Practice problems Oleg Ivrii July 12, 2020 Oleg Ivrii Practice - - PowerPoint PPT Presentation

practice problems
SMART_READER_LITE
LIVE PREVIEW

Practice problems Oleg Ivrii July 12, 2020 Oleg Ivrii Practice - - PowerPoint PPT Presentation

Practice problems Oleg Ivrii July 12, 2020 Oleg Ivrii Practice problems Exam topics The exam will have 6 problems, the topics are: 1 Solve an IVP or a BVP 2 Gronwalls inequality, continuation of solutions 3 ODEs with variable coefficients


slide-1
SLIDE 1

Practice problems

Oleg Ivrii July 12, 2020

Oleg Ivrii Practice problems

slide-2
SLIDE 2

Exam topics

The exam will have 6 problems, the topics are:

1 Solve an IVP or a BVP 2 Gronwall’s inequality, continuation of solutions 3 ODEs with variable coefficients and Wronskians 4 Laplace transform 5 Boundary value problems and the maximum principle 6 Eigenvalue problems and the Sturm-Liouville Theorem Oleg Ivrii Practice problems

slide-3
SLIDE 3

Solve an IVP or a BVP

  • 1. Solve the initial value problem

y′′ + 3y′ + 2y = x3 with the initial conditions y(0) = y′(0) = 0.

Oleg Ivrii Practice problems

slide-4
SLIDE 4

Solve an IVP or a BVP

  • 2. Solve the boundary value problem

y′′ + y = sin(2x), y(0) = 0, y(π) = 0.

Oleg Ivrii Practice problems

slide-5
SLIDE 5

Solve an IVP or a BVP

  • 3. Show that the boundary value problem

y′′ + y = x, y(0) + y′(0) = 0, y(π/2) − y′(π/2) = π/2 has no solution.

Oleg Ivrii Practice problems

slide-6
SLIDE 6

Solve an IVP or a BVP

  • 4. Solve the following boundary value problem

y′′ + 2y′ + 10y = 0, y(0) = y(π/6), y(π/6) = y′(π/6).

Oleg Ivrii Practice problems

slide-7
SLIDE 7

Gronwall’s inequality, continuation of solutions

  • 1. Let y(x) be a solution of the IVP

y′ = y − y2, y(0) = a, 0 < a < 1. Show that a < y(x) ≤ 1 for all x ∈ (0, ∞).

Oleg Ivrii Practice problems

slide-8
SLIDE 8

Gronwall’s inequality, continuation of solutions

  • 2. (Exercise 3, Problem 1) Let y(x) be the solution of the initial

value problem

  • y′(x) = y2 − x,

y(0) = 1, defined for x ∈ (−ε, ε). Show that y(x) extends to the interval [0, 1) with the bounds 1 + x < y(x) < 1 1 − x , x ∈ [0, 1).

Oleg Ivrii Practice problems

slide-9
SLIDE 9

Gronwall’s inequality, continuation of solutions

  • 3. (a) Show that the Riccati equation

y′ = 1 + x2 + y2 has no solution on the interval (0, π). (b) Show that the Riccati equation y′ = 1 + y2 − x2 has a unique solution defined on the entire real axis.

Oleg Ivrii Practice problems

slide-10
SLIDE 10

Gronwall’s inequality, continuation of solutions

  • 4. Show that the IVP

y′ = f (x, y), y(0) = a has at most one solution provided y → f (x, y) is non-decreasing for any x ∈ R.

Oleg Ivrii Practice problems

slide-11
SLIDE 11

ODEs with variable coefficients and Wronskians

  • 1. (a) Suppose u, v be two linearly independent solutions of the

second-order linear homogenous ODE y′′ + p(x)y′ + q(x) = 0. Show that p(x) = −W ′(u, v)(x) W (u, v)(x) , q(x) = W (u′, v′)(x) W (u, v)(x) . (b) Construct a second-order linear homogenous ODE which has solutions u(x) = x and v(x) = sin x.

Oleg Ivrii Practice problems

slide-12
SLIDE 12

ODEs with variable coefficients and Wronskians

  • 2. (Exercise 5, Problem 3) Consider the inhomogeneous Euler

equation y′′ − 2 x · y′ + 2 x2 · y = f (x). (a) Check that y1(x) = x solves the homogeneous Euler equation with f (x) = 0. Find a complementary solution y2(x). (b) Use the method of variation of parameters to write down the general solution of the inhomogeneous Euler equation.

Oleg Ivrii Practice problems

slide-13
SLIDE 13

ODEs with variable coefficients and Wronskians

  • 3. Find the general solution of

y′′′ − 2y′′ − y′ + 2y = 12e2x ex + 1

  • Hint. All roots are integers or complex integers.

Oleg Ivrii Practice problems

slide-14
SLIDE 14

ODEs with variable coefficients and Wronskians

  • 4. (a) Find the general solution of

y′′′ + y′′ + y′ + y = ex. (b) Find the general solution of y′′′ + y′′ + y′ + y = tan x.

  • Hint. All roots are integers or complex integers.

Oleg Ivrii Practice problems

slide-15
SLIDE 15

Boundary value problems and the maximum principle

  • 1. Show that the following boundary value problems have at least
  • ne solution:

(a) y′′ = 1 + x2e−y, y(0) = 1, y(1) = 7, (b) y′′ = sin x cos y + ex, y(0) = 0, y(1) = 1.

Oleg Ivrii Practice problems

slide-16
SLIDE 16

Boundary value problems and the maximum principle

  • 2. Show that the following boundary value problems have at most
  • ne solution:

(a) y′′ = y3 + x, y(0) = 0, y(1) = 1, (b) y′′ = y + cos y + x2, y(0) = 1, y(1) = 5.

Oleg Ivrii Practice problems

slide-17
SLIDE 17

Boundary value problems and the maximum principle

  • 3. (Exercise 5, Problem 4) Show that the boundary value problem

y′′ − xy = 0, x ∈ (0, 1), y(0) = 0, y(1) = 1 has a unique solution. Prove the bounds: x + x2 2 ≤ y(x) ≤ x, x ∈ [0, 1].

  • Note. The problem asks you to prove three things: existence,

uniqueness and the relevant bounds. Each part requires some imagination but can be done separately.

Oleg Ivrii Practice problems

slide-18
SLIDE 18

Boundary value problems and the maximum principle

  • 4. (Exercise 11, Problem 4) Show that the initial value problem

y′′ + y′/x − y = 0, x ∈ (0, 1), y(0) = 1, y′(0) = 0 has a unique solution. Prove the bounds: 1 + x2/4 ≤ y(x) ≤ 1 + x2/3, x ∈ [0, 1].

  • Note. The problem asks you to prove three things: existence,

uniqueness and the relevant bounds. Each part requires some imagination but can be done separately.

Oleg Ivrii Practice problems

slide-19
SLIDE 19

Laplace transform

  • 1. Solve the initial value problem

y′′ − 2y′ + 2y = 0, y(0) = 2, y′(0) = 0 with help of the Laplace transform.

Oleg Ivrii Practice problems

slide-20
SLIDE 20

Laplace transform

  • 2. Solve the initial value problem

y′′ − 4y′ + 4y = 0, y(0) = 1, y′(0) = 1 with help of the Laplace transform.

Oleg Ivrii Practice problems

slide-21
SLIDE 21

Laplace transform

  • 3. Solve the initial value problem

y′′ − 3y′ + 2y = g(t), y(0) = 0, y′(0) = 0, with help of the Laplace transform, where g(t) =

  • sin t,

0 ≤ t ≤ π, 0, t ≥ 0.

Oleg Ivrii Practice problems

slide-22
SLIDE 22

Laplace transform

  • 4. The Bessel function of order zero has the power series expansion

J0(t) =

  • n=0

(−1)nt2n 22n(n!)2 . Show that L

  • J0(t)
  • (s) =

1 √ s2 + 1 and L

  • J0(

√ t)

  • (s) = e−s/4

s .

Oleg Ivrii Practice problems

slide-23
SLIDE 23

Eigenvalue problems and the Sturm-Liouville Theorem

  • 1. You are given that the Sturm-Liouville problem

y′′ = −λy, y(0) = 0, y(1) = 0, has normalized eigenfunctions φn(x) = √ 2 sin(nπx), λn = n2π2. Use this information to solve y′′ = sin(2πx) − sin(3πx), y(0) = 0, y(1) = 0.

Oleg Ivrii Practice problems

slide-24
SLIDE 24

Eigenvalue problems and the Sturm-Liouville Theorem

  • 2. You are given that the Sturm-Liouville problem

y′′ = −λy, y(0) = 0, y(1) = 0, has normalized eigenfunctions φn(x) = √ 2 sin(nπx), λn = n2π2. Find a sequence of coefficients {an} such that y = anφn solves y′′ = x − x2, y(0) = 0, y(1) = 0.

Oleg Ivrii Practice problems

slide-25
SLIDE 25

Eigenvalue problems and the Sturm-Liouville Theorem

  • 3. Solve the eigenvalue problem

−y′′ = λy, x ∈ (0, 1), with the boundary conditions y(0) = y′(1) = 0. Write down the associated eigenfunctions.

Oleg Ivrii Practice problems

slide-26
SLIDE 26

Eigenvalue problems and the Sturm-Liouville Theorem

  • 4. Write down a particular solution to the wave equation on

x ∈ [0, 1] and t ∈ [0, ∞]:              utt = uxx, u(t, 0) = u(t, 1) = 0, u(0, x) = 2 sin(2πx) − 3 sin(3πx), ut(0, x) = 0.

Oleg Ivrii Practice problems

slide-27
SLIDE 27

Thank you for your attention!

Oleg Ivrii Practice problems