Determinant and Trace
|
|
- Bertha McCoy
- 5 years ago
- Views:
Transcription
1 Determinant an Trace Area an mappings from the plane to itself: Recall that in the last set of notes we foun a linear mapping to take the unit square S = {, y } to any parallelogram P with one corner at the origin. We can write the parallelogram P as P = {v + yw :, y }, where v an w are the two vectors which form the eges of P starting at the origin (, ). Then we can write the linear transformation as ([ ) [ v w T = v + yw, [T =, y v 2 w 2 where v = (v, v 2 ) an w = (w, w 2 ) in components. Notice that the mapping T is invertile precisely when it oes not collapse S own to a line segment (or a point), which happens precisely when the area of the parallelogram P is non-zero. Also, recall that we sai T is invertile precisely when its eterminant et([t ) = v w 2 v 2 w 2 is nonzero. We have et([t ) T invertile Area(P ). We ll see net that et([t ) is the area of P, up to a sign. This is easiest to see with the shear map we eamine in the last set of notes. Start with the sheer map T whose matri representation is [ [T =. (In the earlier set of notes we wrote the entry in the upper right corner of [T as a, ut it will turn out to e convenient to call it for our later iscussion.) In this case, T maps the unit [ square S = {, y } to the parallelogram P spanne y the two vectors v = an [ w = ; in other wors, T (S) = P = {v + yw :, y } = We reprouce a picture here: { [ [ + y } :, y. Area = (, ) Area = (, ) We alreay know that the unit square S has area, ut let s see that P also has area. The area of a parallelogram is equal to its ase times its height, an the height an ase of P are oth, so the area of P is =. On the other han, ([ ) et([t ) = et = = = Area(P ).
2 Now we can rescale the sheer T y a in the horizontal irection an y an vertical irection, to have something more general. This time we have [ a [T =, an T (S) = P = {v + yw :, y } = an the picture looks like { [ a [ + y } :, y, (, ) Area = (a, ) Area = a (In this particular picture a = /2 an = 2, ut this choice of scaling factors is not important.) This time the height of the parallelogram P is while its ase is a, so Area(P ) = ase height = a. Again, we have ([ ) et([t ) = a et = a = a = Area(P ). Notice that the asolute value here is necessary, ecause a an coul have opposite signs. [ a Now that we know et([t ) gives the area of the image of the unit square if [T =, it s not too har to see this is true for any linear map. We ll first nee a technical fact. Eercise: Prove et(ab) = et(a) et(b) for 2 2 matrices A an B. (Really, just multiply it out.) Notice that this means et(ab) = et(ba) for any pair of 2 2 matrices. Eercise: Show that for any angle θ we have ([ ) cos θ sin θ et([r θ ) = et =. sin θ cos θ Now let T : R 2 R 2 e a linear mapping of the plane to itself, an suppose [ a [T =. c [ [ [ [ a This means T (e ) = an T (e c 2 ) =, where e = an e 2 = as efore. [ a Now, the vector T (e ) = makes some angle θ with the positive ais, so we apply the c rotation R θ to T to get a new mapping [ [ [ T = R θ T, [ T cos θ sin θ a ã = [R θ [T = =, sin θ cos θ c 2
3 an et([ T ) = et([r θ [T ) = et([r θ ) et([t ) = et([t ). By the computation we i aove, Area( P ) = et([ T ). We also have that T sens the unit square S to a parallelogram P, an T sens S to a parallelogram P. These two parallelograms P an P iffer y a rotation, so they have the same area. Thus we see Area(P ) = Area( P ) = et([ T ) = et([t ). In particular, we have just proven that et([t ) precisely when T is invertile, ecause this is precisely when the image parallelogram P has nonzero area. Orientation an the sign of the eterminant: As we saw in the previous notes, there are actually two linear transformations which map the unit square S onto this parallelogram P, we can also have ([ ) [ T = In this case we see that ([, T ) [ a = et([t ) = a = Area(P ). [ a, [T = Why o we have the minus sign? To unerstan what s going on, it will help to lael the corners of the unit square S an the parallelogram P as in the picture elow.. iv i iii ii ii iii i iv What oes this laeling mean? The[ mapping T sens the vector e, which goes from i to ii in the square on the left to the vector. which also goes from i to ii in the parallelogram on the right. Similarly, the [ mapping T sens the vector e 2, which goes from i to iv in the square on a the left to the vector. which also goes from i to iv in the parallelogram on the right. Now, if we follow the laeling of the corners of the square in orer, as in i to ii to iii to iv, then we traverse along the ounary of the square counter-clockwise. However, if we follow the laeling of th ecorners of the parallelogram in orer, as in i to ii to iii to iv, we traverse along the ounary of the parallelogram clockwise. This means the mapping T reverse the irection we traverse along the ounary of the shape. In other wors, T reverse the orientation. We have iscovere the following general principle: et([t ) < T reverses orientation. This principle is eactly why we wrote et([t ) = Area(P ) efore. In general, if T : R 2 R 2 preserves orientation then et([t ) = Area(P ), ut if T reverses orientation then et([t ) = Area(P ). Higher imensions: So far we ve seen that the eterminant of a 2 2 matri is the area (up to a sign) of the parallelogram which is the image of the unit square. In fact, a similar thing 3
4 is true in higher imensions. Let [T e an n n matri, which we ve seen correspons to a linear map T : R n R n. Then T sens the unit cue S = { i : i =, 2,..., n} to a parallelpipe P, which is spanne y the columns of [T. Then et([t ) = Vol(P ), where Vol gives the n-imensional volume. We egin with a quick illustrative eample. Consier [T = a c e Then the image of the unit cue S uner T is where [ [ T a = c By slicing P with horizontal slices, we see, e >. P = {(, y, z) : (, y) P, z e},, S = {, y }, P = T ( S). Vol(P ) = e Area( P ) = e et([ T ). So, y any reasonale efinition of the eterminant for 3 3 matrices which fits with our efinition for 2 2 matrices, we must have et([t ) = e et([ T ) = e(a c). Eercise: Let [T e a 3 3 matri. Show that you can always perform a rotation to make the last colum of [T into. (Hint: what are the columns of [T?) e At this point, we can write own a reasonale formula for the eterminant of a 3 3 matri. Let [T = a e c f, g h i then ([ e et[t = c et g h ) ([ a f et g h ) ([ a + i et e Here we ve single out the last column, ut we can o the same thing y picking out any row or column. To o this properly, we nee some notation. Let [T = [A ij, so that the entry of [T in the ith row, jth column is A ij. Also, let [ T ij e the 2 2 matri you get from [T y crossing out the ith row an jth column. Then for any choice of j =, 2, 3 we can write ). et([t ) = ( ) +j A j et([ T j ) + ( ) 2+j A 2j et([ T 2j ) + ( ) 3+j A 3j et([ T 3j ), which computes et([t ) y eaning along the jth column. i =, 2, 3 we can write Alternatively, for any choice of et([t ) = ( ) i+ A i et([ T i ) + ( ) i+2 A i2 et([ T i2 ) + ( ) i+3 A i3 et([ T i3 ), which computes et([t ) y epaning along the ith row. The same iea will compute the eterminant of any square matri inuctively. That is, you write the eterminant of an n n matri as a sum of eterminants of (n ) (n ) matrices. We write the general formula as follows. Again, we let A ij e the entry of [T in the ith row, jth 4
5 column, an we let [ T ij e the (n ) (n ) matri you get from [T y crossing out the ith row an the jth column. The for any choice of j =, 2,..., n we compute et([t ) y epaning along the jth column using the formula et([t ) = ( ) +j A j et([ T j ) + ( ) 2+j A 2j et([ T 2j ) + + ( ) n+j A nj et([ T nj ). Alternatively, for any choice of i =, 2,..., n we compute et([t ) y epaning along the ith row using the formula et([t ) = ( ) i+ A i et([ T i ) + ( ) i+2 A i2 et([ T i2 ) + + ( ) i+n A in et([ T in ). We summarize some important properties of the eterminant here.. The eterminant is linear in each row an column. That is, if A is an n n matri an à is the same as A ecept that you multiply the ith row y c, then et(ã) = c et(a). Also, A an A 2 are the same ecept at the ith row an A is what you get y aing together the ith row of A an A 2 then et(a) = et(a ) + et(a 2 ). The same goes for columns. 2. Consequently, if A is an n n matri an c is a numer then et(ca) = c n et(a). 3. An n n matri A is invertile if an only if et(a). 4. In fact, et(a) is the n-imensional volume of the parallelpipe P which is the image of the unit cue S = {,..., n } uner the linear transformation associate to A. (You can prove this y inuction, in a very similar way we got the geometric interpretation for three imensions from the two-imensional version.) 5. Let A an B e n n matrices, then et(ab) = et(a) et(b). 6. Let A e an n n matri an let à e the matri you get y swapping ajacent two rows of A (or y swapping two ajacent columns). Then et(ã) = et(a) Trace: Another important numer associate to an n n matri is its trace. We let [T e an n n matri with A ij eing the entry in the ith row, jth column. Then the trace of [T is given y tr([t ) = A + A A nn, the sum of the entries of [T on the iagonal running from the top left of [T to its ottom right. Later on, we ll see that uner some conitions (for instance, if A ij = A ji ) that the trace measures an average istortion of T as a mapping. That is, if the trace is close to n then T oesn t istort istances too much, ut if the traces is very ifferent from n then it istorts istances a lot. Rememer that this guiline only hols if T is symmetric, that is if A ij = A ji. The trace satisfies the following properties:. If I is the n n ientity matri then tr(i) = n. 2. If A an B are square matrices an c is a numer then tr(a + B) = tr(a) + tr(b), tr(ca) = c tr(a), tr(ab) = tr(ba). Some special matrices: We close with some special types of square matrices. Let [T e a square matri, with entries A ij in the ith row, jth colum as aove. We say [T is iagonal if A ij = for i j. We say [T is upper triangular if A ij = for i > j an that [T is lower triangular if A ij = for i < j. Eercise: Why is a iagonal matri calle iagonal? How aout upper (or lower) triangular matrices? Eercise: Let [T e iagonal, an show that et([t ) = A A 22 A nn, tr([t ) = A + A A nn Eercise: Show that the same formula hols for a upper triangular an lower triangular matrices. 5
Rank, Trace, Determinant, Transpose an Inverse of a Matrix Let A be an n n square matrix: A = a11 a1 a1n a1 a an a n1 a n a nn nn where is the jth col
Review of Linear Algebra { E18 Hanout Vectors an Their Inner Proucts Let X an Y be two vectors: an Their inner prouct is ene as X =[x1; ;x n ] T Y =[y1; ;y n ] T (X; Y ) = X T Y = x k y k k=1 where T an
More informationIntegration by Parts
Integration by Parts 6-3-207 If u an v are functions of, the Prouct Rule says that (uv) = uv +vu Integrate both sies: (uv) = uv = uv + u v + uv = uv vu, vu v u, I ve written u an v as shorthan for u an
More informationThe numbers inside a matrix are called the elements or entries of the matrix.
Chapter Review of Matries. Definitions A matrix is a retangular array of numers of the form a a a 3 a n a a a 3 a n a 3 a 3 a 33 a 3n..... a m a m a m3 a mn We usually use apital letters (for example,
More informationVectors in two dimensions
Vectors in two imensions Until now, we have been working in one imension only The main reason for this is to become familiar with the main physical ieas like Newton s secon law, without the aitional complication
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 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 informationIntegration Review. May 11, 2013
Integration Review May 11, 2013 Goals: Review the funamental theorem of calculus. Review u-substitution. Review integration by parts. Do lots of integration eamples. 1 Funamental Theorem of Calculus In
More informationDiagonalization of Matrices Dr. E. Jacobs
Diagonalization of Matrices Dr. E. Jacobs One of the very interesting lessons in this course is how certain algebraic techniques can be use to solve ifferential equations. The purpose of these notes is
More information5.4 Fundamental Theorem of Calculus Calculus. Do you remember the Fundamental Theorem of Algebra? Just thought I'd ask
5.4 FUNDAMENTAL THEOREM OF CALCULUS Do you remember the Funamental Theorem of Algebra? Just thought I' ask The Funamental Theorem of Calculus has two parts. These two parts tie together the concept of
More informationEuler equations for multiple integrals
Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................
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 informationTutorial 1 Differentiation
Tutorial 1 Differentiation What is Calculus? Calculus 微積分 Differential calculus Differentiation 微分 y lim 0 f f The relation of very small changes of ifferent quantities f f y y Integral calculus Integration
More informationProblem Sheet 2: Eigenvalues and eigenvectors and their use in solving linear ODEs
Problem Sheet 2: Eigenvalues an eigenvectors an their use in solving linear ODEs If you fin any typos/errors in this problem sheet please email jk28@icacuk The material in this problem sheet is not examinable
More informationPure Further Mathematics 1. Revision Notes
Pure Further Mathematics Revision Notes June 20 2 FP JUNE 20 SDB Further Pure Complex Numbers... 3 Definitions an arithmetical operations... 3 Complex conjugate... 3 Properties... 3 Complex number plane,
More informationLemma 8: Suppose the N by N matrix A has the following block upper triangular form:
17 4 Determinants and the Inverse of a Square Matrix In this section, we are going to use our knowledge of determinants and their properties to derive an explicit formula for the inverse of a square matrix
More informationCalculus in the AP Physics C Course The Derivative
Limits an Derivatives Calculus in the AP Physics C Course The Derivative In physics, the ieas of the rate change of a quantity (along with the slope of a tangent line) an the area uner a curve are essential.
More informationG4003 Advanced Mechanics 1. We already saw that if q is a cyclic variable, the associated conjugate momentum is conserved, L = const.
G4003 Avance Mechanics 1 The Noether theorem We alreay saw that if q is a cyclic variable, the associate conjugate momentum is conserve, q = 0 p q = const. (1) This is the simplest incarnation of Noether
More informationDerivative of a Constant Multiple of a Function Theorem: If f is a differentiable function and if c is a constant, then
Bob Brown Math 51 Calculus 1 Chapter 3, Section Complete 1 Review of the Limit Definition of the Derivative Write the it efinition of the erivative function: f () Derivative of a Constant Multiple of a
More informationExamples True or false: 3. Let A be a 3 3 matrix. Then there is a pattern in A with precisely 4 inversions.
The exam will cover Sections 6.-6.2 and 7.-7.4: True/False 30% Definitions 0% Computational 60% Skip Minors and Laplace Expansion in Section 6.2 and p. 304 (trajectories and phase portraits) in Section
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 informationd dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1
Lecture 5 Some ifferentiation rules Trigonometric functions (Relevant section from Stewart, Seventh Eition: Section 3.3) You all know that sin = cos cos = sin. () But have you ever seen a erivation of
More informationAnswers in blue. If you have questions or spot an error, let me know. 1. Find all matrices that commute with A =. 4 3
Answers in blue. If you have questions or spot an error, let me know. 3 4. Find all matrices that commute with A =. 4 3 a b If we set B = and set AB = BA, we see that 3a + 4b = 3a 4c, 4a + 3b = 3b 4d,
More informationExam 2 Review Solutions
Exam Review Solutions 1. True or False, an explain: (a) There exists a function f with continuous secon partial erivatives such that f x (x, y) = x + y f y = x y False. If the function has continuous secon
More informationLinear transformations
Linear Algebra with Computer Science Application February 5, 208 Review. Review: linear combinations Given vectors v, v 2,..., v p in R n and scalars c, c 2,..., c p, the vector w defined by w = c v +
More informationCalculus of Variations
Calculus of Variations Lagrangian formalism is the main tool of theoretical classical mechanics. Calculus of Variations is a part of Mathematics which Lagrangian formalism is base on. In this section,
More informationFree rotation of a rigid body 1 D. E. Soper 2 University of Oregon Physics 611, Theoretical Mechanics 5 November 2012
Free rotation of a rigi boy 1 D. E. Soper 2 University of Oregon Physics 611, Theoretical Mechanics 5 November 2012 1 Introuction In this section, we escribe the motion of a rigi boy that is free to rotate
More informationThe Exact Form and General Integrating Factors
7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily
More informationu!i = a T u = 0. Then S satisfies
Deterministic Conitions for Subspace Ientifiability from Incomplete Sampling Daniel L Pimentel-Alarcón, Nigel Boston, Robert D Nowak University of Wisconsin-Maison Abstract Consier an r-imensional subspace
More informationApplications of the Wronskian to ordinary linear differential equations
Physics 116C Fall 2011 Applications of the Wronskian to orinary linear ifferential equations Consier a of n continuous functions y i (x) [i = 1,2,3,...,n], each of which is ifferentiable at least n times.
More informationYear 11 Matrices Semester 2. Yuk
Year 11 Matrices Semester 2 Chapter 5A input/output Yuk 1 Chapter 5B Gaussian Elimination an Systems of Linear Equations This is an extension of solving simultaneous equations. What oes a System of Linear
More informationThe derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)
Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)
More informationAPPROXIMATE SOLUTION FOR TRANSIENT HEAT TRANSFER IN STATIC TURBULENT HE II. B. Baudouy. CEA/Saclay, DSM/DAPNIA/STCM Gif-sur-Yvette Cedex, France
APPROXIMAE SOLUION FOR RANSIEN HEA RANSFER IN SAIC URBULEN HE II B. Bauouy CEA/Saclay, DSM/DAPNIA/SCM 91191 Gif-sur-Yvette Ceex, France ABSRAC Analytical solution in one imension of the heat iffusion equation
More 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 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 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 informationQuantum Algorithms: Problem Set 1
Quantum Algorithms: Problem Set 1 1. The Bell basis is + = 1 p ( 00i + 11i) = 1 p ( 00i 11i) + = 1 p ( 01i + 10i) = 1 p ( 01i 10i). This is an orthonormal basis for the state space of two qubits. It is
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 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 informationector ition 1. Scalar: physical quantity having only magnitue but no irection is calle a scalar. eg: Time, mass, istance, spee, electric charge, etc.. ector: physical quantity having both magnitue an irection
More informationTrigonometric Functions
72 Chapter 4 Trigonometric Functions 4 Trigonometric Functions To efine the raian measurement system, we consier the unit circle in the y-plane: (cos,) A y (,0) B So far we have use only algebraic functions
More informationTransformations. Chapter D Transformations Translation
Chapter 4 Transformations Transformations between arbitrary vector spaces, especially linear transformations, are usually studied in a linear algebra class. Here, we focus our attention to transformation
More informationIntroduction to Mechanics Work and Energy
Introuction to Mechanics Work an Energy Lana Sherian De Anza College Mar 15, 2018 Last time non-uniform circular motion an tangential acceleration energy an work Overview energy work a more general efinition
More informationSolutions to Practice Problems Tuesday, October 28, 2008
Solutions to Practice Problems Tuesay, October 28, 2008 1. The graph of the function f is shown below. Figure 1: The graph of f(x) What is x 1 + f(x)? What is x 1 f(x)? An oes x 1 f(x) exist? If so, what
More informationEC5555 Economics Masters Refresher Course in Mathematics September 2013
EC5555 Economics Masters Reresher Course in Mathematics September 3 Lecture 5 Unconstraine Optimization an Quaratic Forms Francesco Feri We consier the unconstraine optimization or the case o unctions
More information1300 Linear Algebra and Vector Geometry
1300 Linear Algebra and Vector Geometry R. Craigen Office: MH 523 Email: craigenr@umanitoba.ca May-June 2017 Matrix Inversion Algorithm One payoff from this theorem: It gives us a way to invert matrices.
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 informationNOTES FOR SECOND YEAR LINEAR ALGEBRA
NOTES FOR SECOND YEAR LINEAR ALGEBRA JESSE RATZKIN Introduction and Background We begin with some motivational remarks and then outline a list (not necessarily complete!) of things you should already know
More information6. Friction and viscosity in gasses
IR2 6. Friction an viscosity in gasses 6.1 Introuction Similar to fluis, also for laminar flowing gases Newtons s friction law hols true (see experiment IR1). Using Newton s law the viscosity of air uner
More information1 Last time: determinants
1 Last time: determinants Let n be a positive integer If A is an n n matrix, then its determinant is the number det A = Π(X, A)( 1) inv(x) X S n where S n is the set of n n permutation matrices Π(X, A)
More informationVectors. Slide 2 / 36. Slide 1 / 36. Slide 3 / 36. Slide 4 / 36. Slide 5 / 36. Slide 6 / 36. Scalar versus Vector. Determining magnitude and direction
Slide 1 / 3 Slide 2 / 3 Scalar versus Vector Vectors scalar has only a physical quantity such as mass, speed, and time. vector has both a magnitude and a direction associated with it, such as velocity
More informationDifferentiation ( , 9.5)
Chapter 2 Differentiation (8.1 8.3, 9.5) 2.1 Rate of Change (8.2.1 5) Recall that the equation of a straight line can be written as y = mx + c, where m is the slope or graient of the line, an c is the
More informationAnswers to Coursebook questions Chapter 5.6
Answers to Courseook questions Chapter 56 Questions marke with a star (*) use the formula for the magnetic fiel create y a current μi ( = ) which is not on the syllaus an so is not eaminale See Figure
More information6 General properties of an autonomous system of two first order ODE
6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x
More informationGAUSSIAN ELIMINATION AND LU DECOMPOSITION (SUPPLEMENT FOR MA511)
GAUSSIAN ELIMINATION AND LU DECOMPOSITION (SUPPLEMENT FOR MA511) D. ARAPURA Gaussian elimination is the go to method for all basic linear classes including this one. We go summarize the main ideas. 1.
More informationSECTION 3.2 THE PRODUCT AND QUOTIENT RULES 1 8 3
SECTION 3.2 THE PRODUCT AND QUOTIENT RULES 8 3 L P f Q L segments L an L 2 to be tangent to the parabola at the transition points P an Q. (See the figure.) To simplify the equations you ecie to place the
More informationAcute sets in Euclidean spaces
Acute sets in Eucliean spaces Viktor Harangi April, 011 Abstract A finite set H in R is calle an acute set if any angle etermine by three points of H is acute. We examine the maximal carinality α() of
More informationMatrix multiplications that do row operations
May 6, 204 Matrix multiplications that do row operations page Matrix multiplications that do row operations Introduction We have yet to justify our method for finding inverse matrices using row operations:
More informationSample Solutions from the Student Solution Manual
1 Sample Solutions from the Student Solution Manual 1213 If all the entries are, then the matrix is certainly not invertile; if you multiply the matrix y anything, you get the matrix, not the identity
More information3.3.1 Linear functions yet again and dot product In 2D, a homogenous linear scalar function takes the general form:
3.3 Gradient Vector and Jacobian Matri 3 3.3 Gradient Vector and Jacobian Matri Overview: Differentiable functions have a local linear approimation. Near a given point, local changes are determined by
More informationSolution Set 7, Fall '12
Solution Set 7, 18.06 Fall '12 1. Do Problem 26 from 5.1. (It might take a while but when you see it, it's easy) Solution. Let n 3, and let A be an n n matrix whose i, j entry is i + j. To show that det
More informationAP Physics C - Mechanics
Slide 1 / 36 Slide 2 / 36 P Physics - Mechanics Vectors 2015-12-03 www.njctl.org Scalar Versus Vector Slide 3 / 36 scalar has only a physical quantity such as mass, speed, and time. vector has both a magnitude
More informationMatrices and Vectors
Matrices and Vectors James K. Peterson Department of Biological Sciences and Department of Mathematical Sciences Clemson University November 11, 2013 Outline 1 Matrices and Vectors 2 Vector Details 3 Matrix
More information58. The Triangle Inequality for vectors is. dot product.] 59. The Parallelogram Law states that
786 CAPTER 12 VECTORS AND TE GEOETRY OF SPACE 0, 0, 1, and 1, 1, 1 as shown in the figure. Then the centroid is. ( 1 2, 1 2, 1 2 ) ] x z C 54. If c a a, where a,, and c are all nonzero vectors, show that
More informationComputer Graphics: 2D Transformations. Course Website:
Computer Graphics: D Transformations Course Website: http://www.comp.dit.ie/bmacnamee 5 Contents Wh transformations Transformations Translation Scaling Rotation Homogeneous coordinates Matri multiplications
More informationTOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH
English NUMERICAL MATHEMATICS Vol14, No1 Series A Journal of Chinese Universities Feb 2005 TOEPLITZ AND POSITIVE SEMIDEFINITE COMPLETION PROBLEM FOR CYCLE GRAPH He Ming( Λ) Michael K Ng(Ξ ) Abstract We
More informationThe Non-abelian Hodge Correspondence for Non-Compact Curves
1 Section 1 Setup The Non-abelian Hoge Corresponence for Non-Compact Curves Chris Elliott May 8, 2011 1 Setup In this talk I will escribe the non-abelian Hoge theory of a non-compact curve. This was worke
More informationx y = 1, 2x y + z = 2, and 3w + x + y + 2z = 0
Section. Systems of Linear Equations The equations x + 3 y =, x y + z =, and 3w + x + y + z = 0 have a common feature: each describes a geometric shape that is linear. Upon rewriting the first equation
More informationx f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.
Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?
More informationOPG S. LIST OF FORMULAE [ For Class XII ] OP GUPTA. Electronics & Communications Engineering. Indira Award Winner
OPG S MAHEMAICS LIS OF FORMULAE [ For Class XII ] Covering all the topics of NCER Mathematics et Book Part I For the session 0-4 By OP GUPA Electronics & Communications Engineering Inira Awar Winner Visit
More informationLinear Equations in Linear Algebra
1 Linear Equations in Linear Algebra 1.1 SYSTEMS OF LINEAR EQUATIONS LINEAR EQUATION,, 1 n A linear equation in the variables equation that can be written in the form a a a b 1 1 2 2 n n a a is an where
More informationCenter of Gravity and Center of Mass
Center of Gravity an Center of Mass 1 Introuction. Center of mass an center of gravity closely parallel each other: they both work the same way. Center of mass is the more important, but center of gravity
More informationTHE INFLATION-RESTRICTION SEQUENCE : AN INTRODUCTION TO SPECTRAL SEQUENCES
THE INFLATION-RESTRICTION SEQUENCE : AN INTRODUCTION TO SPECTRAL SEQUENCES TOM WESTON. Example We egin with aelian groups for every p, q and maps : + (here, as in all of homological algera, all maps are
More informationLecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012
CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration
More information45. The Parallelogram Law states that. product of a and b is the vector a b a 2 b 3 a 3 b 2, a 3 b 1 a 1 b 3, a 1 b 2 a 2 b 1. a c. a 1. b 1.
SECTION 10.4 THE CROSS PRODUCT 537 42. Suppose that all sides of a quadrilateral are equal in length and opposite sides are parallel. Use vector methods to show that the diagonals are perpendicular. 43.
More informationI = i 0,
Special Types of Matrices Certain matrices, such as the identity matrix 0 0 0 0 0 0 I = 0 0 0, 0 0 0 have a special shape, which endows the matrix with helpful properties The identity matrix is an example
More information2D Geometric Transformations. (Chapter 5 in FVD)
2D Geometric Transformations (Chapter 5 in FVD) 2D geometric transformation Translation Scaling Rotation Shear Matri notation Compositions Homogeneous coordinates 2 2D Geometric Transformations Question:
More informationA Note on Exact Solutions to Linear Differential Equations by the Matrix Exponential
Avances in Applie Mathematics an Mechanics Av. Appl. Math. Mech. Vol. 1 No. 4 pp. 573-580 DOI: 10.4208/aamm.09-m0946 August 2009 A Note on Exact Solutions to Linear Differential Equations by the Matrix
More information4. Important theorems in quantum mechanics
TFY4215 Kjemisk fysikk og kvantemekanikk - Tillegg 4 1 TILLEGG 4 4. Important theorems in quantum mechanics Before attacking three-imensional potentials in the next chapter, we shall in chapter 4 of this
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 informationAdditional Exercises for Chapter 10
Aitional Eercises for Chapter 0 About the Eponential an Logarithm Functions 6. Compute the area uner the graphs of i. f() =e over the interval [ 3, ]. ii. f() =e over the interval [, 4]. iii. f() = over
More informationVectors and matrices: matrices (Version 2) This is a very brief summary of my lecture notes.
Vectors and matrices: matrices (Version 2) This is a very brief summary of my lecture notes Matrices and linear equations A matrix is an m-by-n array of numbers A = a 11 a 12 a 13 a 1n a 21 a 22 a 23 a
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 informationDot Products, Transposes, and Orthogonal Projections
Dot Products, Transposes, and Orthogonal Projections David Jekel November 13, 2015 Properties of Dot Products Recall that the dot product or standard inner product on R n is given by x y = x 1 y 1 + +
More informationA Second Time Dimension, Hidden in Plain Sight
A Secon Time Dimension, Hien in Plain Sight Brett A Collins. In this paper I postulate the existence of a secon time imension, making five imensions, three space imensions an two time imensions. I will
More information. Using a multinomial model gives us the following equation for P d. , with respect to same length term sequences.
S 63 Lecture 8 2/2/26 Lecturer Lillian Lee Scribes Peter Babinski, Davi Lin Basic Language Moeling Approach I. Special ase of LM-base Approach a. Recap of Formulas an Terms b. Fixing θ? c. About that Multinomial
More informationIntroduction to Matrix Algebra
Introduction to Matrix Algebra August 18, 2010 1 Vectors 1.1 Notations A p-dimensional vector is p numbers put together. Written as x 1 x =. x p. When p = 1, this represents a point in the line. When p
More informationDerivatives of Trigonometric Functions
Derivatives of Trigonometric Functions 9-8-28 In this section, I ll iscuss its an erivatives of trig functions. I ll look at an important it rule first, because I ll use it in computing the erivative of
More informationf(x + h) f(x) f (x) = lim
Introuction 4.3 Some Very Basic Differentiation Formulas If a ifferentiable function f is quite simple, ten it is possible to fin f by using te efinition of erivative irectly: f () 0 f( + ) f() However,
More informationDesigning Information Devices and Systems II Fall 2017 Note Theorem: Existence and Uniqueness of Solutions to Differential Equations
EECS 6B Designing Information Devices an Systems II Fall 07 Note 3 Secon Orer Differential Equations Secon orer ifferential equations appear everywhere in the real worl. In this note, we will walk through
More informationLecture 12. Energy, Force, and Work in Electro- and Magneto-Quasistatics
Lecture 1 Energy, Force, an ork in Electro an MagnetoQuasistatics n this lecture you will learn: Relationship between energy, force, an work in electroquasistatic an magnetoquasistatic systems ECE 303
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 informationMath 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v
Math Fall 06 Section Monay, September 9, 06 First, some important points from the last class: Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v passing through
More information3.7 Implicit Differentiation -- A Brief Introduction -- Student Notes
Fin these erivatives of these functions: y.7 Implicit Differentiation -- A Brief Introuction -- Stuent Notes tan y sin tan = sin y e = e = Write the inverses of these functions: y tan y sin How woul we
More informationDesigning Information Devices and Systems II Spring 2018 J. Roychowdhury and M. Maharbiz Discussion 8A
EECS 6B Designing Information Devices an Systems II Spring 28 J Roychowhury an M Maharbiz Discussion 8A Change of Basis Review Figure : Left: basis vectors x an y Right: basis vectors u an v T We can think
More information18 EVEN MORE CALCULUS
8 EVEN MORE CALCULUS Chapter 8 Even More Calculus Objectives After stuing this chapter you shoul be able to ifferentiate an integrate basic trigonometric functions; unerstan how to calculate rates of change;
More informationWe could express the left side as a sum of vectors and obtain the Vector Form of a Linear System: a 12 a x n. a m2
Week 22 Equations, Matrices and Transformations Coefficient Matrix and Vector Forms of a Linear System Suppose we have a system of m linear equations in n unknowns a 11 x 1 + a 12 x 2 + + a 1n x n b 1
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 information3.2 Differentiability
Section 3 Differentiability 09 3 Differentiability What you will learn about How f (a) Might Fail to Eist Differentiability Implies Local Linearity Numerical Derivatives on a Calculator Differentiability
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 informationIn the usual geometric derivation of Bragg s Law one assumes that crystalline
Diffraction Principles In the usual geometric erivation of ragg s Law one assumes that crystalline arrays of atoms iffract X-rays just as the regularly etche lines of a grating iffract light. While this
More information