Math 201 Lecture 09: Undetermined Coefficient Cont.

Size: px
Start display at page:

Download "Math 201 Lecture 09: Undetermined Coefficient Cont."

Transcription

1 +B Math 201 Lecture 09: Undetermined Coefficient Cont. Jan. 27, 2012 Many examples here are taken from the textbook. The first number in () refers to the problem number in the UA Custom edition, the second number in () refers to the problem number in the 8th edition. To solve 0. Review ay +by +cy=f(t), (1) 1. Solve the homogeneous problem ay +by +cy=0 (2) to get y 1,y 2. Keep record of the roots r 1,2 of the characteristic equation. 2. Guess what y p should look like according to the following rules: If f(t)=ct m e rt, then If f(t)=ct m e αt cosβt or Ct m e αt sinβt, then 1 t 0 )e αt cosβt+t s (B m t m + 1 t 0 )e rt (3) 0 )e αt sinβt. (4) with s=the number of times the pair (α±βi) appears in the list of roots r 1,r The general solution is then given by 4. If initial conditions are given, use them to determine C 1,C 2. Quiz. Solve Solution. First solve the homogeneous equation Next observe 2e t =2t 0 e 1 t, guess y=c 1 y 1 +C 2 y 2 +y p. (5) y y=2e t. (6) y y=0 r 2 1=0 r 1,2 =1, 1;y 1,y 2 =e t,e t. (7) y p =t s Ae t. (8) To determine s, check how many times 1 appears in r 1,r 2 : We have s=1. Therefore our guess is Now substitute this y p into the equation to find A: Therefore So y p =te t. Putting everything together, we have y=ate t. (9) y p =Ate t +2Ae t y p y p =2Ae t. (10) 2Ae t =2e t A=1. (11) y=c 1 e t +C 2 e t +te t. (12) 1

2 +B 2 Math 201 Lecture 09: Undetermined Coefficient Cont. The Equation with more general f(t): 1. Basic Information ay +by +cy=f(t) (13) f(t)=p m (t)e rt or f(t)=p m (t)e αt cosβt+q n (t)e αt sinβt (14) where P m (t) stands for a polynomial of degree m, and Q n stands for a polynomial with degree n. How to get general solution Recall: General solution to reads ay +by +cy=f(t) (15) y=c 1 y 1 +C 2 y 2 +y p (16) where C 1 y 1 +C 2 y 2 is general solution to the homogeneous equation and y p is any one solution to ay +by +cy=0. (17) ay +by +cy=f(t). (18) Compare with the situation in the last lecture, we see that y 1,y 2 stays the same, all we need to do is to figure out y p in this more general case. Key: Linearity. (See Notes & Comments for more explanation). Procedure: If f(t)=cp m (t)e rt, then If f(t)=p m (t)e αt cosβt+q n (t)e αt sinβt, then y p =t s (A m t k + 1 t 0 )e αt cosβt+t s (B m t k + 1 t 0 )e rt (19) 0 )e αt sinβt. (20) with s=the number of times the pair (α± βi) appears in the list of roots r 1,r 2, and k=max{m,n} that is the bigger number of m,n. Example: (4.5 18; ) Solve Solution. First solve the homogeneous equation: y 2y 3y=3t 2 5. (21) y 2y 3y=0 r 2 2r 3=0 r 1,2 =3, 1 (22) so the general solution to the homogeneous equation is y=c 1 e 3t +C 2 e t. (23) Now notice the right hand side is of the form P m (t)e rt with m=2, r=0. So guess y p =t s (A 2 t 2 1 t 0 )e 0t. (24) To determine s, check how many times r=0 appears in the list of roots: r 1,2 =3, 1. 0 times. So s=0. Substitute y p =A 2 t 2 1 t 0 into the equation we reach 2A 2 2(2A 2 t 1 ) 3(A 2 t 2 1 t 0 )=3t 2 5 (25)

3 +B Jan. 27, which simplifies to 3A 2 t 2 +( 4A 2 3A 1 )t+(2a 2 2A 1 3A 0 )=3t 2 5 (26) 3A 2 = 3; (27) 4A 2 3A 1 = 0 (28) 2A 2 2A 1 3A 0 = 5. (29) Solving it we have So Check solution: A 2 = 1;A 1 =4/3;A 0 =1/9. (30) y p = t t (31) e 3t,e t solves the homogeneous problem; y p solves the original problem. So the final answer is y=c 1 e 3t +C 2 e t t t (32) How to solve initial value problem (IVP) Nothing new here. Solve y 2y 3y=3t 2 5, y(0)=0,y (0)=0. (33) Solution. We have already found the general solution To apply initial conditions, prepare: y=c 1 e 3t +C 2 e t t t (34) Now y =3C 1 e 3t C 2 e t 2t (35) y(0)=0 C 1 +C =0 (36) 9 y (0)=0 3C 1 C =0. (37) 3 Solving it (Add two equation to get C 1, then get C 2 using either one equation) we get So the solution to the initial value problem is C 1 = ; C 2= 1 4. (38) How to check solutions y= e3t e t t t (39) Nothing new here. 2. Things to be Careful/Tricky Issues See Common Mistakes for examples. Keep in mind that in the 2nd case, y p =t s (A m t k + 1 t 0 )e αt cosβt+t s (B m t k + 0 )e αt sinβt. (40)

4 4 Math 201 Lecture 09: Undetermined Coefficient Cont. It s t k in both terms. When solving initial value problems, initial conditions should only be used when the general solution is found, that is when y 1, y 2, y p are all figured out. Using initial condition on C 1 y 1 + C 2 y 2 before finding y p is not correct, as adding y p will change the values of y(0),y (0). When the calculation is complicated, it is easy to forget the t s term when writing the final answer. 3. More Examples Sometimes the right hand side is not of the form P m (t)e rt or P m (t)e αt cosβt+q n (t)e αt sinβt, but a sum of terms of these forms. In this case we have to break y p into y p1, y p2, and find each one separately. Example 1. (4.5 28; ) Solve y +y 12y=e t +e 2t 1; y(0)=1,y (0)=3. (41) Solution. First solve the homogeneous equation: y +y 12y=0 r 2 +r 12 r 1,2 = 4,3 C 1 e 4t +C 2 e 3t. (42) Now to find y p, we have to break it up to y p =y p1 +y p2 +y p3 with the latter solving and It is easy to find So The general solution is y p1 +y p1 12y p1 =e t (43) y p2 +y p2 12y p2 =e 2t (44) y p3 +y p3 12y p3 = 1. (45) y p1 = 1 10 et ; y p2 = 1 6 e2t ; y p3 = (46) y p = 1 10 et 1 6 e2t (47) y=c 1 e 4t +C 2 e 3t 1 10 et 1 6 e2t (48) To apply initial conditions, prepare: y = 4C 1 e 4t +3C 2 e 3t 1 10 et 1 3 e2t. (49) Now use initial conditions: y(0)=1 C 1 +C =1; (50) 12 The solutions are The final answer is then y (0)=3 4C 1 +3C =3. (51) 3 C 1 = 1 60,C 2= 7 6. (52) y= 1 60 e 4t e3t 1 10 et 1 6 e2t (53) The method also applies to higher order equations. Example 2. Find a particular solution for y (4) +5y +4y= 10 cost 20 sint. (54)

5 This simplifies to 1 6Asint+6B cost=10 cost 20 sint. (63) Jan. 27, Solution. First solve the homogeneous equation (or more precisely, find the roots to the characteristic equation): y (4) +5y +4y=0 r 4 +5r 2 +4=0 (r 2 +1)(r 2 +4)=0 r 1,2,3,4 =±i,±2i. (55) Note that it s a good habit to organize complex roots in pairs. Now the right hand side is of the form f(t)=p m (t)e αt cosβt+ Q n (t)e αt sinβt with m=n=0, α=0,β=1. So guess y p =t s (A cost+b sint). (56) To determine s, take α ±iβ =±i, and check how many times this pair appears in the list of roots r 1,2,3,4 =±i,±2i. Once. So s=1 and Now substitute this guess into the equation: Compute So the equation becomes y p =t(a cost+b sint). (57) y p =Acost+B sint Atsint+Btcost; (58) y p = 2Asint+2B cost Atcost Btsint; (59) y p = 3Acost 3B sinttsint Btcost; (60) y p (4) =4Asint 4B costtcost+btsint. (61) [4 A sin t 4 B cos t + A t cos t + B t sin t] + 5 [ 2 A sin t + 2 B cos t A t cos t B t sin t] + 4t(A cost+b sint)=10 cost 20 sint. (62) So We have A= 10 3, B= 5 3. (64) ( 10 y p =t 3 cost+ 5 ) 3 sint. (65) If time allows, substitute it back into the equation to check. How are the formulas derived. Start from If f(t)=ct m e rt, then 4. Notes and Comments we will try to derive If f(t)=cp m (t)e rt, then 1 t 0 )e rt (66) 1 t 0 )e rt (67) 1. If at this stage you find that the t cost and t sint terms do not totally cancel out, go back and check your calculation. When s 0, it is very easy to mess up.

6 +y +y 6 Math 201 Lecture 09: Undetermined Coefficient Cont. using linearity. The other case can be dealt with similarly so left as exercise. 2 Note that the value of s is determined by the roots of the characteristic equation together with the value of r. So should stay the same for this more general case. Let s first look at an example. Say f(t)=(t+1)e rt. We need to find y p solving By linearity we know that if we find y p1 solving and y p2 solving then y p is simply y p1 +y p2. For y p1, y p2 we know that it looks like 3 ay +by +cy=(t+1)e rt =te rt +e rt. (68) ay +by +cy=te rt (69) ay +by +cy=e rt (70) y p1 =t s (A 1 t 0 )e rt, y p2 =t s (B 0 )e rt (71) We can simply substitute them into the two equations and find out A 1, A 0, B 0. However there is a more efficient way: Observe y p =y p1 +y p2 =t s (A 1 t+(a 0 +B 0 ))e rt. (72) We see that it is not necessary to figure out A 0 and B 0, all we need to know is A 0 +B 0. Therefore it is more efficient to straightforwardly assume y p =t s (A 1 t 0 )e rt, (73) substitute into the original equation, and figure out A 1,A 0. Now back to the general case: Let P m (t)=a m t m +a m 1 t m 1 + where y pi solves So the correct forms for y pi are Sum them up, we see that y p =y pm +y pm 1 + +a 1 t+a 0. We know that p1 +y p0 (74) ay +by +cy=a i t i e rt. (75) y pi =t s (A ii t i ii 1 t i 1 + i1 t i0 )e rt. (76) where y p =y pm +y pm 1 + p1 +y p0 =t s (A m t m + A i =A mi m 1,i + 1 t 0 )e rt (77) ii. (78) The logic of undetermined coefficients. Warning. Undetermined coefficients is the result of trial and error and cannot be completely derived deductively. So the purpose of what s below is just to understand why the formulas look the way they are. Also we ignore the issue of s in what follows to make things less involved. The basic idea of undetermined coefficients is to make a guess of the form of y p based on the equation, and the right hand side f(t). Let s see what is required for a good guess. First, it s a good idea to include f(t) in the guess. Second, if y involves f(t), then y, y involves f and f. If there is any new type of functions involved in these derivatives, but is not in y, then we may be in trouble as there is no way to balance (See below for an example). So we better include terms arising from f,f in the original guess of y. 2. Some thinking is needed to understand why it s t k in both terms! 3. Make sure you understand why the number s stays the same for y p1 and y p2!

7 Jan. 27, Finally, once such terms are included, y,y will involve terms from f,f (4) so we should include them too in y. Repeating this, we see that a good guess of y must include all terms from all possible differentiations of f(t). Example 3. Let s look at f(t)=t 2 e rt. Taking derivatives we see that f gives a new type of terms: te rt, f gives another new typee rt. But further differentiation does not pop up anything new anymore. So a good guess is Example 4. Let s look at f(t)=tcost+sint. y=(a 2 t 2 1 t 0 )e rt. (79) f cost,tsint; (80) Further differentiation does not give anything new. So the good guess should be Example 5. Let s look at f(t)=t 1. y p =(A 1 t 0 ) cost+(b 1 t+b 0 ) sint. (81) f t 2 ; f t 3 ; f t 4, (82) It clearly never ends: Every time we take one more derivative, a new type of function pops up. So if we want to include them all, we have to set y p =A 1 t 1 2 t 2 + n t n +. (83) This is in fact a legitimate approach and may work in some cases. But it s much more involved in both theory and calculation and is not undetermined coefficients anymore.

Math 201 Lecture 08 Undetermined Coefficients

Math 201 Lecture 08 Undetermined Coefficients Math 201 Lecture 08 Undetermined Coefficients Jan. 25, 2012 Many examples here are taken from the textbook. The first number in () refers to the problem number in the UA Custom edition, the second number

More information

Lecture Notes for Math 251: ODE and PDE. Lecture 12: 3.3 Complex Roots of the Characteristic Equation

Lecture Notes for Math 251: ODE and PDE. Lecture 12: 3.3 Complex Roots of the Characteristic Equation Lecture Notes for Math 21: ODE and PDE. Lecture 12: 3.3 Complex Roots of the Characteristic Equation Shawn D. Ryan Spring 2012 1 Complex Roots of the Characteristic Equation Last Time: We considered the

More information

Second Order Linear ODEs, Part II

Second Order Linear ODEs, Part II Craig J. Sutton craig.j.sutton@dartmouth.edu Department of Mathematics Dartmouth College Math 23 Differential Equations Winter 2013 Outline Non-homogeneous Linear Equations 1 Non-homogeneous Linear Equations

More information

6. Linear Differential Equations of the Second Order

6. Linear Differential Equations of the Second Order September 26, 2012 6-1 6. Linear Differential Equations of the Second Order A differential equation of the form L(y) = g is called linear if L is a linear operator and g = g(t) is continuous. The most

More information

Example. Mathematics 255: Lecture 17. Example. Example (cont d) Consider the equation. d 2 y dt 2 + dy

Example. Mathematics 255: Lecture 17. Example. Example (cont d) Consider the equation. d 2 y dt 2 + dy Mathematics 255: Lecture 17 Undetermined Coefficients Dan Sloughter Furman University October 10, 2008 6y = 5e 4t. so the general solution of 0 = r 2 + r 6 = (r + 3)(r 2), 6y = 0 y(t) = c 1 e 3t + c 2

More information

Lecture 17: Nonhomogeneous equations. 1 Undetermined coefficients method to find a particular

Lecture 17: Nonhomogeneous equations. 1 Undetermined coefficients method to find a particular Lecture 17: Nonhomogeneous equations 1 Undetermined coefficients method to find a particular solution The method of undetermined coefficients (sometimes referred to as the method of justicious guessing)

More information

Math 201 Lecture 05 Bernoulli and Linear Coefficients

Math 201 Lecture 05 Bernoulli and Linear Coefficients Math 0 Lecture 05 Bernoulli and Linear Coefficients Jan. 8, 0 Many eamples here are taken from the tetbook. The first number in () refers to the problem number in the UA Custom edition, the second number

More information

3.5 Undetermined Coefficients

3.5 Undetermined Coefficients 3.5. UNDETERMINED COEFFICIENTS 153 11. t 2 y + ty + 4y = 0, y(1) = 3, y (1) = 4 12. t 2 y 4ty + 6y = 0, y(0) = 1, y (0) = 1 3.5 Undetermined Coefficients In this section and the next we consider the nonhomogeneous

More information

MATH 308 Differential Equations

MATH 308 Differential Equations MATH 308 Differential Equations Summer, 2014, SET 6 JoungDong Kim Set 6: Section 3.3, 3.4, 3.5, 3.6 Section 3.3 Complex Roots of the Characteristic Equation Recall that a second order ODE with constant

More information

Second Order Differential Equations Lecture 6

Second Order Differential Equations Lecture 6 Second Order Differential Equations Lecture 6 Dibyajyoti Deb 6.1. Outline of Lecture Repeated Roots; Reduction of Order Nonhomogeneous Equations; Method of Undetermined Coefficients Variation of Parameters

More information

we get y 2 5y = x + e x + C: From the initial condition y(0) = 1, we get 1 5 = 0+1+C; so that C = 5. Completing the square to solve y 2 5y = x + e x 5

we get y 2 5y = x + e x + C: From the initial condition y(0) = 1, we get 1 5 = 0+1+C; so that C = 5. Completing the square to solve y 2 5y = x + e x 5 Math 24 Final Exam Solution 17 December 1999 1. Find the general solution to the differential equation ty 0 +2y = sin t. Solution: Rewriting the equation in the form (for t 6= 0),we find that y 0 + 2 t

More information

Linear algebra and differential equations (Math 54): Lecture 20

Linear algebra and differential equations (Math 54): Lecture 20 Linear algebra and differential equations (Math 54): Lecture 20 Vivek Shende April 7, 2016 Hello and welcome to class! Last time We started discussing differential equations. We found a complete set of

More information

1 Differential Equations

1 Differential Equations Reading [Simon], Chapter 24, p. 633-657. 1 Differential Equations 1.1 Definition and Examples A differential equation is an equation involving an unknown function (say y = y(t)) and one or more of its

More information

M343 Homework 6. Enrique Areyan May 31, 2013

M343 Homework 6. Enrique Areyan May 31, 2013 M343 Homework 6 Enrique Areyan May 31, 013 Section 3.5. + y + 5y = 3sin(t). The general solution is given by: y h : Characteristic equation: r + r + 5 = 0 r = 1 ± i. The solution in this case is: y h =

More information

Find the Fourier series of the odd-periodic extension of the function f (x) = 1 for x ( 1, 0). Solution: The Fourier series is.

Find the Fourier series of the odd-periodic extension of the function f (x) = 1 for x ( 1, 0). Solution: The Fourier series is. Review for Final Exam. Monday /09, :45-:45pm in CC-403. Exam is cumulative, -4 problems. 5 grading attempts per problem. Problems similar to homeworks. Integration and LT tables provided. No notes, no

More information

Selected Solutions: 3.5 (Undetermined Coefficients)

Selected Solutions: 3.5 (Undetermined Coefficients) Selected Solutions: 3.5 (Undetermined Coefficients) In Exercises 1-10, we want to apply the ideas from the table to specific DEs, and solve for the coefficients as well. If you prefer, you might start

More information

Theory of Higher-Order Linear Differential Equations

Theory of Higher-Order Linear Differential Equations Chapter 6 Theory of Higher-Order Linear Differential Equations 6.1 Basic Theory A linear differential equation of order n has the form a n (x)y (n) (x) + a n 1 (x)y (n 1) (x) + + a 0 (x)y(x) = b(x), (6.1.1)

More information

APPM 2360 Section Exam 3 Wednesday November 19, 7:00pm 8:30pm, 2014

APPM 2360 Section Exam 3 Wednesday November 19, 7:00pm 8:30pm, 2014 APPM 2360 Section Exam 3 Wednesday November 9, 7:00pm 8:30pm, 204 ON THE FRONT OF YOUR BLUEBOOK write: () your name, (2) your student ID number, (3) lecture section, (4) your instructor s name, and (5)

More information

Math 215/255: Elementary Differential Equations I Harish N Dixit, Department of Mathematics, UBC

Math 215/255: Elementary Differential Equations I Harish N Dixit, Department of Mathematics, UBC Math 215/255: Elementary Differential Equations I Harish N Dixit, Department of Mathematics, UBC First Order Equations Linear Equations y + p(x)y = q(x) Write the equation in the standard form, Calculate

More information

1. Why don t we have to worry about absolute values in the general form for first order differential equations with constant coefficients?

1. Why don t we have to worry about absolute values in the general form for first order differential equations with constant coefficients? 1. Why don t we have to worry about absolute values in the general form for first order differential equations with constant coefficients? Let y = ay b with y(0) = y 0 We can solve this as follows y =

More information

Constant coefficients systems

Constant coefficients systems 5.3. 2 2 Constant coefficients systems Section Objective(s): Diagonalizable systems. Real Distinct Eigenvalues. Complex Eigenvalues. Non-Diagonalizable systems. 5.3.. Diagonalizable Systems. Remark: We

More information

Lecture 9. Scott Pauls 1 4/16/07. Dartmouth College. Math 23, Spring Scott Pauls. Last class. Today s material. Group work.

Lecture 9. Scott Pauls 1 4/16/07. Dartmouth College. Math 23, Spring Scott Pauls. Last class. Today s material. Group work. Lecture 9 1 1 Department of Mathematics Dartmouth College 4/16/07 Outline Repeated Roots Repeated Roots Repeated Roots Material from last class Wronskian: linear independence Constant coeffecient equations:

More information

GUIDELINES FOR THE METHOD OF UNDETERMINED COEFFICIENTS

GUIDELINES FOR THE METHOD OF UNDETERMINED COEFFICIENTS GUIDELINES FOR THE METHOD OF UNDETERMINED COEFFICIENTS Given a constant coefficient linear differential equation a + by + cy = g(t), where g is an exponential, a simple sinusoidal function, a polynomial,

More information

Chapter 7. Homogeneous equations with constant coefficients

Chapter 7. Homogeneous equations with constant coefficients Chapter 7. Homogeneous equations with constant coefficients It has already been remarked that we can write down a formula for the general solution of any linear second differential equation y + a(t)y +

More information

1 Systems of Differential Equations

1 Systems of Differential Equations March, 20 7- Systems of Differential Equations Let U e an open suset of R n, I e an open interval in R and : I R n R n e a function from I R n to R n The equation ẋ = ft, x is called a first order ordinary

More information

A: Brief Review of Ordinary Differential Equations

A: Brief Review of Ordinary Differential Equations A: Brief Review of Ordinary Differential Equations Because of Principle # 1 mentioned in the Opening Remarks section, you should review your notes from your ordinary differential equations (odes) course

More information

Math53: Ordinary Differential Equations Autumn 2004

Math53: Ordinary Differential Equations Autumn 2004 Math53: Ordinary Differential Equations Autumn 2004 Unit 2 Summary Second- and Higher-Order Ordinary Differential Equations Extremely Important: Euler s formula Very Important: finding solutions to linear

More information

Solutions to Math 53 Math 53 Practice Final

Solutions to Math 53 Math 53 Practice Final Solutions to Math 5 Math 5 Practice Final 20 points Consider the initial value problem y t 4yt = te t with y 0 = and y0 = 0 a 8 points Find the Laplace transform of the solution of this IVP b 8 points

More information

Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Undetermined Coefficients Page 1

Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Undetermined Coefficients Page 1 Differential Equations Practice: 2nd Order Linear: Nonhomogeneous Equations: Undetermined Coefficients Page 1 Questions Example (3.5.3) Find a general solution of the differential equation y 2y 3y = 3te

More information

Linear Second Order ODEs

Linear Second Order ODEs Chapter 3 Linear Second Order ODEs In this chapter we study ODEs of the form (3.1) y + p(t)y + q(t)y = f(t), where p, q, and f are given functions. Since there are two derivatives, we might expect that

More information

Lecture 8: Ordinary Differential Equations

Lecture 8: Ordinary Differential Equations MIT-WHOI Joint Program Summer Math Review Summer 2015 Lecture 8: Ordinary Differential Equations Lecturer: Isabela Le Bras Date: 31 July 2015 Disclaimer: These notes are for the purposes of this review

More information

Table of contents. d 2 y dx 2, As the equation is linear, these quantities can only be involved in the following manner:

Table of contents. d 2 y dx 2, As the equation is linear, these quantities can only be involved in the following manner: M ath 0 1 E S 1 W inter 0 1 0 Last Updated: January, 01 0 Solving Second Order Linear ODEs Disclaimer: This lecture note tries to provide an alternative approach to the material in Sections 4. 4. 7 and

More information

1 Some general theory for 2nd order linear nonhomogeneous

1 Some general theory for 2nd order linear nonhomogeneous Math 175 Honors ODE I Spring, 013 Notes 5 1 Some general theory for nd order linear nonhomogeneous equations 1.1 General form of the solution Suppose that p; q; and g are continuous on an interval I; and

More information

Math 54. Selected Solutions for Week 10

Math 54. Selected Solutions for Week 10 Math 54. Selected Solutions for Week 10 Section 4.1 (Page 399) 9. Find a synchronous solution of the form A cos Ωt+B sin Ωt to the given forced oscillator equation using the method of Example 4 to solve

More information

Today. The geometry of homogeneous and nonhomogeneous matrix equations. Solving nonhomogeneous equations. Method of undetermined coefficients

Today. The geometry of homogeneous and nonhomogeneous matrix equations. Solving nonhomogeneous equations. Method of undetermined coefficients Today The geometry of homogeneous and nonhomogeneous matrix equations Solving nonhomogeneous equations Method of undetermined coefficients 1 Second order, linear, constant coeff, nonhomogeneous (3.5) Our

More information

DIFFERENTIAL EQUATIONS REVIEW. Here are notes to special make-up discussion 35 on November 21, in case you couldn t make it.

DIFFERENTIAL EQUATIONS REVIEW. Here are notes to special make-up discussion 35 on November 21, in case you couldn t make it. DIFFERENTIAL EQUATIONS REVIEW PEYAM RYAN TABRIZIAN Here are notes to special make-up discussion 35 on November 21, in case you couldn t make it. Welcome to the special Friday after-school special of That

More information

Lecture Notes for Math 251: ODE and PDE. Lecture 13: 3.4 Repeated Roots and Reduction Of Order

Lecture Notes for Math 251: ODE and PDE. Lecture 13: 3.4 Repeated Roots and Reduction Of Order Lecture Notes for Math 251: ODE and PDE. Lecture 13: 3.4 Repeated Roots and Reduction Of Order Shawn D. Ryan Spring 2012 1 Repeated Roots of the Characteristic Equation and Reduction of Order Last Time:

More information

Math 2142 Homework 5 Part 1 Solutions

Math 2142 Homework 5 Part 1 Solutions Math 2142 Homework 5 Part 1 Solutions Problem 1. For the following homogeneous second order differential equations, give the general solution and the particular solution satisfying the given initial conditions.

More information

Study guide - Math 220

Study guide - Math 220 Study guide - Math 220 November 28, 2012 1 Exam I 1.1 Linear Equations An equation is linear, if in the form y + p(t)y = q(t). Introducing the integrating factor µ(t) = e p(t)dt the solutions is then in

More information

MATH 312 Section 4.3: Homogeneous Linear Equations with Constant Coefficients

MATH 312 Section 4.3: Homogeneous Linear Equations with Constant Coefficients MATH 312 Section 4.3: Homogeneous Linear Equations with Constant Coefficients Prof. Jonathan Duncan Walla Walla College Spring Quarter, 2007 Outline 1 Getting Started 2 Second Order Equations Two Real

More information

Chapter 4: Higher Order Linear Equations

Chapter 4: Higher Order Linear Equations Chapter 4: Higher Order Linear Equations MATH 351 California State University, Northridge April 7, 2014 MATH 351 (Differential Equations) Ch 4 April 7, 2014 1 / 11 Sec. 4.1: General Theory of nth Order

More information

The Method of Undetermined Coefficients.

The Method of Undetermined Coefficients. The Method of Undetermined Coefficients. James K. Peterson Department of Biological Sciences and Department of Mathematical Sciences Clemson University May 24, 2017 Outline 1 Annihilators 2 Finding The

More information

MAT187H1F Lec0101 Burbulla

MAT187H1F Lec0101 Burbulla Spring 2017 Second Order Linear Homogeneous Differential Equation DE: A(x) d 2 y dx 2 + B(x)dy dx + C(x)y = 0 This equation is called second order because it includes the second derivative of y; it is

More information

UNDETERMINED COEFFICIENTS SUPERPOSITION APPROACH *

UNDETERMINED COEFFICIENTS SUPERPOSITION APPROACH * 4.4 UNDETERMINED COEFFICIENTS SUPERPOSITION APPROACH 19 Discussion Problems 59. Two roots of a cubic auxiliary equation with real coeffi cients are m 1 1 and m i. What is the corresponding homogeneous

More information

Work sheet / Things to know. Chapter 3

Work sheet / Things to know. Chapter 3 MATH 251 Work sheet / Things to know 1. Second order linear differential equation Standard form: Chapter 3 What makes it homogeneous? We will, for the most part, work with equations with constant coefficients

More information

Worksheet # 2: Higher Order Linear ODEs (SOLUTIONS)

Worksheet # 2: Higher Order Linear ODEs (SOLUTIONS) Name: November 8, 011 Worksheet # : Higher Order Linear ODEs (SOLUTIONS) 1. A set of n-functions f 1, f,..., f n are linearly independent on an interval I if the only way that c 1 f 1 (t) + c f (t) +...

More information

Nonhomogeneous Equations and Variation of Parameters

Nonhomogeneous Equations and Variation of Parameters Nonhomogeneous Equations Variation of Parameters June 17, 2016 1 Nonhomogeneous Equations 1.1 Review of First Order Equations If we look at a first order homogeneous constant coefficient ordinary differential

More information

MATH 24 EXAM 3 SOLUTIONS

MATH 24 EXAM 3 SOLUTIONS MATH 4 EXAM 3 S Consider the equation y + ω y = cosω t (a) Find the general solution of the homogeneous equation (b) Find the particular solution of the non-homogeneous equation using the method of Undetermined

More information

Old Math 330 Exams. David M. McClendon. Department of Mathematics Ferris State University

Old Math 330 Exams. David M. McClendon. Department of Mathematics Ferris State University Old Math 330 Exams David M. McClendon Department of Mathematics Ferris State University Last updated to include exams from Fall 07 Contents Contents General information about these exams 3 Exams from Fall

More information

Algebra & Trig Review

Algebra & Trig Review Algebra & Trig Review 1 Algebra & Trig Review This review was originally written for my Calculus I class, but it should be accessible to anyone needing a review in some basic algebra and trig topics. The

More information

Work sheet / Things to know. Chapter 3

Work sheet / Things to know. Chapter 3 MATH 251 Work sheet / Things to know 1. Second order linear differential equation Standard form: Chapter 3 What makes it homogeneous? We will, for the most part, work with equations with constant coefficients

More information

Higher-order differential equations

Higher-order differential equations Higher-order differential equations Peyam Tabrizian Wednesday, November 16th, 2011 This handout is meant to give you a couple more example of all the techniques discussed in chapter 6, to counterbalance

More information

Section 9.8 Higher Order Linear Equations

Section 9.8 Higher Order Linear Equations Section 9.8 Higher Order Linear Equations Key Terms: Higher order linear equations Equivalent linear systems for higher order equations Companion matrix Characteristic polynomial and equation A linear

More information

Math : Solutions to Assignment 10

Math : Solutions to Assignment 10 Math -3: Solutions to Assignment. There are two tanks. The first tank initially has gallons of pure water. The second tank initially has 8 gallons of a water/salt solution with oz of salt. Both tanks drain

More information

Math 216 Second Midterm 19 March, 2018

Math 216 Second Midterm 19 March, 2018 Math 26 Second Midterm 9 March, 28 This sample exam is provided to serve as one component of your studying for this exam in this course. Please note that it is not guaranteed to cover the material that

More information

MATH 320 INHOMOGENEOUS LINEAR SYSTEMS OF DIFFERENTIAL EQUATIONS

MATH 320 INHOMOGENEOUS LINEAR SYSTEMS OF DIFFERENTIAL EQUATIONS MATH 2 INHOMOGENEOUS LINEAR SYSTEMS OF DIFFERENTIAL EQUATIONS W To find a particular solution for a linear inhomogeneous system of differential equations x Ax = ft) or of a mechanical system with external

More information

SECOND ORDER ODE S. 1. A second order differential equation is an equation of the form. F (x, y, y, y ) = 0.

SECOND ORDER ODE S. 1. A second order differential equation is an equation of the form. F (x, y, y, y ) = 0. SECOND ORDER ODE S 1. A second der differential equation is an equation of the fm F (x, y, y, y ) = 0. A solution of the differential equation is a function y = y(x) that satisfies the equation. A differential

More information

1 y 2 dy = (2 + t)dt 1 y. = 2t + t2 2 + C 1 2t + t 2 /2 + C. 1 t 2 /2 + 2t 1. e y y = 2t 2. e y dy = 2t 2 dt. e y = 2 3 t3 + C. y = ln( 2 3 t3 + C).

1 y 2 dy = (2 + t)dt 1 y. = 2t + t2 2 + C 1 2t + t 2 /2 + C. 1 t 2 /2 + 2t 1. e y y = 2t 2. e y dy = 2t 2 dt. e y = 2 3 t3 + C. y = ln( 2 3 t3 + C). Math 53 First Midterm Page. Solve each of the following initial value problems. (a) y = y + ty, y() = 3. The equation is separable : y = y ( + t). Thus y = y dy = ( + t)dt y = t + t + C t + t / + C. For

More information

Section 6.4 DEs with Discontinuous Forcing Functions

Section 6.4 DEs with Discontinuous Forcing Functions Section 6.4 DEs with Discontinuous Forcing Functions Key terms/ideas: Discontinuous forcing function in nd order linear IVPs Application of Laplace transforms Comparison to viewing the problem s solution

More information

Solutions to the Homework Replaces Section 3.7, 3.8

Solutions to the Homework Replaces Section 3.7, 3.8 Solutions to the Homework Replaces Section 3.7, 3.8. Show that the period of motion of an undamped vibration of a mass hanging from a vertical spring is 2π L/g SOLUTION: With no damping, mu + ku = 0 has

More information

Solutions to Homework 3

Solutions to Homework 3 Solutions to Homework 3 Section 3.4, Repeated Roots; Reduction of Order Q 1). Find the general solution to 2y + y = 0. Answer: The charactertic equation : r 2 2r + 1 = 0, solving it we get r = 1 as a repeated

More information

Solutions to the Homework Replaces Section 3.7, 3.8

Solutions to the Homework Replaces Section 3.7, 3.8 Solutions to the Homework Replaces Section 3.7, 3.8 1. Our text (p. 198) states that µ ω 0 = ( 1 γ2 4km ) 1/2 1 1 2 γ 2 4km How was this approximation made? (Hint: Linearize 1 x) SOLUTION: We linearize

More information

IV Higher Order Linear ODEs

IV Higher Order Linear ODEs IV Higher Order Linear ODEs Boyce & DiPrima, Chapter 4 H.J.Eberl - MATH*2170 0 IV Higher Order Linear ODEs IV.1 General remarks Boyce & DiPrima, Section 4.1 H.J.Eberl - MATH*2170 1 Problem formulation

More information

Math 23: Differential Equations (Winter 2017) Midterm Exam Solutions

Math 23: Differential Equations (Winter 2017) Midterm Exam Solutions Math 3: Differential Equations (Winter 017) Midterm Exam Solutions 1. [0 points] or FALSE? You do not need to justify your answer. (a) [3 points] Critical points or equilibrium points for a first order

More information

1. (10 points) Find the general solution to the following second-order differential equation:

1. (10 points) Find the general solution to the following second-order differential equation: Math 307A, Winter 014 Midterm Solutions Page 1 of 8 1. (10 points) Find the general solution to the following second-order differential equation: 4y 1y + 9y = 9t. To find the general solution to this nonhomogeneous

More information

Partial proof: y = ϕ 1 (t) is a solution to y + p(t)y = 0 implies. Thus y = cϕ 1 (t) is a solution to y + p(t)y = 0 since

Partial proof: y = ϕ 1 (t) is a solution to y + p(t)y = 0 implies. Thus y = cϕ 1 (t) is a solution to y + p(t)y = 0 since Existence and Uniqueness for LINEAR DEs. Homogeneous: y (n) + p 1 (t)y (n 1) +...p n 1 (t)y + p n (t)y = 0 Non-homogeneous: g(t) 0 y (n) + p 1 (t)y (n 1) +...p n 1 (t)y + p n (t)y = g(t) 1st order LINEAR

More information

Name: Solutions Final Exam

Name: Solutions Final Exam Instructions. Answer each of the questions on your own paper. Put your name on each page of your paper. Be sure to show your work so that partial credit can be adequately assessed. Credit will not be given

More information

DIFFERENTIAL EQUATIONS

DIFFERENTIAL EQUATIONS DIFFERENTIAL EQUATIONS Basic Concepts Paul Dawkins Table of Contents Preface... Basic Concepts... 1 Introduction... 1 Definitions... Direction Fields... 8 Final Thoughts...19 007 Paul Dawkins i http://tutorial.math.lamar.edu/terms.aspx

More information

Math 211. Substitute Lecture. November 20, 2000

Math 211. Substitute Lecture. November 20, 2000 1 Math 211 Substitute Lecture November 20, 2000 2 Solutions to y + py + qy =0. Look for exponential solutions y(t) =e λt. Characteristic equation: λ 2 + pλ + q =0. Characteristic polynomial: λ 2 + pλ +

More information

Math 20D Final Exam 8 December has eigenvalues 3, 3, 0 and find the eigenvectors associated with 3. ( 2) det

Math 20D Final Exam 8 December has eigenvalues 3, 3, 0 and find the eigenvectors associated with 3. ( 2) det Math D Final Exam 8 December 9. ( points) Show that the matrix 4 has eigenvalues 3, 3, and find the eigenvectors associated with 3. 4 λ det λ λ λ = (4 λ) det λ ( ) det + det λ = (4 λ)(( λ) 4) + ( λ + )

More information

One sided tests. An example of a two sided alternative is what we ve been using for our two sample tests:

One sided tests. An example of a two sided alternative is what we ve been using for our two sample tests: One sided tests So far all of our tests have been two sided. While this may be a bit easier to understand, this is often not the best way to do a hypothesis test. One simple thing that we can do to get

More information

Algebra Year 10. Language

Algebra Year 10. Language Algebra Year 10 Introduction In Algebra we do Maths with numbers, but some of those numbers are not known. They are represented with letters, and called unknowns, variables or, most formally, literals.

More information

Introduction. So, why did I even bother to write this?

Introduction. So, why did I even bother to write this? Introduction This review was originally written for my Calculus I class, but it should be accessible to anyone needing a review in some basic algebra and trig topics. The review contains the occasional

More information

Exam Basics. midterm. 1 There will be 9 questions. 2 The first 3 are on pre-midterm material. 3 The next 1 is a mix of old and new material.

Exam Basics. midterm. 1 There will be 9 questions. 2 The first 3 are on pre-midterm material. 3 The next 1 is a mix of old and new material. Exam Basics 1 There will be 9 questions. 2 The first 3 are on pre-midterm material. 3 The next 1 is a mix of old and new material. 4 The last 5 questions will be on new material since the midterm. 5 60

More information

MA Ordinary Differential Equations

MA Ordinary Differential Equations MA 108 - Ordinary Differential Equations Santanu Dey Department of Mathematics, Indian Institute of Technology Bombay, Powai, Mumbai 76 dey@math.iitb.ac.in March 26, 2014 Outline of the lecture Method

More information

Continuity and One-Sided Limits

Continuity and One-Sided Limits Continuity and One-Sided Limits 1. Welcome to continuity and one-sided limits. My name is Tuesday Johnson and I m a lecturer at the University of Texas El Paso. 2. With each lecture I present, I will start

More information

First order equations. The variation of parameters formula gives for the solution of the initial-value problem:

First order equations. The variation of parameters formula gives for the solution of the initial-value problem: Linear differential equations with discontinuous forcing terms Many external effects are modeled as forces starting to act on the system instantaneously at some positive time, either persisting or being

More information

Math 3313: Differential Equations Second-order ordinary differential equations

Math 3313: Differential Equations Second-order ordinary differential equations Math 3313: Differential Equations Second-order ordinary differential equations Thomas W. Carr Department of Mathematics Southern Methodist University Dallas, TX Outline Mass-spring & Newton s 2nd law Properties

More information

APPM 2360: Midterm 3 July 12, 2013.

APPM 2360: Midterm 3 July 12, 2013. APPM 2360: Midterm 3 July 12, 2013. ON THE FRONT OF YOUR BLUEBOOK write: (1) your name, (2) your instructor s name, (3) your recitation section number and (4) a grading table. Text books, class notes,

More information

5.2 Infinite Series Brian E. Veitch

5.2 Infinite Series Brian E. Veitch 5. Infinite Series Since many quantities show up that cannot be computed exactly, we need some way of representing it (or approximating it). One way is to sum an infinite series. Recall that a n is the

More information

Chapter 3 : Linear Differential Eqn. Chapter 3 : Linear Differential Eqn.

Chapter 3 : Linear Differential Eqn. Chapter 3 : Linear Differential Eqn. 1.0 Introduction Linear differential equations is all about to find the total solution y(t), where : y(t) = homogeneous solution [ y h (t) ] + particular solution y p (t) General form of differential equation

More information

= 2e t e 2t + ( e 2t )e 3t = 2e t e t = e t. Math 20D Final Review

= 2e t e 2t + ( e 2t )e 3t = 2e t e t = e t. Math 20D Final Review Math D Final Review. Solve the differential equation in two ways, first using variation of parameters and then using undetermined coefficients: Corresponding homogenous equation: with characteristic equation

More information

Section 4.7: Variable-Coefficient Equations

Section 4.7: Variable-Coefficient Equations Cauchy-Euler Equations Section 4.7: Variable-Coefficient Equations Before concluding our study of second-order linear DE s, let us summarize what we ve done. In Sections 4.2 and 4.3 we showed how to find

More information

A First Course in Elementary Differential Equations: Problems and Solutions. Marcel B. Finan Arkansas Tech University c All Rights Reserved

A First Course in Elementary Differential Equations: Problems and Solutions. Marcel B. Finan Arkansas Tech University c All Rights Reserved A First Course in Elementary Differential Equations: Problems and Solutions Marcel B. Finan Arkansas Tech University c All Rights Reserved 1 4 The Method of Variation of Parameters Problem 4.1 Solve y

More information

MATHEMATICS FOR ENGINEERS & SCIENTISTS 23

MATHEMATICS FOR ENGINEERS & SCIENTISTS 23 MATHEMATICS FOR ENGINEERS & SCIENTISTS 3.5. Second order linear O.D.E.s: non-homogeneous case.. We ll now consider non-homogeneous second order linear O.D.E.s. These are of the form a + by + c rx) for

More information

Calculus IV - HW 3. Due 7/ Give the general solution to the following differential equations: y = c 1 e 5t + c 2 e 5t. y = c 1 e 2t + c 2 e 4t.

Calculus IV - HW 3. Due 7/ Give the general solution to the following differential equations: y = c 1 e 5t + c 2 e 5t. y = c 1 e 2t + c 2 e 4t. Calculus IV - HW 3 Due 7/13 Section 3.1 1. Give the general solution to the following differential equations: a y 25y = 0 Solution: The characteristic equation is r 2 25 = r 5r + 5. It follows that the

More information

APPM 2360: Final Exam 10:30am 1:00pm, May 6, 2015.

APPM 2360: Final Exam 10:30am 1:00pm, May 6, 2015. APPM 23: Final Exam :3am :pm, May, 25. ON THE FRONT OF YOUR BLUEBOOK write: ) your name, 2) your student ID number, 3) lecture section, 4) your instructor s name, and 5) a grading table for eight questions.

More information

Math 308 Week 8 Solutions

Math 308 Week 8 Solutions Math 38 Week 8 Solutions There is a solution manual to Chapter 4 online: www.pearsoncustom.com/tamu math/. This online solutions manual contains solutions to some of the suggested problems. Here are solutions

More information

4.3 Linear, Homogeneous Equations with Constant Coefficients. Jiwen He

4.3 Linear, Homogeneous Equations with Constant Coefficients. Jiwen He 4.3 Exercises Math 3331 Differential Equations 4.3 Linear, Homogeneous Equations with Constant Coefficients Jiwen He Department of Mathematics, University of Houston jiwenhe@math.uh.edu math.uh.edu/ jiwenhe/math3331

More information

Higher Order Linear ODEs

Higher Order Linear ODEs c03.qxd 6/18/11 2:57 PM Page 57 CHAPTER 3 Higher Order Linear ODEs Chapters 1 and 2 demonstrate and illustrate that first- and second-order ODEs are, by far, the most important ones in usual engineering

More information

Math 111, Introduction to the Calculus, Fall 2011 Midterm I Practice Exam 1 Solutions

Math 111, Introduction to the Calculus, Fall 2011 Midterm I Practice Exam 1 Solutions Math 111, Introduction to the Calculus, Fall 2011 Midterm I Practice Exam 1 Solutions For each question, there is a model solution (showing you the level of detail I expect on the exam) and then below

More information

µ = e R p(t)dt where C is an arbitrary constant. In the presence of an initial value condition

µ = e R p(t)dt where C is an arbitrary constant. In the presence of an initial value condition MATH 3860 REVIEW FOR FINAL EXAM The final exam will be comprehensive. It will cover materials from the following sections: 1.1-1.3; 2.1-2.2;2.4-2.6;3.1-3.7; 4.1-4.3;6.1-6.6; 7.1; 7.4-7.6; 7.8. The following

More information

ACCUPLACER MATH 0310

ACCUPLACER MATH 0310 The University of Teas at El Paso Tutoring and Learning Center ACCUPLACER MATH 00 http://www.academics.utep.edu/tlc MATH 00 Page Linear Equations Linear Equations Eercises 5 Linear Equations Answer to

More information

Exam II Review: Selected Solutions and Answers

Exam II Review: Selected Solutions and Answers November 9, 2011 Exam II Review: Selected Solutions and Answers NOTE: For additional worked problems see last year s review sheet and answers, the notes from class, and your text. Answers to problems from

More information

Lecture 6: Differential Equations Describing Vibrations

Lecture 6: Differential Equations Describing Vibrations Lecture 6: Differential Equations Describing Vibrations In Chapter 3 of the Benson textbook, we will look at how various types of musical instruments produce sound, focusing on issues like how the construction

More information

MATH 1910 Limits Numerically and Graphically Introduction to Limits does not exist DNE DOES does not Finding Limits Numerically

MATH 1910 Limits Numerically and Graphically Introduction to Limits does not exist DNE DOES does not Finding Limits Numerically MATH 90 - Limits Numerically and Graphically Introduction to Limits The concept of a limit is our doorway to calculus. This lecture will explain what the limit of a function is and how we can find such

More information

REVIEW PROBLEMS FOR MIDTERM II MATH 2373, FALL 2016 ANSWER KEY

REVIEW PROBLEMS FOR MIDTERM II MATH 2373, FALL 2016 ANSWER KEY REVIEW PROBLEMS FOR MIDTERM II MATH 7, FALL 6 ANSWER KEY This list of problems is not guaranteed to be an absolutely complete review. For completeness you must also make sure that you know how to do all

More information

Descriptive Statistics (And a little bit on rounding and significant digits)

Descriptive Statistics (And a little bit on rounding and significant digits) Descriptive Statistics (And a little bit on rounding and significant digits) Now that we know what our data look like, we d like to be able to describe it numerically. In other words, how can we represent

More information

Ex. 1. Find the general solution for each of the following differential equations:

Ex. 1. Find the general solution for each of the following differential equations: MATH 261.007 Instr. K. Ciesielski Spring 2010 NAME (print): SAMPLE TEST # 2 Solve the following exercises. Show your work. (No credit will be given for an answer with no supporting work shown.) Ex. 1.

More information

Chapter 5 Simplifying Formulas and Solving Equations

Chapter 5 Simplifying Formulas and Solving Equations Chapter 5 Simplifying Formulas and Solving Equations Look at the geometry formula for Perimeter of a rectangle P = L W L W. Can this formula be written in a simpler way? If it is true, that we can simplify

More information