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Fall 2018 MATH 2930: Review of First & Second Order Differential Equations, Summaries of Differential Equations

Solutions to exercises on approximating solutions to first order differential equations using euler's method and finding general solutions to second order linear homogeneous differential equations with constant coefficients. It covers topics such as euler's method, general solutions of differential equations, and the behavior of solutions as t increases.

What you will learn

  • What is the general solution of a second order linear homogeneous differential equation with constant coefficients?
  • How to approximate solutions to first order differential equations using Euler's method?
  • How does the behavior of solutions change as t increases for a second order linear homogeneous differential equation?

Typology: Summaries

2021/2022

Uploaded on 09/12/2022

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MATH 2930, Fall 2018
TA: Aleksandra Niepla
Sections: 212, 217 Name:
Chapter 2.7, 3.1, 3.3 Review
Objectives: (1) Approximate solutions to first order differential equations using Euler’s method (2) Practice
solving second order linear homogeneous differential equations with constant coefficients
Part 1- Numerical Approximations: Euler’s Method
1. Consider the initial value problem
y0= 0.5t+ 2y, y(0) = 1
(i) Find approximate values of the solution of the given initial value problem at t= 0.1,0.2,0.3,and 0.4
using Euler’s method with h= 0.1.
(ii) Find the solution y(t) of the given problem and evaluate y(t) at t= 0.1,0.2,0.3,and 0.4.Compare
your results with those of part (i).
(i) We have the following approximations:
(ii) Rewriting the equation we have:
y02y= 0.5t.
Let µ(t) = eR2dt =e2t.Then
(e2ty(t))0= 0.5e2tte2t.
Integrating both sides and dividing by e2twe get:
y(t) = t
2+Ce2t.
The initial condition implies that C= 1.So, the solutions is:
y(t) = t/2 + e2t.
Moreover, using a calculator we have:
y(0.1) = 1.27, y(0.2) = 1.59, y(0.3) = 1.97, y (0.4) = 2.43.
Part 2- Second Order Linear Differential Equations
1. Find the general solution of the given differential equation
y00 + 2y03y= 0.
The characteristic equation is
pf3
pf4

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MATH 2930, Fall 2018 TA: Aleksandra Niepla Sections: 212, 217 (^) Name:

Chapter 2.7, 3.1, 3.3 Review

Objectives: (1) Approximate solutions to first order differential equations using Euler’s method (2) Practice solving second order linear homogeneous differential equations with constant coefficients

Part 1- Numerical Approximations: Euler’s Method

  1. Consider the initial value problem

y′^ = 0. 5 − t + 2y, y(0) = 1

(i) Find approximate values of the solution of the given initial value problem at t = 0. 1 , 0. 2 , 0. 3 , and 0. 4 using Euler’s method with h = 0. 1. (ii) Find the solution y(t) of the given problem and evaluate y(t) at t = 0. 1 , 0. 2 , 0. 3 , and 0. 4. Compare your results with those of part (i).

(i) We have the following approximations:

(ii) Rewriting the equation we have:

y′^ − 2 y = 0. 5 − t. Let μ(t) = e

∫ (^) − 2 dt = e−^2 t. Then (e−^2 ty(t))′^ = 0. 5 e−^2 t^ − te−^2 t. Integrating both sides and dividing by e−^2 t^ we get:

y(t) = t 2

  • Ce^2 t. The initial condition implies that C = 1. So, the solutions is:

y(t) = t/2 + e^2 t. Moreover, using a calculator we have:

y(0.1) = 1. 27 , y(0.2) = 1. 59 , y(0.3) = 1. 97 , y(0.4) = 2. 43.

Part 2- Second Order Linear Differential Equations

  1. Find the general solution of the given differential equation

y′′^ + 2y′^ − 3 y = 0.

The characteristic equation is

r^2 + 2r − 3 = 0. We factor to find its roots:

r^2 + 2r − 3 = 0 =⇒ (r + 3)(r − 1) = 0 =⇒ r 1 = − 3 , r 2 = 1. So, the general solutions is y(t) = c 1 e−^3 t^ + c 2 et.

  1. Find the solution of the given initial value problem. Describe its behavior as t increases:

y′′^ + 8y′^ − 9 y = 0 y(1) = 1, y′(1) = 0.

The characteristic equation is

r^2 + 8r − 9 − 0. We factor to find its roots

r^2 + 8r − 9 = 0 =⇒ (r + 9)(r − 1) = 0 =⇒ r 1 = − 9 , r 2 = 1. Therefore, the general solutions is

y(t) = c 1 e−^9 t^ + c 2 et. Using the two initial conditions provided we obtain the following system of equations:

c 1 e−^9 + c 2 e = 1 and − 9 c 1 e−^9 + c 2 e = 0 Multiplying the first by 9 and adding to the second gives:

10 ec 2 = 9 =⇒ c 2 =

e−^1.

Next, we can plug c 2 into the first equation and solve for c 1 :

c 1 e−^9 +^9 10 = 1 =⇒ c 1 = 1 10 e^9.

So, the final solutions is:

y(t) =

10 e

−9(t−1) (^) +^9 10 e

t− (^1) ; y → ∞ as t → ∞.

  1. Find the general solution of the given differential equation

y′′^ + 6y′^ + 13y = 0.

The characteristic equation is

r^2 + 6r + 13 = 0. The roots are:

r =

= − 3 − 2 i, −3 + 2i.

So, the general solutions is y(t) = c 1 e−^3 t^ cos(2t) + c 2 sin(2t)e−^3 t.

d^2 y dt^2

d dt

dy dx

t

dy dx

t^2

d^2 y dx^2

t^2

dy dx

t^2

t^2

d^2 y dx^2

dy dx

Plugging this into the differential equation we obtain:

d^2 dx^2

dy dx

dy dx

  • 2y = 0.

This is now a homogeneous second order differential equation with characteristic equation:

r^2 + 3r + 2 = 0. The roots are r = − 1 , − 2. So the general solution is:

y(x) = c 1 e−x^ + c 2 e−^2 x.

Finally, using that x = ln(t), we get

y(t) = c 1 t−^1 + c 2 t−^2.