATICS This gives a mahemaical model for he given problem. Sep 3 Equaion (1) is a linear equaion and can be easily solved. The soluion of (1) is given by ye where, c is he consan of inegraion. Noe ha when = 0, y = 250. Therefore, 250 = C or C = 50 Then (2) reduces o or or Therefore = 40 = 200e + C or y () = C e... (2) 40 y = e... (3) y 200 = e = 40log 40 e 50 y 200 e 50 y 200 Here, he equaion (4) gives he ime a which he sal in ank is y kg. e... (4) Sep 4 Since 40 is always posiive, from (3), we conclude ha y > 200 a all imes Thus, he minimum amoun of sal conen in he ank is 200 kg. Also, from (4), we conclude ha > 0 if and only if 0 < y 200 < 50 i.e., if and only if 200 < y < 250 i.e., he amoun of sal conen in he ank afer he sar of inflow and ouflow of he brine is beween 200 kg and 250 kg. Limiaions of Mahemaical Modelling Till oday many mahemaical models have been developed and applied successfully o undersand and ge an insigh ino housands of siuaions. Some of he subjecs like mahemaical physics, mahemaical economics, operaions research, bio-mahemaics ec. are almos synonymous wih mahemaical modelling. Bu here are sill a large number of siuaions which are ye o be modelled. The reason behind his is ha eiher he siuaion are found o be very complex or he mahemaical models formed are mahemaically inracable.

12 MATHEMATICAL MODELLING 267 The developmen of he powerful compuers and super compuers has enabled us o mahemaically model a large number of siuaions (even complex siuaions). Due o hese fas and advanced compuers, i has been possible o prepare more realisic models which can obain beer agreemens wih observaions. However, we do no have good guidelines for choosing various parameers / variables and also for esimaing he values of hese parameers / variables used in a mahemaical model. Infac, we can prepare reasonably accurae models o fi any daa by choosing five or six parameers / variables. We require a minimal number of parameers / variables o be able o esimae hem accuraely. Mahemaical modelling of large or complex siuaions has is own special problems. These ype of siuaions usually occur in he sudy of world models of environmen, oceanography, polluion conrol ec. Mahemaical modellers from all disciplines mahemaics, compuer science, physics, engineering, social sciences, ec., are involved in meeing hese challenges wih courage.

MATHEMATICAL MODELLING

MATHEMATICAL MODELLING 256 MATHEMATICS Appendix 2 MATHEMATICAL MODELLING A.2.1 Inroducion In class XI, we have learn abou mahemaical modelling as an aemp o sudy some par (or form) of some real-life problems in mahemaical erms,

More information

1.6. Slopes of Tangents and Instantaneous Rate of Change

1.6. Slopes of Tangents and Instantaneous Rate of Change 1.6 Slopes of Tangens and Insananeous Rae of Change When you hi or kick a ball, he heigh, h, in meres, of he ball can be modelled by he equaion h() 4.9 2 v c. In his equaion, is he ime, in seconds; c represens

More information

Math 333 Problem Set #2 Solution 14 February 2003

Math 333 Problem Set #2 Solution 14 February 2003 Mah 333 Problem Se #2 Soluion 14 February 2003 A1. Solve he iniial value problem dy dx = x2 + e 3x ; 2y 4 y(0) = 1. Soluion: This is separable; we wrie 2y 4 dy = x 2 + e x dx and inegrae o ge The iniial

More information

Vehicle Arrival Models : Headway

Vehicle Arrival Models : Headway Chaper 12 Vehicle Arrival Models : Headway 12.1 Inroducion Modelling arrival of vehicle a secion of road is an imporan sep in raffic flow modelling. I has imporan applicaion in raffic flow simulaion where

More information

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still.

Lecture 2-1 Kinematics in One Dimension Displacement, Velocity and Acceleration Everything in the world is moving. Nothing stays still. Lecure - Kinemaics in One Dimension Displacemen, Velociy and Acceleraion Everyhing in he world is moving. Nohing says sill. Moion occurs a all scales of he universe, saring from he moion of elecrons in

More information

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle

Physics 235 Chapter 2. Chapter 2 Newtonian Mechanics Single Particle Chaper 2 Newonian Mechanics Single Paricle In his Chaper we will review wha Newon s laws of mechanics ell us abou he moion of a single paricle. Newon s laws are only valid in suiable reference frames,

More information

CSE 3802 / ECE Numerical Methods in Scientific Computation. Jinbo Bi. Department of Computer Science & Engineering

CSE 3802 / ECE Numerical Methods in Scientific Computation. Jinbo Bi. Department of Computer Science & Engineering CSE 3802 / ECE 3431 Numerical Mehods in Scienific Compuaion Jinbo Bi Deparmen of Compuer Science & Engineering hp://www.engr.uconn.edu/~jinbo 1 Ph.D in Mahemaics The Insrucor Previous professional experience:

More information

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates

Biol. 356 Lab 8. Mortality, Recruitment, and Migration Rates Biol. 356 Lab 8. Moraliy, Recruimen, and Migraion Raes (modified from Cox, 00, General Ecology Lab Manual, McGraw Hill) Las week we esimaed populaion size hrough several mehods. One assumpion of all hese

More information

STATE-SPACE MODELLING. A mass balance across the tank gives:

STATE-SPACE MODELLING. A mass balance across the tank gives: B. Lennox and N.F. Thornhill, 9, Sae Space Modelling, IChemE Process Managemen and Conrol Subjec Group Newsleer STE-SPACE MODELLING Inroducion: Over he pas decade or so here has been an ever increasing

More information

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010

Simulation-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Simulaion-Solving Dynamic Models ABE 5646 Week 2, Spring 2010 Week Descripion Reading Maerial 2 Compuer Simulaion of Dynamic Models Finie Difference, coninuous saes, discree ime Simple Mehods Euler Trapezoid

More information

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon

3.1.3 INTRODUCTION TO DYNAMIC OPTIMIZATION: DISCRETE TIME PROBLEMS. A. The Hamiltonian and First-Order Conditions in a Finite Time Horizon 3..3 INRODUCION O DYNAMIC OPIMIZAION: DISCREE IME PROBLEMS A. he Hamilonian and Firs-Order Condiions in a Finie ime Horizon Define a new funcion, he Hamilonian funcion, H. H he change in he oal value of

More information

Math 115 Final Exam December 14, 2017

Math 115 Final Exam December 14, 2017 On my honor, as a suden, I have neiher given nor received unauhorized aid on his academic work. Your Iniials Only: Iniials: Do no wrie in his area Mah 5 Final Exam December, 07 Your U-M ID # (no uniqname):

More information

KINEMATICS IN ONE DIMENSION

KINEMATICS IN ONE DIMENSION KINEMATICS IN ONE DIMENSION PREVIEW Kinemaics is he sudy of how hings move how far (disance and displacemen), how fas (speed and velociy), and how fas ha how fas changes (acceleraion). We say ha an objec

More information

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes

23.5. Half-Range Series. Introduction. Prerequisites. Learning Outcomes Half-Range Series 2.5 Inroducion In his Secion we address he following problem: Can we find a Fourier series expansion of a funcion defined over a finie inerval? Of course we recognise ha such a funcion

More information

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x

u(x) = e x 2 y + 2 ) Integrate and solve for x (1 + x)y + y = cos x Answer: Divide both sides by 1 + x and solve for y. y = x y + cos x . 1 Mah 211 Homework #3 February 2, 2001 2.4.3. y + (2/x)y = (cos x)/x 2 Answer: Compare y + (2/x) y = (cos x)/x 2 wih y = a(x)x + f(x)and noe ha a(x) = 2/x. Consequenly, an inegraing facor is found wih

More information

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws

Chapter 15: Phenomena. Chapter 15 Chemical Kinetics. Reaction Rates. Reaction Rates R P. Reaction Rates. Rate Laws Chaper 5: Phenomena Phenomena: The reacion (aq) + B(aq) C(aq) was sudied a wo differen emperaures (98 K and 35 K). For each emperaure he reacion was sared by puing differen concenraions of he 3 species

More information

Seminar 4: Hotelling 2

Seminar 4: Hotelling 2 Seminar 4: Hoelling 2 November 3, 211 1 Exercise Par 1 Iso-elasic demand A non renewable resource of a known sock S can be exraced a zero cos. Demand for he resource is of he form: D(p ) = p ε ε > A a

More information

Solutions to Assignment 1

Solutions to Assignment 1 MA 2326 Differenial Equaions Insrucor: Peronela Radu Friday, February 8, 203 Soluions o Assignmen. Find he general soluions of he following ODEs: (a) 2 x = an x Soluion: I is a separable equaion as we

More information

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should

In this chapter the model of free motion under gravity is extended to objects projected at an angle. When you have completed it, you should Cambridge Universiy Press 978--36-60033-7 Cambridge Inernaional AS and A Level Mahemaics: Mechanics Coursebook Excerp More Informaion Chaper The moion of projeciles In his chaper he model of free moion

More information

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes

2.7. Some common engineering functions. Introduction. Prerequisites. Learning Outcomes Some common engineering funcions 2.7 Inroducion This secion provides a caalogue of some common funcions ofen used in Science and Engineering. These include polynomials, raional funcions, he modulus funcion

More information

Solutionbank Edexcel AS and A Level Modular Mathematics

Solutionbank Edexcel AS and A Level Modular Mathematics Page of 4 Soluionbank Edexcel AS and A Level Modular Mahemaics Exercise A, Quesion Quesion: Skech he graphs of (a) y = e x + (b) y = 4e x (c) y = e x 3 (d) y = 4 e x (e) y = 6 + 0e x (f) y = 00e x + 0

More information

04. Kinetics of a second order reaction

04. Kinetics of a second order reaction 4. Kineics of a second order reacion Imporan conceps Reacion rae, reacion exen, reacion rae equaion, order of a reacion, firs-order reacions, second-order reacions, differenial and inegraed rae laws, Arrhenius

More information

On a Discrete-In-Time Order Level Inventory Model for Items with Random Deterioration

On a Discrete-In-Time Order Level Inventory Model for Items with Random Deterioration Journal of Agriculure and Life Sciences Vol., No. ; June 4 On a Discree-In-Time Order Level Invenory Model for Iems wih Random Deerioraion Dr Biswaranjan Mandal Associae Professor of Mahemaics Acharya

More information

APPM 2360 Homework Solutions, Due June 10

APPM 2360 Homework Solutions, Due June 10 2.2.2: Find general soluions for he equaion APPM 2360 Homework Soluions, Due June 10 Soluion: Finding he inegraing facor, dy + 2y = 3e µ) = e 2) = e 2 Muliplying he differenial equaion by he inegraing

More information

Economics 8105 Macroeconomic Theory Recitation 6

Economics 8105 Macroeconomic Theory Recitation 6 Economics 8105 Macroeconomic Theory Reciaion 6 Conor Ryan Ocober 11h, 2016 Ouline: Opimal Taxaion wih Governmen Invesmen 1 Governmen Expendiure in Producion In hese noes we will examine a model in which

More information

Morning Time: 1 hour 30 minutes Additional materials (enclosed):

Morning Time: 1 hour 30 minutes Additional materials (enclosed): ADVANCED GCE 78/0 MATHEMATICS (MEI) Differenial Equaions THURSDAY JANUARY 008 Morning Time: hour 30 minues Addiional maerials (enclosed): None Addiional maerials (required): Answer Bookle (8 pages) Graph

More information

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8)

Econ107 Applied Econometrics Topic 7: Multicollinearity (Studenmund, Chapter 8) I. Definiions and Problems A. Perfec Mulicollineariy Econ7 Applied Economerics Topic 7: Mulicollineariy (Sudenmund, Chaper 8) Definiion: Perfec mulicollineariy exiss in a following K-variable regression

More information

Final Spring 2007

Final Spring 2007 .615 Final Spring 7 Overview The purpose of he final exam is o calculae he MHD β limi in a high-bea oroidal okamak agains he dangerous n = 1 exernal ballooning-kink mode. Effecively, his corresponds o

More information

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n

Module 2 F c i k c s la l w a s o s f dif di fusi s o i n Module Fick s laws of diffusion Fick s laws of diffusion and hin film soluion Adolf Fick (1855) proposed: d J α d d d J (mole/m s) flu (m /s) diffusion coefficien and (mole/m 3 ) concenraion of ions, aoms

More information

Predator - Prey Model Trajectories and the nonlinear conservation law

Predator - Prey Model Trajectories and the nonlinear conservation law Predaor - Prey Model Trajecories and he nonlinear conservaion law James K. Peerson Deparmen of Biological Sciences and Deparmen of Mahemaical Sciences Clemson Universiy Ocober 28, 213 Ouline Drawing Trajecories

More information

Chapter 2. First Order Scalar Equations

Chapter 2. First Order Scalar Equations Chaper. Firs Order Scalar Equaions We sar our sudy of differenial equaions in he same way he pioneers in his field did. We show paricular echniques o solve paricular ypes of firs order differenial equaions.

More information

Lab #2: Kinematics in 1-Dimension

Lab #2: Kinematics in 1-Dimension Reading Assignmen: Chaper 2, Secions 2-1 hrough 2-8 Lab #2: Kinemaics in 1-Dimension Inroducion: The sudy of moion is broken ino wo main areas of sudy kinemaics and dynamics. Kinemaics is he descripion

More information

EXERCISES FOR SECTION 1.5

EXERCISES FOR SECTION 1.5 1.5 Exisence and Uniqueness of Soluions 43 20. 1 v c 21. 1 v c 1 2 4 6 8 10 1 2 2 4 6 8 10 Graph of approximae soluion obained using Euler s mehod wih = 0.1. Graph of approximae soluion obained using Euler

More information

Inventory Control of Perishable Items in a Two-Echelon Supply Chain

Inventory Control of Perishable Items in a Two-Echelon Supply Chain Journal of Indusrial Engineering, Universiy of ehran, Special Issue,, PP. 69-77 69 Invenory Conrol of Perishable Iems in a wo-echelon Supply Chain Fariborz Jolai *, Elmira Gheisariha and Farnaz Nojavan

More information

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8.

Kinematics Vocabulary. Kinematics and One Dimensional Motion. Position. Coordinate System in One Dimension. Kinema means movement 8. Kinemaics Vocabulary Kinemaics and One Dimensional Moion 8.1 WD1 Kinema means movemen Mahemaical descripion of moion Posiion Time Inerval Displacemen Velociy; absolue value: speed Acceleraion Averages

More information

Appendix 14.1 The optimal control problem and its solution using

Appendix 14.1 The optimal control problem and its solution using 1 Appendix 14.1 he opimal conrol problem and is soluion using he maximum principle NOE: Many occurrences of f, x, u, and in his file (in equaions or as whole words in ex) are purposefully in bold in order

More information

2. Nonlinear Conservation Law Equations

2. Nonlinear Conservation Law Equations . Nonlinear Conservaion Law Equaions One of he clear lessons learned over recen years in sudying nonlinear parial differenial equaions is ha i is generally no wise o ry o aack a general class of nonlinear

More information

SPH3U: Projectiles. Recorder: Manager: Speaker:

SPH3U: Projectiles. Recorder: Manager: Speaker: SPH3U: Projeciles Now i s ime o use our new skills o analyze he moion of a golf ball ha was ossed hrough he air. Le s find ou wha is special abou he moion of a projecile. Recorder: Manager: Speaker: 0

More information

Single and Double Pendulum Models

Single and Double Pendulum Models Single and Double Pendulum Models Mah 596 Projec Summary Spring 2016 Jarod Har 1 Overview Differen ypes of pendulums are used o model many phenomena in various disciplines. In paricular, single and double

More information

Let us start with a two dimensional case. We consider a vector ( x,

Let us start with a two dimensional case. We consider a vector ( x, Roaion marices We consider now roaion marices in wo and hree dimensions. We sar wih wo dimensions since wo dimensions are easier han hree o undersand, and one dimension is a lile oo simple. However, our

More information

This document was generated at 7:34 PM, 07/27/09 Copyright 2009 Richard T. Woodward

This document was generated at 7:34 PM, 07/27/09 Copyright 2009 Richard T. Woodward his documen was generaed a 7:34 PM, 07/27/09 Copyrigh 2009 Richard. Woodward 15. Bang-bang and mos rapid approach problems AGEC 637 - Summer 2009 here are some problems for which he opimal pah does no

More information

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page

dy dx = xey (a) y(0) = 2 (b) y(1) = 2.5 SOLUTION: See next page Assignmen 1 MATH 2270 SOLUTION Please wrie ou complee soluions for each of he following 6 problems (one more will sill be added). You may, of course, consul wih your classmaes, he exbook or oher resources,

More information

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18

A First Course on Kinetics and Reaction Engineering. Class 19 on Unit 18 A Firs ourse on Kineics and Reacion Engineering lass 19 on Uni 18 Par I - hemical Reacions Par II - hemical Reacion Kineics Where We re Going Par III - hemical Reacion Engineering A. Ideal Reacors B. Perfecly

More information

Math 315: Linear Algebra Solutions to Assignment 6

Math 315: Linear Algebra Solutions to Assignment 6 Mah 35: Linear Algebra s o Assignmen 6 # Which of he following ses of vecors are bases for R 2? {2,, 3, }, {4,, 7, 8}, {,,, 3}, {3, 9, 4, 2}. Explain your answer. To generae he whole R 2, wo linearly independen

More information

Math 2214 Solution Test 1B Fall 2017

Math 2214 Solution Test 1B Fall 2017 Mah 14 Soluion Tes 1B Fall 017 Problem 1: A ank has a capaci for 500 gallons and conains 0 gallons of waer wih lbs of sal iniiall. A soluion conaining of 8 lbsgal of sal is pumped ino he ank a 10 galsmin.

More information

CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS

CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS CHEAPEST PMT ONLINE TEST SERIES AIIMS/NEET TOPPER PREPARE QUESTIONS For more deails see las page or conac @aimaiims.in Physics Mock Tes Paper AIIMS/NEET 07 Physics 06 Saurday Augus 0 Uni es : Moion in

More information

Matlab and Python programming: how to get started

Matlab and Python programming: how to get started Malab and Pyhon programming: how o ge sared Equipping readers he skills o wrie programs o explore complex sysems and discover ineresing paerns from big daa is one of he main goals of his book. In his chaper,

More information

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x

WEEK-3 Recitation PHYS 131. of the projectile s velocity remains constant throughout the motion, since the acceleration a x WEEK-3 Reciaion PHYS 131 Ch. 3: FOC 1, 3, 4, 6, 14. Problems 9, 37, 41 & 71 and Ch. 4: FOC 1, 3, 5, 8. Problems 3, 5 & 16. Feb 8, 018 Ch. 3: FOC 1, 3, 4, 6, 14. 1. (a) The horizonal componen of he projecile

More information

Macroeconomic Theory Ph.D. Qualifying Examination Fall 2005 ANSWER EACH PART IN A SEPARATE BLUE BOOK. PART ONE: ANSWER IN BOOK 1 WEIGHT 1/3

Macroeconomic Theory Ph.D. Qualifying Examination Fall 2005 ANSWER EACH PART IN A SEPARATE BLUE BOOK. PART ONE: ANSWER IN BOOK 1 WEIGHT 1/3 Macroeconomic Theory Ph.D. Qualifying Examinaion Fall 2005 Comprehensive Examinaion UCLA Dep. of Economics You have 4 hours o complee he exam. There are hree pars o he exam. Answer all pars. Each par has

More information

Math 105 Second Midterm March 16, 2017

Math 105 Second Midterm March 16, 2017 Mah 105 Second Miderm March 16, 2017 UMID: Insrucor: Iniials: Secion: 1. Do no open his exam unil you are old o do so. 2. Do no wrie your name anywhere on his exam. 3. This exam has 9 pages including his

More information

Sub Module 2.6. Measurement of transient temperature

Sub Module 2.6. Measurement of transient temperature Mechanical Measuremens Prof. S.P.Venkaeshan Sub Module 2.6 Measuremen of ransien emperaure Many processes of engineering relevance involve variaions wih respec o ime. The sysem properies like emperaure,

More information

8. Basic RL and RC Circuits

8. Basic RL and RC Circuits 8. Basic L and C Circuis This chaper deals wih he soluions of he responses of L and C circuis The analysis of C and L circuis leads o a linear differenial equaion This chaper covers he following opics

More information

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits

EECE251. Circuit Analysis I. Set 4: Capacitors, Inductors, and First-Order Linear Circuits EEE25 ircui Analysis I Se 4: apaciors, Inducors, and Firs-Order inear ircuis Shahriar Mirabbasi Deparmen of Elecrical and ompuer Engineering Universiy of Briish olumbia shahriar@ece.ubc.ca Overview Passive

More information

This document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC

This document was generated at 1:04 PM, 09/10/13 Copyright 2013 Richard T. Woodward. 4. End points and transversality conditions AGEC his documen was generaed a 1:4 PM, 9/1/13 Copyrigh 213 Richard. Woodward 4. End poins and ransversaliy condiions AGEC 637-213 F z d Recall from Lecure 3 ha a ypical opimal conrol problem is o maimize (,,

More information

IB Physics Kinematics Worksheet

IB Physics Kinematics Worksheet IB Physics Kinemaics Workshee Wrie full soluions and noes for muliple choice answers. Do no use a calculaor for muliple choice answers. 1. Which of he following is a correc definiion of average acceleraion?

More information

!!"#"$%&#'()!"#&'(*%)+,&',-)./0)1-*23)

!!#$%&#'()!#&'(*%)+,&',-)./0)1-*23) "#"$%&#'()"#&'(*%)+,&',-)./)1-*) #$%&'()*+,&',-.%,/)*+,-&1*#$)()5*6$+$%*,7&*-'-&1*(,-&*6&,7.$%$+*&%'(*8$&',-,%'-&1*(,-&*6&,79*(&,%: ;..,*&1$&$.$%&'()*1$$.,'&',-9*(&,%)?%*,('&5

More information

MA Study Guide #1

MA Study Guide #1 MA 66 Su Guide #1 (1) Special Tpes of Firs Order Equaions I. Firs Order Linear Equaion (FOL): + p() = g() Soluion : = 1 µ() [ ] µ()g() + C, where µ() = e p() II. Separable Equaion (SEP): dx = h(x) g()

More information

6.003 Homework 1. Problems. Due at the beginning of recitation on Wednesday, February 10, 2010.

6.003 Homework 1. Problems. Due at the beginning of recitation on Wednesday, February 10, 2010. 6.003 Homework Due a he beginning of reciaion on Wednesday, February 0, 200. Problems. Independen and Dependen Variables Assume ha he heigh of a waer wave is given by g(x v) where x is disance, v is velociy,

More information

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17

Designing Information Devices and Systems I Spring 2019 Lecture Notes Note 17 EES 16A Designing Informaion Devices and Sysems I Spring 019 Lecure Noes Noe 17 17.1 apaciive ouchscreen In he las noe, we saw ha a capacior consiss of wo pieces on conducive maerial separaed by a nonconducive

More information

Structural Dynamics and Earthquake Engineering

Structural Dynamics and Earthquake Engineering Srucural Dynamics and Earhquae Engineering Course 1 Inroducion. Single degree of freedom sysems: Equaions of moion, problem saemen, soluion mehods. Course noes are available for download a hp://www.c.up.ro/users/aurelsraan/

More information

ADVANCED MATHEMATICS FOR ECONOMICS /2013 Sheet 3: Di erential equations

ADVANCED MATHEMATICS FOR ECONOMICS /2013 Sheet 3: Di erential equations ADVANCED MATHEMATICS FOR ECONOMICS - /3 Shee 3: Di erenial equaions Check ha x() =± p ln(c( + )), where C is a posiive consan, is soluion of he ODE x () = Solve he following di erenial equaions: (a) x

More information

Ordinary Differential Equations

Ordinary Differential Equations Lecure 22 Ordinary Differenial Equaions Course Coordinaor: Dr. Suresh A. Karha, Associae Professor, Deparmen of Civil Engineering, IIT Guwahai. In naure, mos of he phenomena ha can be mahemaically described

More information

5.2. The Natural Logarithm. Solution

5.2. The Natural Logarithm. Solution 5.2 The Naural Logarihm The number e is an irraional number, similar in naure o π. Is non-erminaing, non-repeaing value is e 2.718 281 828 59. Like π, e also occurs frequenly in naural phenomena. In fac,

More information

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore

Solutions of Sample Problems for Third In-Class Exam Math 246, Spring 2011, Professor David Levermore Soluions of Sample Problems for Third In-Class Exam Mah 6, Spring, Professor David Levermore Compue he Laplace ransform of f e from is definiion Soluion The definiion of he Laplace ransform gives L[f]s

More information

MEI STRUCTURED MATHEMATICS 4758

MEI STRUCTURED MATHEMATICS 4758 OXFORD CAMBRIDGE AND RSA EXAMINATIONS Advanced Subsidiary General Cerificae of Educaion Advanced General Cerificae of Educaion MEI STRUCTURED MATHEMATICS 4758 Differenial Equaions Thursday 5 JUNE 006 Afernoon

More information

PROBLEMS FOR MATH 162 If a problem is starred, all subproblems are due. If only subproblems are starred, only those are due. SLOPES OF TANGENT LINES

PROBLEMS FOR MATH 162 If a problem is starred, all subproblems are due. If only subproblems are starred, only those are due. SLOPES OF TANGENT LINES PROBLEMS FOR MATH 6 If a problem is sarred, all subproblems are due. If onl subproblems are sarred, onl hose are due. 00. Shor answer quesions. SLOPES OF TANGENT LINES (a) A ball is hrown ino he air. Is

More information

Fishing limits and the Logistic Equation. 1

Fishing limits and the Logistic Equation. 1 Fishing limis and he Logisic Equaion. 1 1. The Logisic Equaion. The logisic equaion is an equaion governing populaion growh for populaions in an environmen wih a limied amoun of resources (for insance,

More information

= ( ) ) or a system of differential equations with continuous parametrization (T = R

= ( ) ) or a system of differential equations with continuous parametrization (T = R XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan

Ground Rules. PC1221 Fundamentals of Physics I. Kinematics. Position. Lectures 3 and 4 Motion in One Dimension. A/Prof Tay Seng Chuan Ground Rules PC11 Fundamenals of Physics I Lecures 3 and 4 Moion in One Dimension A/Prof Tay Seng Chuan 1 Swich off your handphone and pager Swich off your lapop compuer and keep i No alking while lecure

More information

Basic Circuit Elements Professor J R Lucas November 2001

Basic Circuit Elements Professor J R Lucas November 2001 Basic Circui Elemens - J ucas An elecrical circui is an inerconnecion of circui elemens. These circui elemens can be caegorised ino wo ypes, namely acive and passive elemens. Some Definiions/explanaions

More information

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes

23.2. Representing Periodic Functions by Fourier Series. Introduction. Prerequisites. Learning Outcomes Represening Periodic Funcions by Fourier Series 3. Inroducion In his Secion we show how a periodic funcion can be expressed as a series of sines and cosines. We begin by obaining some sandard inegrals

More information

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4.

Reading from Young & Freedman: For this topic, read sections 25.4 & 25.5, the introduction to chapter 26 and sections 26.1 to 26.2 & 26.4. PHY1 Elecriciy Topic 7 (Lecures 1 & 11) Elecric Circuis n his opic, we will cover: 1) Elecromoive Force (EMF) ) Series and parallel resisor combinaions 3) Kirchhoff s rules for circuis 4) Time dependence

More information

Solutions Problem Set 3 Macro II (14.452)

Solutions Problem Set 3 Macro II (14.452) Soluions Problem Se 3 Macro II (14.452) Francisco A. Gallego 04/27/2005 1 Q heory of invesmen in coninuous ime and no uncerainy Consider he in nie horizon model of a rm facing adjusmen coss o invesmen.

More information

Mathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation

Mathcad Lecture #8 In-class Worksheet Curve Fitting and Interpolation Mahcad Lecure #8 In-class Workshee Curve Fiing and Inerpolaion A he end of his lecure, you will be able o: explain he difference beween curve fiing and inerpolaion decide wheher curve fiing or inerpolaion

More information

AP Chemistry--Chapter 12: Chemical Kinetics

AP Chemistry--Chapter 12: Chemical Kinetics AP Chemisry--Chaper 12: Chemical Kineics I. Reacion Raes A. The area of chemisry ha deals wih reacion raes, or how fas a reacion occurs, is called chemical kineics. B. The rae of reacion depends on he

More information

EE100 Lab 3 Experiment Guide: RC Circuits

EE100 Lab 3 Experiment Guide: RC Circuits I. Inroducion EE100 Lab 3 Experimen Guide: A. apaciors A capacior is a passive elecronic componen ha sores energy in he form of an elecrosaic field. The uni of capaciance is he farad (coulomb/vol). Pracical

More information

The average rate of change between two points on a function is d t

The average rate of change between two points on a function is d t SM Dae: Secion: Objecive: The average rae of change beween wo poins on a funcion is d. For example, if he funcion ( ) represens he disance in miles ha a car has raveled afer hours, hen finding he slope

More information

1 Differential Equation Investigations using Customizable

1 Differential Equation Investigations using Customizable Differenial Equaion Invesigaions using Cusomizable Mahles Rober Decker The Universiy of Harford Absrac. The auhor has developed some plaform independen, freely available, ineracive programs (mahles) for

More information

Linear Response Theory: The connection between QFT and experiments

Linear Response Theory: The connection between QFT and experiments Phys540.nb 39 3 Linear Response Theory: The connecion beween QFT and experimens 3.1. Basic conceps and ideas Q: How do we measure he conduciviy of a meal? A: we firs inroduce a weak elecric field E, and

More information

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively:

( ) a system of differential equations with continuous parametrization ( T = R + These look like, respectively: XIII. DIFFERENCE AND DIFFERENTIAL EQUATIONS Ofen funcions, or a sysem of funcion, are paramerized in erms of some variable, usually denoed as and inerpreed as ime. The variable is wrien as a funcion of

More information

Introduction to Numerical Analysis. In this lesson you will be taken through a pair of techniques that will be used to solve the equations of.

Introduction to Numerical Analysis. In this lesson you will be taken through a pair of techniques that will be used to solve the equations of. Inroducion o Nuerical Analysis oion In his lesson you will be aen hrough a pair of echniques ha will be used o solve he equaions of and v dx d a F d for siuaions in which F is well nown, and he iniial

More information

Application of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing

Application of a Stochastic-Fuzzy Approach to Modeling Optimal Discrete Time Dynamical Systems by Using Large Scale Data Processing Applicaion of a Sochasic-Fuzzy Approach o Modeling Opimal Discree Time Dynamical Sysems by Using Large Scale Daa Processing AA WALASZE-BABISZEWSA Deparmen of Compuer Engineering Opole Universiy of Technology

More information

HOTELLING LOCATION MODEL

HOTELLING LOCATION MODEL HOTELLING LOCATION MODEL THE LINEAR CITY MODEL The Example of Choosing only Locaion wihou Price Compeiion Le a be he locaion of rm and b is he locaion of rm. Assume he linear ransporaion cos equal o d,

More information

Solutions from Chapter 9.1 and 9.2

Solutions from Chapter 9.1 and 9.2 Soluions from Chaper 9 and 92 Secion 9 Problem # This basically boils down o an exercise in he chain rule from calculus We are looking for soluions of he form: u( x) = f( k x c) where k x R 3 and k is

More information

Exponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits

Exponential Weighted Moving Average (EWMA) Chart Under The Assumption of Moderateness And Its 3 Control Limits DOI: 0.545/mjis.07.5009 Exponenial Weighed Moving Average (EWMA) Char Under The Assumpion of Moderaeness And Is 3 Conrol Limis KALPESH S TAILOR Assisan Professor, Deparmen of Saisics, M. K. Bhavnagar Universiy,

More information

18 Biological models with discrete time

18 Biological models with discrete time 8 Biological models wih discree ime The mos imporan applicaions, however, may be pedagogical. The elegan body of mahemaical heory peraining o linear sysems (Fourier analysis, orhogonal funcions, and so

More information

The equation to any straight line can be expressed in the form:

The equation to any straight line can be expressed in the form: Sring Graphs Par 1 Answers 1 TI-Nspire Invesigaion Suden min Aims Deermine a series of equaions of sraigh lines o form a paern similar o ha formed by he cables on he Jerusalem Chords Bridge. Deermine he

More information

Internet Traffic Modeling for Efficient Network Research Management Prof. Zhili Sun, UniS Zhiyong Liu, CATR

Internet Traffic Modeling for Efficient Network Research Management Prof. Zhili Sun, UniS Zhiyong Liu, CATR Inerne Traffic Modeling for Efficien Nework Research Managemen Prof. Zhili Sun, UniS Zhiyong Liu, CATR UK-China Science Bridge Workshop 13-14 December 2011, London Ouline Inroducion Background Classical

More information

Kinematics and kinematic functions

Kinematics and kinematic functions Kinemaics and kinemaic funcions Kinemaics deals wih he sudy of four funcions (called kinemaic funcions or KFs) ha mahemaically ransform join variables ino caresian variables and vice versa Direc Posiion

More information

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t

R t. C t P t. + u t. C t = αp t + βr t + v t. + β + w t Exercise 7 C P = α + β R P + u C = αp + βr + v (a) (b) C R = α P R + β + w (c) Assumpions abou he disurbances u, v, w : Classical assumions on he disurbance of one of he equaions, eg. on (b): E(v v s P,

More information

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11.

Math 334 Test 1 KEY Spring 2010 Section: 001. Instructor: Scott Glasgow Dates: May 10 and 11. 1 Mah 334 Tes 1 KEY Spring 21 Secion: 1 Insrucor: Sco Glasgow Daes: Ma 1 and 11. Do NOT wrie on his problem saemen bookle, excep for our indicaion of following he honor code jus below. No credi will be

More information

Math 2214 Solution Test 1A Spring 2016

Math 2214 Solution Test 1A Spring 2016 Mah 14 Soluion Tes 1A Spring 016 sec Problem 1: Wha is he larges -inerval for which ( 4) = has a guaraneed + unique soluion for iniial value (-1) = 3 according o he Exisence Uniqueness Theorem? Soluion

More information

Decimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0.

Decimal moved after first digit = 4.6 x Decimal moves five places left SCIENTIFIC > POSITIONAL. a) g) 5.31 x b) 0. PHYSICS 20 UNIT 1 SCIENCE MATH WORKSHEET NAME: A. Sandard Noaion Very large and very small numbers are easily wrien using scienific (or sandard) noaion, raher han decimal (or posiional) noaion. Sandard

More information

UCLA: Math 3B Problem set 3 (solutions) Fall, 2018

UCLA: Math 3B Problem set 3 (solutions) Fall, 2018 UCLA: Mah 3B Problem se 3 (soluions) Fall, 28 This problem se concenraes on pracice wih aniderivaives. You will ge los of pracice finding simple aniderivaives as well as finding aniderivaives graphically

More information

10. State Space Methods

10. State Space Methods . Sae Space Mehods. Inroducion Sae space modelling was briefly inroduced in chaper. Here more coverage is provided of sae space mehods before some of heir uses in conrol sysem design are covered in he

More information

SOLUTIONS TO ECE 3084

SOLUTIONS TO ECE 3084 SOLUTIONS TO ECE 384 PROBLEM 2.. For each sysem below, specify wheher or no i is: (i) memoryless; (ii) causal; (iii) inverible; (iv) linear; (v) ime invarian; Explain your reasoning. If he propery is no

More information

Section 4.4 Logarithmic Properties

Section 4.4 Logarithmic Properties Secion. Logarihmic Properies 5 Secion. Logarihmic Properies In he previous secion, we derived wo imporan properies of arihms, which allowed us o solve some asic eponenial and arihmic equaions. Properies

More information

Math 116 Practice for Exam 2

Math 116 Practice for Exam 2 Mah 6 Pracice for Exam Generaed Ocober 3, 7 Name: SOLUTIONS Insrucor: Secion Number:. This exam has 5 quesions. Noe ha he problems are no of equal difficuly, so you may wan o skip over and reurn o a problem

More information

CHAPTER 2 Signals And Spectra

CHAPTER 2 Signals And Spectra CHAPER Signals And Specra Properies of Signals and Noise In communicaion sysems he received waveform is usually caegorized ino he desired par conaining he informaion, and he undesired par. he desired par

More information