Including the Consumer Function. 1.0 Constant demand as consumer utility function
|
|
- Megan Quinn
- 5 years ago
- Views:
Transcription
1 Incluin the Consumer Function What we i in the previous notes was solve the cost minimization problem. In these notes, we want to (a) see what such a solution means in the context of solvin a social surplus maximization problem an (b) exten the formulation to inclue eman responsiveness.. Constant eman as consumer utility function In the formulation of our cost minimization problem, we minimize the cost of supply subject to the requirement that the total supply equale the fixe system eman. Here, our only ecision variables were eneration levels, i.e., emans were not ecision variables but rather constants. This implies that eman is insensitive to price, i.e., eman is inelastic. This means that the
2 consumer is not solvin the followin problem: ax U(x)-px () where U is the consumer s utility function (benefit from consumin x), epenent on x which is eman an p which is price, but rather is solvin the followin problem: ax U(x) () That is, the consumer is maximizin utility, which is a function of eman, but the consumer is totally inorin the price when oin so. This is the way most resiential consumers use electricity. The consumer therefore etermines how much eman they will consume via a local ecision-makin problem (e.., What o I nee to o toay ), an the social optimum can be solve treatin the consumer eman as a constant. This means that the consumer eman function is a vertical line, as shown in Fi..
3 price Fi. : Deman function for constant eman Since the consumer eman is a constant, the consumer utility is also a constant. As a result, the social optimum is obtaine via solution of a maximization problem that only inclues enerator cost functions (multiplie by -) in the objective function. This is: ax: ( C k ( q k )) () k Alternatively, the social optimum is obtaine via solution of a minimization problem that only inclues enerator cost functions in the objective function. This is what we i in our LOF, an it is what utility companies have one for years.
4 in: C k ( q k ) () k Now, however, we want to account for the possibility that the consumer will watch their price an ajust their eman as a function of that price. In this case, we must inclue the consumers utilities in the objective function, leain to the objective function use in the formulation for our present problem, which is: ( U ( x ) C ( q )) ax: k k k k (5) k In both cases, we are maximizin the social surplus, the ifference between the consumers utilities an the suppliers costs.. LOF with Consumer Utility As in previous notes on LOF, we brin in network constraints, but this time we will o so with an objective function that maximizes social surplus. In aition, as with our LOF, we will use a piecewise linear approximation of the cost curves with only piece per curve. Thus, each eneration
5 unit an each consumer is represente in the objective function by a constant times the W output for that unit or the W consumption by that consumer. So here is the formal statement of our problem: min Subject to: k s k k + { enerator buses} k { loa buses} s k k (6) ' (7) ( D A) (8) (9), max,max { enerator buses} { loa buses} k k, max, k () 5 k k, max, k () 6 where k k k, k,... N () 7 We want to maximize social surplus as efine by U k - C k, but this is the same as minimizin C k - U k. We make this chane because the L available to us in atlab is a minimizin L. So these are the DC power flow equations to represent the network. However, we must inclue all noal injections, N an all anles N in this set of equations. These are the equation to et the line flows. Aain, we nee to inclue all anles N in this set of equations. These are the limits on the line flows. Notice that there is only one circuit ratin, but it must be enforce as a limit if the flow is in one irection or in the other. 5 These are the limits on the linear cost curve variables. 6 The limits on the linear eman curve variables. 5
6 We ientify the ecision vector as: n bm b n n x ; n n s s s s c () We are now in a position to state the LOF more compactly. ax x c T Subject to: () eq b eq x A, max min x x x (5) where the equality constraints in the A eq matrix equation moel the line flow equations an DC power flow equations. 7 This equation relates the variables use in the cost curves ( kj ) to the variables use in the DC power flow equations ( k ). 6
7 ) ( + A D (6) ' + (7) an the inequality constraints are iven by:,max,max,max,max,max max,max, bm b n n n bm b n n bm ma b (8) Some particular notes about the above problem statement: The upper riht-han m n submatrix of A eq is D A. The lower riht-han n n submatrix of A eq is. 7
8 The riht-han-sie of the equality constraint equation, b eq, is all zeroes because we now have variables for the eman which means it must be inclue in the A eq matrix instea of bein a fixe constant (an therefore represente in the b eq vector).. Example: Unconstraine transmission We illustrate usin an example that is similar to the example use in the LOF notes, which is a combination of previous examples. These are The example use in the notes calle Linear rorammin Approach Usin iecewise Linear Cost Curves where we optimize a unit system, where all units were connecte to the same bus an supplyin a loa at that bus. In this example, we use sements to approximate each cost curve. 8
9 The example in the notes calle The ower Flow Equations where we ha units connecte to ifferent buses in a bus network supplyin loa at ifferent buses. The one-line iaram for the example system is iven in Fi.. y -j y -j y -j y -j y -j Fi. : One line iaram for example system We will use the same ata for the unit costcurves as we i in the LOF notes. These were 9
10 K ( ) s ( ) s ( ) s K K where the eneration variables are in pu an the coefficients are s 7 $/pu-hr s $/pu-hr s 5 $/pu-hr The constraints are 5< < 7.5< <5 5< <8 We will not a the constant factor to the objective function. We will use the followin linearize utility functions for eman: D D ( ) s ( ) s where the loa variables are in per-unit an the coefficients are s - $/pu-hr s - $/pu-hr
11 The constraints are < < < < Objective function: Let s explicitly write out the solution vector. 5 x So, usin these coefficients, the objective function is:
12 ( ) [ ] T x c x Z Equality constraints: The equality constraints are iven in eqs. (6) an (7), repeate here for convenience: ) ( + A D (6) ' + (7) We nee to buil all of these equality constraints into a matrix form of A eq xb eq. We bein by notin imensions. Columns: Since the solution vector x is x, A eq must have columns in orer to pre-multiply x.
13 Rows: Since there are 5 branches, eq. (6) will contribute 5 rows to A eq. Since there are buses, eq. (7) will contribute rows to A eq. So A eq will have total of 9 rows. Therefore, the imensions of A eq will be 9. We bein with the line flow equations, eq. (6). From the notes on ower flow equations, we can recall the D an A matrix. The D matrix is exactly the same as before, which is: D An the noe-arc incience matrix, A, is:
14 - - A The DxA prouce require by eq. () is then iven by: - - A D So base on eq. () an the solution vector, we can see that these elements will occupy the upper riht han corner of A eq. So that will take care of the last columns in the first 5 rows. ut what about the first columns? These are the elements in the line flow equations that multiply the variables,,,,,,,,, 5. Since we o not use the eneration or eman variables within the line flow
15 equations, the first 5 columns of these top 5 rows will be zeros. The last 5 columns in these top 5 rows will also be zeros, except the one element in each of these rows that multiply the corresponin line flow variable, an that element will be -. Finally, with respect to these top 5 equations, eq. (6) inicates that the rihthan-sie will be for each of them. Thus, we can now write own all elements in the first 5 rows of our matrix, as follows: 5
16 5 eq x A Now we nee to write the last equations. These are the DC power flow equations corresponin to eq. (7). Aain, we must remember that the solution vector contains all anles, an therefore the DC power flow matrix nees to be a x. This aumente DC power flow matrix is iven below: 6
17 ' So base on eq. (7) an the solution vector, we can see that this matrix will occupy the lower riht han sie of the A eq matrix. So that will take care of the last columns in the bottom rows. The resultin matrix appears as: 5 eq x A 7
18 Once aain, we nee to consier the first eiht columns. Columns 6- correspon to the line flow variables, which o not appear in the DC power flow equations, so these will be zero. 5 eq x A The first three columns multiply the eneration variables,, an, an columns an 5 multiply the loa variables an. However, the DC power flow equations, eq. (7), require the neative of the injections for all buses, an the injections are the 8
19 eneration minus the loa, i.e., k - k. So we want to moel k + k on the left-hansie in the last rows. This will be one by placin a - an + in the appropriate place. 5 eq x A Inequality constraints: The inequality constraints are simple, as iven below. Notice that the -5 to 5 constraints on line flows imply we are moelin no transmission constraints. 9
20 Solution by atlab: The coe for solvin this linear proram usin atlab is iven below: %uil objective function vector. c[ ]'; %uil A matrix for inequality constraints Ax<b. A[]; %uil b, the riht-han-sie of inequality constraints. b[]; %uil Aeq matrix for equality constraints.
21 Aeq[ - -; - - ; - - ; - - ; - - ; ; - - -; ;]; %uil riht-han sie of equality constraint. It will be vector of zeros beqzeros(9,); %uil upper an lower bouns on ecision variables. L[ pi -pi -pi -pi]'; U[ pi pi pi pi]'; [X,FVAL,EXITFLAG,OUTUT,LADA]LINROG(c,A,b,Aeq,beq,L,U); %'X', X,FVAL,'eqaulity', LADA.eqlin, 'upper', LADA.upper, 'lower', LADA.lower % % Compute the ollars pai to each participant: ollarsc.*x; %Write out the ollars pai to each participant ollars The solution vector x is iven below. The limits on the variables are also repeate here so that it is easy to see which ones are at their limit.
22
23 One can easily check to see that the power is conserve at the buses. Objective function value: The objective function that atlab provies (FVAL) is Z-.8 $/hr. This is neative of the social surplus (atlab requires all problems to be minimization problems, so we ha to minimize the neative of the social surplus in orer to maximize social surplus). So the social surplus (Total Utility of Loa less Total Cost of Supply) is $.8. Not too much! This is because the emaners are valuin the enery at just a little above cost. If we chane the utility function coefficients to -5 an -, from - an -, respectively, the social surplus woul chane to $9/hr. If we chane utility function coefficients to - an -9, respectively, the social surplus woul be -$9/hr, inicatin the cost of supply is more than the utility of
24 consumption, an the only reason any power is bein consume is the lower boun constraints we have place on eneration an eman. Larane multipliers: Now let s investiate Larane multipliers for this case, assumin infinite capacity lines. These Larane multipliers (the same as the ual variables), are iven in Table. Table : Larane multipliers for infinite transmission capacity Equality constraints Lower bouns Upper bouns Equation Value* Variable value variable value
25 Larane multipliers on the last equality constraints are very interestin, since they ive the improvement in the objective function if we increase the riht-han-sie of the corresponin equation by unit. These are the noal prices, iven in $/per unit-hr. The numbers are all $/per unithr; if we ivie this by the power base ( VA), we et $./W-hr. This is also the coefficient of the eman at bus,. Now let s consier the Larane multipliers: Lower bouns: an are non-zero, inicatin they are at their lower bouns, as confirme by ecision vector on p.. Upper bouns: an are non-zero, inicatin they are at their upper bouns, as confirme by ecision vector on p.. Not constraine (reulatin): Only has Larane multipliers for both lower an upper bouns, inicatin it is not at either boun (this variable is reulatin ). 5
26 Connection! There is only ONE unconstraine variable,, an it is also the variable that is settin the noal prices ($./W-hr) throuhout the network! A look at the coefficients will show why: s $/pu-hr s - $/pu-hr s 5 $/pu-hr s - $/pu-hr s 7 $/pu-hr Think of the alorithm like this: It first sets eneration an loa at lower limits (there is no choice about this much supply an eman). One variable must come off its lower boun in orer to provie power balance. Since sum of loa lower bouns is, an sum of en lower bouns is.7, one or more of the ens must come off their lower bouns by.6 in orer to provie a feasible solution. This en will be the least expensive one(s). In this case, it is G an G. (G ets pushe to its limit in this step) Then it takes a W of supply an a W of eman from the en/loa pair that is not at 6
27 upper bouns an provies the most positive surplus. This will be the en with the least cost an the loa with the reatest utility, as lon as the surplus is positive. In our example, the first en/loa pair taken, after finin a feasible solution, are G/D. As soon as either the en or the loa of the max-surplus en/loa pair reaches its upper limit, it will replace that en or loa with the one that yiels the next larest surplus. In our case, G reaches its upper limit first, an it tries to replace it with G. ut the G/D pair has coefficients that result in a neative surplus! So the maximum surplus is foun when G reaches its upper limit. You shoul be able to see that the alorithm will always terminate with just one en or loa reulatin, an that en or loa will set the noal price throuhout the network (for the unconstraine transmission case). 7
28 Settlement: The cost (for suppliers) an the utility (for the emaners) of the market equilibrium are compute by multiplyin the cost coefficient (in the vector c) by the amount of W bouht or sol (in the vector X). In atlab, this can be achieve by usin the vectorize multiplication function c.*x. The result of oin this is in Table. Table : Unconstraine case Cost or utility ($/hr) K ( ) s 65.5 K ( ) s 86.5 K ( ) s 57. D ( ) s -. D ( ) s -. However, this is not the settlement. The settlement is the ollars actually pai by the emaners an to the suppliers. The settlement epens on the noal prices, as iven in Table. The cost & utility is also 8
29 provie in Table so that the supplier an consumer benefit may be etermine. Table : Unconstraine case col col col col col5 k or k Cost or utility λ k ($/mwhr) λ k * k or enefit col- col ($/hr) λ k * k Observe the followin:. The sum of col is neative. This is because we are efinin eneration costs as positive an eman utility as neative. So we have more utility than cost, a esirable situation.. Col5 ives benefit, which shoul sum to have a sin opposite to that of col 9
30 since col is the neative of social surplus (or social benefit).. So the social surplus is the same as the total social benefit, an this is the same as the objective function.. Example: Constraine transmission We will constrain the transmission on branch. Reference to the ol solution of Fi., repeate here for convenience, inicates that the flow on branch is.65. So we will constrain that flow to be.6.
31 .5pu.5pu pu pu.pu The atlab coe for this is iven below. %uil objective function vector. c[ ]'; %uil A matrix for inequality constraints Ax<b. A[]; %uil b, the riht-han-sie of inequality constraints. b[]; %uil Aeq matrix for equality constraints. Aeq[ - -; - - ; - - ; - - ; - - ; ; - - -; ;]; %uil riht-han sie of equality constraint. It will be vector of zeros beqzeros(9,); %uil upper an lower bouns on ecision variables. L[ pi -pi -pi -pi]'; U[ pi pi pi pi]'; [X,FVAL,EXITFLAG,OUTUT,LADA]LINROG(c,A,b,Aeq,beq,L,U);
32 %'X', X,FVAL,'eqaulity', LADA.eqlin, 'upper', LADA.upper, 'lower', LADA.lower % % Compute the ollars pai to each participant: ollarsc.*x; %Write out the ollars pai to each participant ollars The new an the ol ecision vectors are provie below, toether with the limits. New solution Ol solution Limits
33 The new solution is provie in Fi pu.pu.867pu.5pu.8pu Fi.
34 Objective function value: The objective function that atlab provie (FVAL) in the unconstraine case was Z-.8 $/hr (social surplus of $.8/hr). Now in the constraine case it is Z-$.75/hr (social surplus of $.75/hr). The social surplus has ecrease, confirmin the principle that ain new constraints can never result in an improvement in the objective function. Larane multipliers: The Larane multipliers (the same as the ual variables), are iven in Table.
35 Table : Larane multipliers for constraine transmission capacity Equality constraints Lower bouns Upper bouns Equation Value* Variable value variable value Some observations:.in the unconstraine case, all four noal prices were $/Whr, now, in the constraine case, only bus is $/Whr (set by ), which is a reulatin (not at a limit) unit. An all of the remainin noal prices are ifferent. 5
36 . is also reulatin, an therefore the bus noal price is set by the bi which was $.7/hr..uses an have loa or eneration at a limit. us has at its lower limit, an bus has at its upper limit. So neither of these buses are reulatin. Notice that the noal prices at these buses are ifferent from the cost or utility function coefficient at the bus: us has utility function coefficient of whereas its L is.7 us has cost function coefficient of 5 whereas its L is 9.. This shows that buses with reulatin units or emans set their own price, whereas non-reulatin buses have prices set by other buses in the network..if there were no binin transmission constraints (effectively an infinite transmission capacity situation), then the prices at buses an woul be set by one other bus in the network. ut with a 6
37 binin transmission constraint (i.e., presence of conestion), then the prices will be set by the units neee to supply an aitional W at the bus AND maintain flow within the limit. As we have seen before, this will necessarily involve more than one unit. Settlement: The cost (for suppliers) an the utility (for the emaners) of the market equilibrium are compute by multiplyin the cost coefficient (in the vector c) by the amount of W bouht or sol (in the vector X). In atlab, this can be achieve by usin the vectorize multiplication function c.*x. The result of oin this is in Table. This result is also compare to that of the unconstaine case to illustrate. 7
38 Table : Constraine case Constraine Case ($/hr) Unconstraine Case ($/hr) K s ( ) K ( ) s K ( ) s D ( ) s D ( ) s However, this is not the settlement. The settlement is the ollars actually pai by the emaners an to the suppliers. The settlement epens on the noal prices, as compute in Table. The cost & utility is also provie in Table so that the supplier an consumer benefit may be etermine. 8
39 Table : Unconstraine case col col col col col5 k or k Cost or utility λ k ($/mwhr) λ k * k or enefit col- col ($/hr) λ k * k I think that the col shoul be Why it is not I o not know. Some error here.rounoff? ut note the value of the col5. This is the amount of benefit. It is NOT the same as the objective. Why? ecause the conestion rents must be pai as well, in this case, it is clear that they are $.5. 9
Linearized optimal power flow
Linearized optimal power flow. Some introductory comments The advantae of the economic dispatch formulation to obtain minimum cost allocation of demand to the eneration units is that it is computationally
More informationDirect Computation of Generator Internal Dynamic States from Terminal Measurements
Direct Computation of Generator nternal Dynamic States from Terminal Measurements aithianathan enkatasubramanian Rajesh G. Kavasseri School of Electrical En. an Computer Science Dept. of Electrical an
More informationTorque OBJECTIVE INTRODUCTION APPARATUS THEORY
Torque OBJECTIVE To verify the rotational an translational conitions for equilibrium. To etermine the center of ravity of a rii boy (meter stick). To apply the torque concept to the etermination of an
More informationPRACTICE 4. CHARGING AND DISCHARGING A CAPACITOR
PRACTICE 4. CHARGING AND DISCHARGING A CAPACITOR. THE PARALLEL-PLATE CAPACITOR. The Parallel plate capacitor is a evice mae up by two conuctor parallel plates with total influence between them (the surface
More informationState-Space Model for a Multi-Machine System
State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal
More informationAnalysis of Halo Implanted MOSFETs
Analysis of alo Implante MOSFETs olin McAnrew an Patrick G Drennan Freescale Semiconuctor, Tempe, AZ, olinmcanrew@freescalecom ABSTAT MOSFETs with heavily ope reions at one or both ens of the channel exhibit
More informationLinear First-Order Equations
5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)
More informationMath 342 Partial Differential Equations «Viktor Grigoryan
Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite
More informationTable of Common Derivatives By David Abraham
Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec
More informationUnit #6 - Families of Functions, Taylor Polynomials, l Hopital s Rule
Unit # - Families of Functions, Taylor Polynomials, l Hopital s Rule Some problems an solutions selecte or aapte from Hughes-Hallett Calculus. Critical Points. Consier the function f) = 54 +. b) a) Fin
More informationJUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson
JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises
More informationApplying Axiomatic Design Theory to the Multi-objective Optimization of Disk Brake *
Applyin Aiomatic esin Theory to the Multi-objective Optimization of isk Brake * Zhiqian Wu Xianfu Chen an Junpin Yuan School of Mechanical an Electronical Enineerin East China Jiaoton University Nanchan
More informationUsing Quasi-Newton Methods to Find Optimal Solutions to Problematic Kriging Systems
Usin Quasi-Newton Methos to Fin Optimal Solutions to Problematic Kriin Systems Steven Lyster Centre for Computational Geostatistics Department of Civil & Environmental Enineerin University of Alberta Solvin
More information19 Eigenvalues, Eigenvectors, Ordinary Differential Equations, and Control
19 Eigenvalues, Eigenvectors, Orinary Differential Equations, an Control This section introuces eigenvalues an eigenvectors of a matrix, an iscusses the role of the eigenvalues in etermining the behavior
More informationQubit channels that achieve capacity with two states
Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March
More informationMath 1B, lecture 8: Integration by parts
Math B, lecture 8: Integration by parts Nathan Pflueger 23 September 2 Introuction Integration by parts, similarly to integration by substitution, reverses a well-known technique of ifferentiation an explores
More informationPhysics 2212 K Quiz #2 Solutions Summer 2016
Physics 1 K Quiz # Solutions Summer 016 I. (18 points) A positron has the same mass as an electron, but has opposite charge. Consier a positron an an electron at rest, separate by a istance = 1.0 nm. What
More informationDesigning Information Devices and Systems I Spring 2018 Lecture Notes Note 16
EECS 16A Designing Information Devices an Systems I Spring 218 Lecture Notes Note 16 16.1 Touchscreen Revisite We ve seen how a resistive touchscreen works by using the concept of voltage iviers. Essentially,
More informationSituation awareness of power system based on static voltage security region
The 6th International Conference on Renewable Power Generation (RPG) 19 20 October 2017 Situation awareness of power system base on static voltage security region Fei Xiao, Zi-Qing Jiang, Qian Ai, Ran
More informationby using the derivative rules. o Building blocks: d
Calculus for Business an Social Sciences - Prof D Yuen Eam Review version /9/01 Check website for any poste typos an upates Eam is on Sections, 5, 6,, 1,, Derivatives Rules Know how to fin the formula
More informationFinal Exam Study Guide and Practice Problems Solutions
Final Exam Stuy Guie an Practice Problems Solutions Note: These problems are just some of the types of problems that might appear on the exam. However, to fully prepare for the exam, in aition to making
More informationMath Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors
Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+
More informationDAMAGE LOCALIZATION IN OUTPUT-ONLY SYSTEMS: A FLEXIBILITY BASED APPROACH
DAAG LOCALIZAION IN OUPU-ONLY SYSS: A LXIBILIY BASD APPROACH Dionisio Bernal an Burcu Gunes Department of Civil an nvironmental nineerin, 47 Snell nineerin Center, Northeastern University, Boston A 0115,
More informationWeb Appendix to Firm Heterogeneity and Aggregate Welfare (Not for Publication)
Web ppeni to Firm Heterogeneity an ggregate Welfare Not for Publication Marc J. Melitz Harvar University, NBER, an CEPR Stephen J. Reing Princeton University, NBER, an CEPR March 6, 203 Introuction his
More informationSTABILITY ESTIMATES FOR SOLUTIONS OF A LINEAR NEUTRAL STOCHASTIC EQUATION
TWMS J. Pure Appl. Math., V.4, N.1, 2013, pp.61-68 STABILITY ESTIMATES FOR SOLUTIONS OF A LINEAR NEUTRAL STOCHASTIC EQUATION IRADA A. DZHALLADOVA 1 Abstract. A linear stochastic functional ifferential
More informationChapter 3 Notes, Applied Calculus, Tan
Contents 3.1 Basic Rules of Differentiation.............................. 2 3.2 The Prouct an Quotient Rules............................ 6 3.3 The Chain Rule...................................... 9 3.4
More informationLectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs
Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent
More informationStructures of lubrication type PILLOBALLs. Structures of maintenance-free type PILLOBALLs. Outer ring. Bushing (Special copper alloy)
PILLOBALL Spherical Bushins - Insert PILLOBALL Ro Ens - Insert PILLOBALL Ro Ens - Die-cast PILLOBALL Ro Ens - Maintenance-free Structure an Features PILLOBALLs are compact self-alinin spherical bushins
More informationModule 2. DC Circuit. Version 2 EE IIT, Kharagpur
Moule 2 DC Circuit Lesson 9 Analysis of c resistive network in presence of one non-linear element Objectives To unerstan the volt (V ) ampere ( A ) characteristics of linear an nonlinear elements. Concept
More informationA Course in Machine Learning
A Course in Machine Learning Hal Daumé III 12 EFFICIENT LEARNING So far, our focus has been on moels of learning an basic algorithms for those moels. We have not place much emphasis on how to learn quickly.
More informationBENFORD S LAW AND HOSMER-LEMESHOW TEST
Journal of Mathematical Sciences: Avances an Applications Volume 4, 6, Paes 57-73 Availale at http://scientificavancescoin DI: http://xoior/864/jmsaa_778 BFRD S LAW AD SMR-LMSW TST ZRA JASAK LB Banka Sarajevo
More informationSystems of Linear Equations in Two Variables. Break Even. Example. 240x x This is when total cost equals total revenue.
Systems of Linear Equations in Two Variables 1 Break Even This is when total cost equals total revenue C(x) = R(x) A company breaks even when the profit is zero P(x) = R(x) C(x) = 0 2 R x 565x C x 6000
More informationDiophantine Approximations: Examining the Farey Process and its Method on Producing Best Approximations
Diophantine Approximations: Examining the Farey Process an its Metho on Proucing Best Approximations Kelly Bowen Introuction When a person hears the phrase irrational number, one oes not think of anything
More informationand from it produce the action integral whose variation we set to zero:
Lagrange Multipliers Monay, 6 September 01 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine
More informationLagrangian and Hamiltonian Mechanics
Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical
More informationSome vector algebra and the generalized chain rule Ross Bannister Data Assimilation Research Centre, University of Reading, UK Last updated 10/06/10
Some vector algebra an the generalize chain rule Ross Bannister Data Assimilation Research Centre University of Reaing UK Last upate 10/06/10 1. Introuction an notation As we shall see in these notes the
More informationSurvey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013
Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing
More information7.1 Support Vector Machine
67577 Intro. to Machine Learning Fall semester, 006/7 Lecture 7: Support Vector Machines an Kernel Functions II Lecturer: Amnon Shashua Scribe: Amnon Shashua 7. Support Vector Machine We return now to
More informationThe Uniqueness of the Overall Assurance Interval for Epsilon in DEA Models by the Direction Method
Available online at http://nrm.srbiau.ac.ir Vol., No., Summer 5 Journal of New Researches in Mathematics Science an Research Branch (IAU) he Uniqueness of the Overall Assurance Interval for Epsilon in
More informationHomework 7 Due 18 November at 6:00 pm
Homework 7 Due 18 November at 6:00 pm 1. Maxwell s Equations Quasi-statics o a An air core, N turn, cylinrical solenoi of length an raius a, carries a current I Io cos t. a. Using Ampere s Law, etermine
More informationMake graph of g by adding c to the y-values. on the graph of f by c. multiplying the y-values. even-degree polynomial. graph goes up on both sides
Reference 1: Transformations of Graphs an En Behavior of Polynomial Graphs Transformations of graphs aitive constant constant on the outsie g(x) = + c Make graph of g by aing c to the y-values on the graph
More informationMathcad Lecture #5 In-class Worksheet Plotting and Calculus
Mathca Lecture #5 In-class Worksheet Plotting an Calculus At the en of this lecture, you shoul be able to: graph expressions, functions, an matrices of ata format graphs with titles, legens, log scales,
More informationComputing Exact Confidence Coefficients of Simultaneous Confidence Intervals for Multinomial Proportions and their Functions
Working Paper 2013:5 Department of Statistics Computing Exact Confience Coefficients of Simultaneous Confience Intervals for Multinomial Proportions an their Functions Shaobo Jin Working Paper 2013:5
More informationELECTRON DIFFRACTION
ELECTRON DIFFRACTION Electrons : wave or quanta? Measurement of wavelength an momentum of electrons. Introuction Electrons isplay both wave an particle properties. What is the relationship between the
More informationLecture 22. Lecturer: Michel X. Goemans Scribe: Alantha Newman (2004), Ankur Moitra (2009)
8.438 Avance Combinatorial Optimization Lecture Lecturer: Michel X. Goemans Scribe: Alantha Newman (004), Ankur Moitra (009) MultiFlows an Disjoint Paths Here we will survey a number of variants of isjoint
More informationinflow outflow Part I. Regular tasks for MAE598/494 Task 1
MAE 494/598, Fall 2016 Project #1 (Regular tasks = 20 points) Har copy of report is ue at the start of class on the ue ate. The rules on collaboration will be release separately. Please always follow the
More informationA simple model for the small-strain behaviour of soils
A simple moel for the small-strain behaviour of soils José Jorge Naer Department of Structural an Geotechnical ngineering, Polytechnic School, University of São Paulo 05508-900, São Paulo, Brazil, e-mail:
More informationLinear and quadratic approximation
Linear an quaratic approximation November 11, 2013 Definition: Suppose f is a function that is ifferentiable on an interval I containing the point a. The linear approximation to f at a is the linear function
More informationCapacitance and Dielectrics
3/30/05 apacitance an Dielectrics Goals of this Lecture To unerstan capacitors an calculate capacitance To analyze networks of capacitors To calculate the enery store in a capacitor To examine ielectrics
More informationECE 422 Power System Operations & Planning 7 Transient Stability
ECE 4 Power System Operations & Planning 7 Transient Stability Spring 5 Instructor: Kai Sun References Saaat s Chapter.5 ~. EPRI Tutorial s Chapter 7 Kunur s Chapter 3 Transient Stability The ability of
More informationImplicit Differentiation
Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,
More informationETNA Kent State University
% w Electronic Transactions on Numerical Analysis. Volume 21, pp. 35-42, 2005. Copyriht 2005,. ISSN 1068-9613. QR FACTORIZATIONS USING A RESTRICTED SET OF ROTATIONS DIANNE P. O LEARY AND STEPHEN S. BULLOCK
More informationCalculus and optimization
Calculus an optimization These notes essentially correspon to mathematical appenix 2 in the text. 1 Functions of a single variable Now that we have e ne functions we turn our attention to calculus. A function
More informationG j dq i + G j. q i. = a jt. and
Lagrange Multipliers Wenesay, 8 September 011 Sometimes it is convenient to use reunant coorinates, an to effect the variation of the action consistent with the constraints via the metho of Lagrange unetermine
More informationLecture 6: Calculus. In Song Kim. September 7, 2011
Lecture 6: Calculus In Song Kim September 7, 20 Introuction to Differential Calculus In our previous lecture we came up with several ways to analyze functions. We saw previously that the slope of a linear
More informationSchrödinger s equation.
Physics 342 Lecture 5 Schröinger s Equation Lecture 5 Physics 342 Quantum Mechanics I Wenesay, February 3r, 2010 Toay we iscuss Schröinger s equation an show that it supports the basic interpretation of
More informationARCH 614 Note Set 5 S2012abn. Moments & Supports
RCH 614 Note Set 5 S2012abn Moments & Supports Notation: = perpenicular istance to a force from a point = name for force vectors or magnitue of a force, as is P, Q, R x = force component in the x irection
More informationThe Ehrenfest Theorems
The Ehrenfest Theorems Robert Gilmore Classical Preliminaries A classical system with n egrees of freeom is escribe by n secon orer orinary ifferential equations on the configuration space (n inepenent
More informationUnit #4 - Inverse Trig, Interpreting Derivatives, Newton s Method
Unit #4 - Inverse Trig, Interpreting Derivatives, Newton s Metho Some problems an solutions selecte or aapte from Hughes-Hallett Calculus. Computing Inverse Trig Derivatives. Starting with the inverse
More informationQuantum Search on the Spatial Grid
Quantum Search on the Spatial Gri Matthew D. Falk MIT 2012, 550 Memorial Drive, Cambrige, MA 02139 (Date: December 11, 2012) This paper explores Quantum Search on the two imensional spatial gri. Recent
More information2Algebraic ONLINE PAGE PROOFS. foundations
Algebraic founations. Kick off with CAS. Algebraic skills.3 Pascal s triangle an binomial expansions.4 The binomial theorem.5 Sets of real numbers.6 Surs.7 Review . Kick off with CAS Playing lotto Using
More informationII. First variation of functionals
II. First variation of functionals The erivative of a function being zero is a necessary conition for the etremum of that function in orinary calculus. Let us now tackle the question of the equivalent
More informationMathematical Foundations -1- Constrained Optimization. Constrained Optimization. An intuitive approach 2. First Order Conditions (FOC) 7
Mathematical Foundations -- Constrained Optimization Constrained Optimization An intuitive approach First Order Conditions (FOC) 7 Constraint qualifications 9 Formal statement of the FOC for a maximum
More informationMath 115 Section 018 Course Note
Course Note 1 General Functions Definition 1.1. A function is a rule that takes certain numbers as inputs an assigns to each a efinite output number. The set of all input numbers is calle the omain of
More informationANALYZE In all three cases (a) (c), the reading on the scale is. w = mg = (11.0 kg) (9.8 m/s 2 ) = 108 N.
Chapter 5 1. We are only concerned with horizontal forces in this problem (ravity plays no direct role). We take East as the +x direction and North as +y. This calculation is efficiently implemented on
More information23 Implicit differentiation
23 Implicit ifferentiation 23.1 Statement The equation y = x 2 + 3x + 1 expresses a relationship between the quantities x an y. If a value of x is given, then a corresponing value of y is etermine. For
More information2-7. Fitting a Model to Data I. A Model of Direct Variation. Lesson. Mental Math
Lesson 2-7 Fitting a Moel to Data I BIG IDEA If you etermine from a particular set of ata that y varies irectly or inversely as, you can graph the ata to see what relationship is reasonable. Using that
More informationMatrix multiplication: a group-theoretic approach
CSG399: Gems of Theoretical Computer Science. Lec. 21-23. Mar. 27-Apr. 3, 2009. Instructor: Emanuele Viola Scribe: Ravi Sundaram Matrix multiplication: a roup-theoretic approach Given two n n matrices
More informationELEC3114 Control Systems 1
ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.
More information1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.
Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency
More informationPower Generation and Distribution via Distributed Coordination Control
Power Generation an Distribution via Distribute Coorination Control Byeong-Yeon Kim, Kwang-Kyo Oh, an Hyo-Sung Ahn arxiv:407.4870v [math.oc] 8 Jul 204 Abstract This paper presents power coorination, power
More informationTHE ACCURATE ELEMENT METHOD: A NEW PARADIGM FOR NUMERICAL SOLUTION OF ORDINARY DIFFERENTIAL EQUATIONS
THE PUBISHING HOUSE PROCEEDINGS O THE ROMANIAN ACADEMY, Series A, O THE ROMANIAN ACADEMY Volume, Number /, pp. 6 THE ACCURATE EEMENT METHOD: A NEW PARADIGM OR NUMERICA SOUTION O ORDINARY DIERENTIA EQUATIONS
More informationAssignment 1. g i (x 1,..., x n ) dx i = 0. i=1
Assignment 1 Golstein 1.4 The equations of motion for the rolling isk are special cases of general linear ifferential equations of constraint of the form g i (x 1,..., x n x i = 0. i=1 A constraint conition
More information2.2 Differentiation and Integration of Vector-Valued Functions
.. DIFFERENTIATION AND INTEGRATION OF VECTOR-VALUED FUNCTIONS133. Differentiation and Interation of Vector-Valued Functions Simply put, we differentiate and interate vector functions by differentiatin
More informationOPTIMAL CONTROL OF A PRODUCTION SYSTEM WITH INVENTORY-LEVEL-DEPENDENT DEMAND
Applie Mathematics E-Notes, 5(005), 36-43 c ISSN 1607-510 Available free at mirror sites of http://www.math.nthu.eu.tw/ amen/ OPTIMAL CONTROL OF A PRODUCTION SYSTEM WITH INVENTORY-LEVEL-DEPENDENT DEMAND
More informationTMA 4195 Matematisk modellering Exam Tuesday December 16, :00 13:00 Problems and solution with additional comments
Problem F U L W D g m 3 2 s 2 0 0 0 0 2 kg 0 0 0 0 0 0 Table : Dimension matrix TMA 495 Matematisk moellering Exam Tuesay December 6, 2008 09:00 3:00 Problems an solution with aitional comments The necessary
More informationThis section outlines the methodology used to calculate the wave load and wave wind load values.
COMPUTERS AND STRUCTURES, INC., JUNE 2014 AUTOMATIC WAVE LOADS TECHNICAL NOTE CALCULATION O WAVE LOAD VALUES This section outlines the methoology use to calculate the wave loa an wave win loa values. Overview
More informationOn the enumeration of partitions with summands in arithmetic progression
AUSTRALASIAN JOURNAL OF COMBINATORICS Volume 8 (003), Pages 149 159 On the enumeration of partitions with summans in arithmetic progression M. A. Nyblom C. Evans Department of Mathematics an Statistics
More informationOptimization of Geometries by Energy Minimization
Optimization of Geometries by Energy Minimization by Tracy P. Hamilton Department of Chemistry University of Alabama at Birmingham Birmingham, AL 3594-140 hamilton@uab.eu Copyright Tracy P. Hamilton, 1997.
More informationThermal conductivity of graded composites: Numerical simulations and an effective medium approximation
JOURNAL OF MATERIALS SCIENCE 34 (999)5497 5503 Thermal conuctivity of grae composites: Numerical simulations an an effective meium approximation P. M. HUI Department of Physics, The Chinese University
More informationLecture 1b. Differential operators and orthogonal coordinates. Partial derivatives. Divergence and divergence theorem. Gradient. A y. + A y y dy. 1b.
b. Partial erivatives Lecture b Differential operators an orthogonal coorinates Recall from our calculus courses that the erivative of a function can be efine as f ()=lim 0 or using the central ifference
More informationLATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION
The Annals of Statistics 1997, Vol. 25, No. 6, 2313 2327 LATTICE-BASED D-OPTIMUM DESIGN FOR FOURIER REGRESSION By Eva Riccomagno, 1 Rainer Schwabe 2 an Henry P. Wynn 1 University of Warwick, Technische
More information1 CHAPTER 7 PROJECTILES. 7.1 No Air Resistance
CHAPTER 7 PROJECTILES 7 No Air Resistance We suppose that a particle is projected from a point O at the oriin of a coordinate system, the y-axis bein vertical and the x-axis directed alon the round The
More informationPARALLEL-PLATE CAPACITATOR
Physics Department Electric an Magnetism Laboratory PARALLEL-PLATE CAPACITATOR 1. Goal. The goal of this practice is the stuy of the electric fiel an electric potential insie a parallelplate capacitor.
More informationMA 2232 Lecture 08 - Review of Log and Exponential Functions and Exponential Growth
MA 2232 Lecture 08 - Review of Log an Exponential Functions an Exponential Growth Friay, February 2, 2018. Objectives: Review log an exponential functions, their erivative an integration formulas. Exponential
More informationBalancing Expected and Worst-Case Utility in Contracting Models with Asymmetric Information and Pooling
Balancing Expecte an Worst-Case Utility in Contracting Moels with Asymmetric Information an Pooling R.B.O. erkkamp & W. van en Heuvel & A.P.M. Wagelmans Econometric Institute Report EI2018-01 9th January
More informationSturm-Liouville Theory
LECTURE 5 Sturm-Liouville Theory In the three preceing lectures I emonstrate the utility of Fourier series in solving PDE/BVPs. As we ll now see, Fourier series are just the tip of the iceberg of the theory
More informationFluid Pressure and Fluid Force
SECTION 7.7 Flui Pressure an Flui Force 07 Section 7.7 Flui Pressure an Flui Force Fin flui pressure an flui force. Flui Pressure an Flui Force Swimmers know that the eeper an object is submerge in a flui,
More informationLower Bounds for the Smoothed Number of Pareto optimal Solutions
Lower Bouns for the Smoothe Number of Pareto optimal Solutions Tobias Brunsch an Heiko Röglin Department of Computer Science, University of Bonn, Germany brunsch@cs.uni-bonn.e, heiko@roeglin.org Abstract.
More informationLecture 6: Control of Three-Phase Inverters
Yoash Levron The Anrew an Erna Viterbi Faculty of Electrical Engineering, Technion Israel Institute of Technology, Haifa 323, Israel yoashl@ee.technion.ac.il Juri Belikov Department of Computer Systems,
More informationGoal of this chapter is to learn what is Capacitance, its role in electronic circuit, and the role of dielectrics.
PHYS 220, Engineering Physics, Chapter 24 Capacitance an Dielectrics Instructor: TeYu Chien Department of Physics an stronomy University of Wyoming Goal of this chapter is to learn what is Capacitance,
More informationStatic Equilibrium. Theory: The conditions for the mechanical equilibrium of a rigid body are (a) (b)
LPC Physics A 00 Las Positas College, Physics Department Staff Purpose: To etermine that, for a boy in equilibrium, the following are true: The sum of the torques about any point is zero The sum of forces
More informationCalculus of Variations
16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t
More informationHomework 2 Solutions EM, Mixture Models, PCA, Dualitys
Homewor Solutions EM, Mixture Moels, PCA, Dualitys CMU 0-75: Machine Learning Fall 05 http://www.cs.cmu.eu/~bapoczos/classes/ml075_05fall/ OUT: Oct 5, 05 DUE: Oct 9, 05, 0:0 AM An EM algorithm for a Mixture
More information7.5 Performance of Convolutional Codes General Comments
7.5 Performance of Convolutional Coes 7.5-1 7.5.1 General Comments Convolutional coes expan the banwith for a fixe information rate, or lower the information rate for a fixe banwith. We hope for some error
More informationMechanics Physics 151
Mechanics Physics 151 Lecture 3 Continuous Systems an Fiels (Chapter 13) Where Are We Now? We ve finishe all the essentials Final will cover Lectures 1 through Last two lectures: Classical Fiel Theory
More informationAnalytic Scaling Formulas for Crossed Laser Acceleration in Vacuum
October 6, 4 ARDB Note Analytic Scaling Formulas for Crosse Laser Acceleration in Vacuum Robert J. Noble Stanfor Linear Accelerator Center, Stanfor University 575 San Hill Roa, Menlo Park, California 945
More informationOn the Aloha throughput-fairness tradeoff
On the Aloha throughput-fairness traeoff 1 Nan Xie, Member, IEEE, an Steven Weber, Senior Member, IEEE Abstract arxiv:1605.01557v1 [cs.it] 5 May 2016 A well-known inner boun of the stability region of
More informationθ x = f ( x,t) could be written as
9. Higher orer PDEs as systems of first-orer PDEs. Hyperbolic systems. For PDEs, as for ODEs, we may reuce the orer by efining new epenent variables. For example, in the case of the wave equation, (1)
More informationQuantum Mechanics in Three Dimensions
Physics 342 Lecture 20 Quantum Mechanics in Three Dimensions Lecture 20 Physics 342 Quantum Mechanics I Monay, March 24th, 2008 We begin our spherical solutions with the simplest possible case zero potential.
More information