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Distinct Roots of Second Order Equations

Slide Duration:

Section 1: First-Order Equations
Linear Equations

1h 7m 21s

Intro
0:00
Lesson Objectives
0:19
How to Solve Linear Equations
2:54
Calculate the Integrating Factor
2:58
Changes the Left Side so We Can Integrate Both Sides
3:27
Solving Linear Equations
5:32
Further Notes
6:10
If P(x) is Negative
6:26
Leave Off the Constant
9:38
The C Is Important When Integrating Both Sides of the Equation
9:55
Example 1
10:29
Example 2
22:56
Example 3
36:12
Example 4
39:24
Example 5
44:10
Example 6
56:42
Separable Equations

35m 11s

Intro
0:00
Lesson Objectives
0:19
Some Equations Are Both Linear and Separable So You Can Use Either Technique to Solve Them
1:33
Important to Add C When You Do the Integration
2:27
Example 1
4:28
Example 2
10:45
Example 3
14:43
Example 4
19:21
Example 5
27:23
Slope & Direction Fields

1h 11m 36s

Intro
0:00
Lesson Objectives
0:20
If You Can Manipulate a Differential Equation Into a Certain Form, You Can Draw a Slope Field Also Known as a Direction Field
0:23
How You Do This
0:45
Solution Trajectories
2:49
Never Cross Each Other
3:44
General Solution to the Differential Equation
4:03
Use an Initial Condition to Find Which Solution Trajectory You Want
4:59
Example 1
6:52
Example 2
14:20
Example 3
26:36
Example 4
34:21
Example 5
46:09
Example 6
59:51
Applications, Modeling, & Word Problems of First-Order Equations

1h 5m 19s

Intro
0:00
Lesson Overview
0:38
Mixing
1:00
Population
2:49
Finance
3:22
Set Variables
4:39
Write Differential Equation
6:29
Solve It
10:54
11:47
Example 1
13:29
Example 2
24:53
Example 3
32:13
Example 4
42:46
Example 5
55:05
Autonomous Equations & Phase Plane Analysis

1h 1m 20s

Intro
0:00
Lesson Overview
0:18
Autonomous Differential Equations Have the Form y' = f(x)
0:21
Phase Plane Analysis
0:48
y' < 0
2:56
y' > 0
3:04
If we Perturb the Equilibrium Solutions
5:51
Equilibrium Solutions
7:44
8:06
Solutions Will Tend Away From Unstable Equilibria
9:32
Semistable Equilibria
10:59
Example 1
11:43
Example 2
15:50
Example 3
28:27
Example 4
31:35
Example 5
43:03
Example 6
49:01
Section 2: Second-Order Equations
Distinct Roots of Second Order Equations

28m 44s

Intro
0:00
Lesson Overview
0:36
Linear Means
0:50
Second-Order
1:15
Homogeneous
1:30
Constant Coefficient
1:55
Solve the Characteristic Equation
2:33
Roots r1 and r2
3:43
To Find c1 and c2, Use Initial Conditions
4:50
Example 1
5:46
Example 2
8:20
Example 3
16:20
Example 4
18:26
Example 5
23:52
Complex Roots of Second Order Equations

31m 49s

Intro
0:00
Lesson Overview
0:15
Sometimes The Characteristic Equation Has Complex Roots
1:12
Example 1
3:21
Example 2
7:42
Example 3
15:25
Example 4
18:59
Example 5
27:52
Repeated Roots & Reduction of Order

43m 2s

Intro
0:00
Lesson Overview
0:23
If the Characteristic Equation Has a Double Root
1:46
Reduction of Order
3:10
Example 1
7:23
Example 2
9:20
Example 3
14:12
Example 4
31:49
Example 5
33:21
Undetermined Coefficients of Inhomogeneous Equations

50m 1s

Intro
0:00
Lesson Overview
0:11
Inhomogeneous Equation Means the Right Hand Side is Not 0 Anymore
0:21
First Solve the Homogeneous Equation
1:04
Find a Particular Solution to the Inhomogeneous Equation Using Undetermined Coefficients
2:03
g(t) vs. Guess for ypar
2:42
If Any Term of Your Guess for ypar Looks Like Any Term of yhom
5:07
Example 1
7:54
Example 2
15:25
Example 3
23:45
Example 4
33:35
Example 5
42:57
Inhomogeneous Equations: Variation of Parameters

49m 22s

Intro
0:00
Lesson Overview
0:31
Inhomogeneous vs. Homogeneous
0:47
First Solve the Homogeneous Equation
1:17
Notice There is No Coefficient in Front of y''
1:27
Find a Particular Solution to the Inhomogeneous Equation Using Variation of Parameters
2:32
How to Solve
4:33
Hint on Solving the System
5:23
Example 1
7:27
Example 2
17:46
Example 3
23:14
Example 4
31:49
Example 5
36:00
Section 3: Series Solutions
Review of Power Series

57m 38s

Intro
0:00
Lesson Overview
0:36
Taylor Series Expansion
0:37
Maclaurin Series
2:36
Common Maclaurin Series to Remember From Calculus
3:35
7:58
Ratio Test
12:05
Example 1
15:18
Example 2
20:02
Example 3
27:32
Example 4
39:33
Example 5
45:42
Series Solutions Near an Ordinary Point

1h 20m 28s

Intro
0:00
Lesson Overview
0:49
Guess a Power Series Solution and Calculate Its Derivatives, Example 1
1:03
Guess a Power Series Solution and Calculate Its Derivatives, Example 2
3:14
Combine the Series
5:00
Match Exponents on x By Shifting Indices
5:11
Match Starting Indices By Pulling Out Initial Terms
5:51
Find a Recurrence Relation on the Coefficients
7:09
Example 1
7:46
Example 2
19:10
Example 3
29:57
Example 4
41:46
Example 5
57:23
Example 6
1:09:12
Euler Equations

24m 42s

Intro
0:00
Lesson Overview
0:11
Euler Equation
0:15
Real, Distinct Roots
2:22
Real, Repeated Roots
2:37
Complex Roots
2:49
Example 1
3:51
Example 2
6:20
Example 3
8:27
Example 4
13:04
Example 5
15:31
Example 6
18:31
Series Solutions

1h 26m 17s

Intro
0:00
Lesson Overview
0:13
Singular Point
1:17
Definition: Pole of Order n
1:58
Pole Of Order n
2:04
Regular Singular Point
3:25
Solving Around Regular Singular Points
7:08
Indical Equation
7:30
If the Difference Between the Roots is An Integer
8:06
If the Difference Between the Roots is Not An Integer
8:29
Example 1
8:47
Example 2
14:57
Example 3
25:40
Example 4
47:23
Example 5
1:09:01
Section 4: Laplace Transform
Laplace Transforms

41m 52s

Intro
0:00
Lesson Overview
0:09
Laplace Transform of a Function f(t)
0:18
Laplace Transform is Linear
1:04
Example 1
1:43
Example 2
18:30
Example 3
22:06
Example 4
28:27
Example 5
33:54
Inverse Laplace Transforms

47m 5s

Intro
0:00
Lesson Overview
0:09
Laplace Transform L{f}
0:13
Run Partial Fractions
0:24
Common Laplace Transforms
1:20
Example 1
3:24
Example 2
9:55
Example 3
14:49
Example 4
22:03
Example 5
33:51
Laplace Transform Initial Value Problems

45m 15s

Intro
0:00
Lesson Overview
0:12
0:14
Take the Laplace Transform of Both Sides of the Differential Equation
0:37
Plug in the Identities
1:20
Take the Inverse Laplace Transform to Find y
2:40
Example 1
4:15
Example 2
11:30
Example 3
17:59
Example 4
24:51
Example 5
36:05
Section 5: Review of Linear Algebra
Review of Linear Algebra

57m 30s

Intro
0:00
Lesson Overview
0:41
Matrix
0:54
Determinants
4:45
3x3 Determinants
5:08
Eigenvalues and Eigenvectors
7:01
Eigenvector
7:48
Eigenvalue
7:54
Lesson Overview
8:17
Characteristic Polynomial
8:47
Find Corresponding Eigenvector
9:03
Example 1
10:19
Example 2
16:49
Example 3
20:52
Example 4
25:34
Example 5
35:05
Section 6: Systems of Equations
Distinct Real Eigenvalues

59m 26s

Intro
0:00
Lesson Overview
1:11
How to Solve Systems
2:48
Find the Eigenvalues and Their Corresponding Eigenvectors
2:50
General Solution
4:30
Use Initial Conditions to Find c1 and c2
4:57
Graphing the Solutions
5:20
Solution Trajectories Tend Towards 0 or ∞ Depending on Whether r1 or r2 are Positive or Negative
6:35
Solution Trajectories Tend Towards the Axis Spanned by the Eigenvector Corresponding to the Larger Eigenvalue
7:27
Example 1
9:05
Example 2
21:06
Example 3
26:38
Example 4
36:40
Example 5
43:26
Example 6
51:33
Complex Eigenvalues

1h 3m 54s

Intro
0:00
Lesson Overview
0:47
Recall That to Solve the System of Linear Differential Equations, We find the Eigenvalues and Eigenvectors
0:52
If the Eigenvalues are Complex, Then They Will Occur in Conjugate Pairs
1:13
Expanding Complex Solutions
2:55
Euler's Formula
2:56
Multiply This Into the Eigenvector, and Separate Into Real and Imaginary Parts
1:18
Graphing Solutions From Complex Eigenvalues
5:34
Example 1
9:03
Example 2
20:48
Example 3
28:34
Example 4
41:28
Example 5
51:21
Repeated Eigenvalues

45m 17s

Intro
0:00
Lesson Overview
0:44
If the Characteristic Equation Has a Repeated Root, Then We First Find the Corresponding Eigenvector
1:14
Find the Generalized Eigenvector
1:25
Solutions from Repeated Eigenvalues
2:22
Form the Two Principal Solutions and the Two General Solution
2:23
Use Initial Conditions to Solve for c1 and c2
3:41
Graphing the Solutions
3:53
Example 1
8:10
Example 2
16:24
Example 3
23:25
Example 4
31:04
Example 5
38:17
Section 7: Inhomogeneous Systems
Undetermined Coefficients for Inhomogeneous Systems

43m 37s

Intro
0:00
Lesson Overview
0:35
First Solve the Corresponding Homogeneous System x'=Ax
0:37
Solving the Inhomogeneous System
2:32
Look for a Single Particular Solution xpar to the Inhomogeneous System
2:36
Plug the Guess Into the System and Solve for the Coefficients
3:27
Add the Homogeneous Solution and the Particular Solution to Get the General Solution
3:52
Example 1
4:49
Example 2
9:30
Example 3
15:54
Example 4
20:39
Example 5
29:43
Example 6
37:41
Variation of Parameters for Inhomogeneous Systems

1h 8m 12s

Intro
0:00
Lesson Overview
0:37
Find Two Solutions to the Homogeneous System
2:04
Look for a Single Particular Solution xpar to the inhomogeneous system as follows
2:59
Solutions by Variation of Parameters
3:35
General Solution and Matrix Inversion
6:35
General Solution
6:41
Hint for Finding Ψ-1
6:58
Example 1
8:13
Example 2
16:23
Example 3
32:23
Example 4
37:34
Example 5
49:00
Section 8: Numerical Techniques
Euler's Method

45m 30s

Intro
0:00
Lesson Overview
0:32
Euler's Method is a Way to Find Numerical Approximations for Initial Value Problems That We Cannot Solve Analytically
0:34
Based on Drawing Lines Along Slopes in a Direction Field
1:18
Formulas for Euler's Method
1:57
Example 1
4:47
Example 2
14:45
Example 3
24:03
Example 4
33:01
Example 5
37:55
Runge-Kutta & The Improved Euler Method

41m 4s

Intro
0:00
Lesson Overview
0:43
Runge-Kutta is Know as the Improved Euler Method
0:46
More Sophisticated Than Euler's Method
1:09
It is the Fundamental Algorithm Used in Most Professional Software to Solve Differential Equations
1:16
Order 2 Runge-Kutta Algorithm
1:45
Runge-Kutta Order 2 Algorithm
2:09
Example 1
4:57
Example 2
10:57
Example 3
19:45
Example 4
24:35
Example 5
31:39
Section 9: Partial Differential Equations
Review of Partial Derivatives

38m 22s

Intro
0:00
Lesson Overview
1:04
Partial Derivative of u with respect to x
1:37
Geometrically, ux Represents the Slope As You Walk in the x-direction on the Surface
2:47
Computing Partial Derivatives
3:46
Algebraically, to Find ux You Treat The Other Variable t as a Constant and Take the Derivative with Respect to x
3:49
Second Partial Derivatives
4:16
Clairaut's Theorem Says that the Two 'Mixed Partials' Are Always Equal
5:21
Example 1
5:34
Example 2
7:40
Example 3
11:17
Example 4
14:23
Example 5
31:55
The Heat Equation

44m 40s

Intro
0:00
Lesson Overview
0:28
Partial Differential Equation
0:33
Most Common Ones
1:17
Boundary Value Problem
1:41
Common Partial Differential Equations
3:41
Heat Equation
4:04
Wave Equation
5:44
Laplace's Equation
7:50
Example 1
8:35
Example 2
14:21
Example 3
21:04
Example 4
25:54
Example 5
35:12
Separation of Variables

57m 44s

Intro
0:00
Lesson Overview
0:26
Separation of Variables is a Technique for Solving Some Partial Differential Equations
0:29
Separation of Variables
2:35
Try to Separate the Variables
2:38
If You Can, Then Both Sides Must Be Constant
2:52
Reorganize These Intro Two Ordinary Differential Equations
3:05
Example 1
4:41
Example 2
11:06
Example 3
18:30
Example 4
25:49
Example 5
32:53
Fourier Series

1h 24m 33s

Intro
0:00
Lesson Overview
0:38
Fourier Series
0:42
Find the Fourier Coefficients by the Formulas
2:05
Notes on Fourier Series
3:34
Formula Simplifies
3:35
Function Must be Periodic
4:23
Even and Odd Functions
5:37
Definition
5:45
Examples
6:03
Even and Odd Functions and Fourier Series
9:47
If f is Even
9:52
If f is Odd
11:29
Extending Functions
12:46
If We Want a Cosine Series
14:13
If We Wants a Sine Series
15:20
Example 1
17:39
Example 2
43:23
Example 3
51:14
Example 4
1:01:52
Example 5
1:11:53
Solution of the Heat Equation

47m 41s

Intro
0:00
Lesson Overview
0:22
Solving the Heat Equation
1:03
Procedure for the Heat Equation
3:29
Extend So That its Fourier Series Will Have Only Sines
3:57
Find the Fourier Series for f(x)
4:19
Example 1
5:21
Example 2
8:08
Example 3
17:42
Example 4
25:13
Example 5
28:53
Example 6
42:22

• ## Related Books

 3 answersLast reply by: Dr. William MurraySun Jan 18, 2015 10:32 AMPost by John Panagiotopoulos on June 21, 2013how did you get that equation y=ce^rt.....Do you have a proof you could put up please? 1 answerLast reply by: Dr. William MurraySun Apr 14, 2013 5:58 PMPost by Nicholas Wilkins on April 9, 2013I believe you left out the 'describe the behavior of the solution as t approaches infinity.' (in the second example)

### Distinct Roots of Second Order Equations

Distinct Roots of Second Order Equations (PDF)

### Distinct Roots of Second Order Equations

Lecture Slides are screen-captured images of important points in the lecture. Students can download and print out these lecture slide images to do practice problems as well as take notes while watching the lecture.

• Intro 0:00
• Lesson Overview 0:36
• Linear Means
• Second-Order
• Homogeneous
• Constant Coefficient
• Solve the Characteristic Equation
• Roots r1 and r2
• To Find c1 and c2, Use Initial Conditions
• Example 1 5:46
• Example 2 8:20
• Example 3 16:20
• Example 4 18:26
• Example 5 23:52

### Transcription: Distinct Roots of Second Order Equations

Hello and welcome back to www.educator.com, I'm Will Murray and we are studying differential equations, today we are going to study second order equations and there are several different cases that arise when you study second order equations.0000

We are going to study something called the characteristic equation which will have 2 roots and there are different things that can happen if those 2 roots are distinct if it is different from each other or if they are the same.0014

Or they turn out to be complex numbers, we are going to have one lecture on each one, today we are going to talk about the case of distinct roots, let us jump right in there.0027

We are going to solve a second order linear homogeneous constant coefficient differential equations, that is a quite a mouthful there, let me explain what each one of those words means.0037

Linear means you have this form Ay″ + By′ + Cy, that is where the linear differential equation is contrast of that would be if you had something like y x y′ would be a non-linear differential equations.0051

Right now we are just studying linear differential equations, second order means that you have y″ appearing, that is what the second order refers to is that you have not just y′ but y″.0070

That is what that word means, homogeneous means that the right hand side is 0, the fact that we have a 0 over here makes it a homogeneous equation, later on we are going to study inhomogeneous equations where we have other functions on the right hand side.0089

We will learn how to solve them when we do not have 0 on the right hand side but that is more complicated issue, we are not going to get to that today.0107

And then constant coefficient means that the a, b, and c are constants, they are just numbers there, that is what constant coefficient means, that is what all those words mean.0116

Linear means Ay″ + By′ + Cy, second order means you have y″ in there, homogeneous means the right hand side is 0 and constant coefficient means the a, b, and c are constants they are not functions of x or t or any other variable.0134

Let us learn how to solve those, it is actually a pretty straight forward algorithm to solve those, what you have to do is to solve this thing called the characteristic equation.0152

And that is basically translating the differential equation and writing this other equation in terms of R, our variables are going to be R and we are going to solve this quadratic equation AR^2 + BR + C = 0.0164

Remember A, B, and C are constants, this is just a quadratic equation, you can solve it using the quadratic formula or completing the square or if you are lucky you can factor it.0184

Whatever techniques you have learned from algebra you can use to solve this quadratic equation.0196

This is really just an algebra problem to solve the quadratic equation, of course as you remember when you solve quadratic equation and algebra you get 2 roots, r1 and r2, and today we are talking about the case where the roots are distinct.0203

Sometimes you have multiple roots or sometimes you have complex roots but we are going to put those off for another lectures, today we are talking about 2 distinct real roots.0231

And then the general solution to the differential equation is C1 e^r1(T) + C2 e^r2(T), basically all of this is prefab except for you put the r1 and r2 in as exponents on the e terms.0241

That is the general solution to the differential equation, it has 2 constants in it, the reason it has 2 constants is because it was a second order equation.0266

The general solution to a first order equation always has one arbitrary constant in it and the general solution to a second order equation always has 2 arbitrary constants.0278

And to find those arbitrary constants it is just like with a first order equations you use initial conditions, before we had one initial condition for a second order equation you need 2 initial conditions.0290

They are usually given in the form of y and 0 equals a certain number and y′ of 0 is equals to a certain number, what you will do is you take those initial conditions, plug goes back into the general solution and you get 2 equations and 2 unknowns.0302

Each initial condition gives you one equation and the 2 unknowns that I'm talking about here are C1 and C2, you get 2 equations for C1 and C2, and then you will solve those to figure out what C1 and C2 are.0320

Then you will plug goes back into the general solution and get a specific solution, that is the way it works, it will make more sense after we work out some examples, let us go ahead and try one out.0336

We are asked to find the general solution to the differential equation y″ of T +2y′ of T -8 y of T is equal 0, this is a second order linear homogeneous constant coefficient differential equation.0345

And remember the way we solve these things is we write down the characteristic equation which is AR^2 + BR + C is equal to 0 and A, B, and, C are just the coefficients from the differential equation.0363

In this case the A is one, the B is 2 and the C is -8, remember to keep track of that negative sign, that is a part of the coefficient, we got r^2 + 2r -8 is equal to 0 and that is just a quadratic.0380

You can solve using quadratic formula if you like, this one as is actually a pretty easy one, we can factor this one, I can factor this into r + 4 x r - 2 is equal 0 and that means my roots are r=-4 or 2.0402

Now I can write down my general solution here, the general solution and I'm following the format the we had at the beginning of the lesson, C1 e^-4t, putting the roots up in the exponents + C2 e^2t.0428

I do not have any initial conditions for this one, I'm just going to stop here with the general solution I can not find what the values of the constants are unless I have initial conditions.0451

I'm done with the general solution, just to recap what we did there, we took the differential equation, we wrote down the characteristic equation, filled in the constants, factored it, solve for values of r.0466

And in those values of r became the exponents in the general solution and we did E to each one of those values of r x TE and then we multiply each one by an arbitrary constant.0480

We got our general solution, we cannot figure out what the values of the constants are unless we have initial conditions, in our next example we have to solve the initial value problem y″ +2y′ -8 y =0.0492

And y(0)=1 and y′ of 0 is equal to 10, this is actually the same differential equation that we had in the previous problem, I'm going to go ahead and write down the general solution that we had from the previous problem.0511

Because that much of the problem is the same, y general is equal to c1e^-4T + C2e^2t, that I came from the previous problem, if you do not remember how we derive that just check back in example 1 and you will see where that comes from.0528

That was the solution to the differential equation, we solve that now we have to use the initial conditions to figure out what the values of the constants are, what we are going to do is look at that first initial condition.0550

We are going to plug in T equal 0 and y equals one, I will say one is equal to c1 E^ -4 x 0 + C2 e^2 x 0 and ofcourse e^0 is just one, that tells me that one is C1 + C2 , that is one equation in my unknown C1 and C2.0565

To get a second equation I'm going to use this other initial condition y′ of 0 is equal to 10, in order to use that, I got to find the derivative of y, I'm going t go back to the general solution and I'm going to find y′ is equal to.0593

Now C1 x is derivative of e^-4T, that -4 will pop out, I get -4 C1e^-4T, this is the derivative I'm finding now, +2 C2e^2t and then I will plug in n, again T is equal to 0 and y′ is equal to 10.0611

I will plug-in 10 for y′ and I will plug in 0 for T, which will give me -4C1 e^0 is just 1, +2 x C2 and the e^0 is just one again.0638

What I have here is one equation and another equation, 2 equations and 2 unknowns to solve for C1 and C2 and there is a lot of different ways you can solve 2 equations and 2 unknowns.0655

You probably learned several different ways in algebra class, you can use substitution, you can use linear combinations, you can use addition and subtraction, you can use matrices.0670

There is a lot of different ways to solve this, if you do not remember how do this, you might want to check back at the www.educator.com lectures on algebra.0681

The way I'm going to do it is use linear combination, I think I'm going to multiply this equation both sides by 4, the reason I'm doing that is I'm going to add it to this equation and I want those 4's to cancel.0689

If I multiply this equation by 4, I will get 4 is equal to 4C1 + 4C2 and then I will write the other equation over here 10 is equal to -4C1 + 2C2 and I'm going to add those equations together and the point of doing that is that I will get 14 on the left is equal to 0C1 + 6C2.0705

Now I'm going to solve for C2, I get C2 is equal to 14/6 which I can simplify down into 7/3 and now I plug that back into the first equation and try to figure out what C1 is.0758

I got one is equal to C1 + C2 and that is equal to c1 + 7/3 is one, I will subtract 7/3 from both sides and I will C1 is equal to 1 is 3/3, that is -4/3, now I figured out my values of C1 and C2 I will plug those back into the general solution.0779

This is the specific solution which satisfies the initial conditions y=-4/3 e^-4T + 7/3 e^2T, that is my specific solution that is supposed to satisfy both initial conditions.0815

Let me just recap what we did there, we started with the general solution and we got that from example 1, that is where that came from we did not actually solve that here, but if you check back in example 1, you will see where that general solution came from.0846

And then we tried to make it fit the 2 initial conditions, we looked at the initial conditions y(0) equal one, we plug y(0) in, we plug T= 0 and and we got e^0 on both sides we just got C1 + C2=1.0865

That is where we got one equation for C1 and C2 and then we took the derivative of the original equation, we got Y′ =-4 C1 x e^-4T and 2C2 x ei^2T and we plug in 0 there because we are looking at y′ of 0 is equal to 10.0887

We got 10 is equal to 4C1 + 2C2 and that gave us a second equation in C1 and C2, we got 2 linear equations and C1 and C2, there are lots of different ways you can solve these.0916

Any of them should work, if you have another way of solving 2 equations and 2 unknowns, it is okay if you use a different way but the way I used was to multiply the first equation by 4 and then add it to the second equation.0932

The point was that it made the C1 term go away and we got 6 C2 is equal to 14 , C2 is equal to 14(6) or 7/3 and then we plug back in for C2 into the first equation and we got C1 is equal to -4/3 and then we plugged C1 and C2 back into the general solution.0946

And we got our specific solution that satisfies both initial conditions, for our next example we have to find the general solution of y″ -4 y′ -5 y is equal to 0.0975

Again this is a linear homogeneous constant coefficients second-order differential equation, we are going to use the method of the characteristic equation to solve it, I'm going to write down the characteristic equation.0990

It is just the same equation as the differential equation except you use R instead of y and you translated into a polynomial, we have r ^2 from the y″ - 4 r -5 = 0.1003

And now we want to solve this to find the roots of this quadratic equation, you can use the quadratic formula, I'm going to factory it because it turns out that this one factors nicely.1021

We get r -5 x r + 1 is equal 0, my r is equal to 5 or-1 and what you do with those roots is you put them in the exponents and you multiply them by T, my general solution is y is equal to C1 e^-1t, I will just put e^-t + C2 e^5T.1032

By the way it does not matter which order you put them in, you can switch the order and have it C1 e^5T or C2 Ee^T, works just as well.1067

What we found here is the general solution to that second-order differential equation and we do not have any initial conditions on this, we are going to stop to the general solution, we do not have a way to find the values of the constant C1 and C2.1082

That is going to come in the next example, let us go ahead and take a look at that.1102

In example 4, we have to solve the initial value problem, it is the same differential equation as before y″ -4 y′ -5 y is equal to 0, but now we had 2 initial conditions, y(0)=4 and y′(0)=2.1109

Remember in the previous example we found the general solution to the differential equation y(gen) is equal to C1 e^-T + C2 e^5T and what we are going to doing with that is plug in our initial conditions.1128

This says when T is equal 0, y is equal 4, I will say 4 is equal to C1 x e^ -0+ C2 e^5 x 0, that is equal to C1 + C2 because e^0 is just 1 and then y′ of 0, to use that we have to take the derivative of our general solution.1152

y′ is negative C1 e^-T +5 C2 e^5T and again I will plug in T equal 0 and I will plug in 2 for y′, 2 is equal to -C1 e^-0 + 5 C2 E^5 x 0, that is -C1 +5 C2 because e^0 just 1 is equal to 2.1182

I have 2 equations and 2 unknowns and again there are several different ways you can solve this, you could do a substitution, solve for 1 variable and 1 equation and substitute it to the other equation.1226

You could use matrices, you can use linear combinations, what I'm going to do is take these 2 equations and I will just add 1 to the other one because I see that if I do that, the C1's will cancel each other out and I will get 6 C2.1239

I'm adding these 2 equations here, 6C2 is equal to 6 and there is no C1's because those cancel each other out, I will get C2 is equal to 1 and then if I plug that back in here to C1 + C2 is equal 4, I will get C1 is equal to 3.1258

Now I got my values of C1 and C2, I will plug goes back into my general solution and get the specific solution as C1 was 3, I get 3 e^-T + C2 is 1, just + e^5T.1280

That is my specific solution which satisfies both the differential equation and the 2 initial conditions, just to recap there we got our general solution that was from the previous example, example 3.1300

If you do not remember how we derive that, just check back in example 3 and you will see where that came from and then we plug in our 2 initial conditions, we plug our first one in and plug in T=0 and y=4.1319

We plug in 0 for T and 4 y and that reduce down to C1 + C2=4, for the second initial condition we had to figure out the derivative, we took the derivative of the general solution and we got -C1 e^-T + 5C2 e^5T.1332

And then we plug in 2 for y′ and we got 2 is equal to what we get plugging in 0, again that turn into -C1 +5C2=2, each one of those initial conditions gave us an equation and 2 unknowns.1355

Our unknowns now are C1 and C2, once we got those 2 equations and 2 unknowns, it turns into an algebra problem of solving for C1 and C2 and this one I was able to solve by adding the 2 equations.1373

I got 6c2=6, C2 is equal to 1 then I substituted back to get C1 is equal to 3, if you do not like the way I did that by adding the equations, you can also solve for one variable and substitute it into the other equation.1387

You can use matrices and determinants, there are lots of different ways to do and that just depends on what you are most comfortable with from your algebra class.1403

Once you figure out the C1 and C2, we plug those into the general solution up here and here and we get our specific solution y=3 e^-T + e^5T, that is our specific solution to the differential equation and both initial conditions.1410

Our last example here, we have to find at least one non zero solution to the differential equation y″ + 6y′ + 9y is equal to 0.1433

Just like all the others, we start out with the characteristic equation, that means we convert the y into r and the derivatives into exponents, r^2 + 6r +9 = 0.1445

That actually factors as a perfect square, that is r +3 ^2 is equal to 0, we get a double root, r=-3 and then our other root is also -3, we really only get one root from that, we had a solution here y is C1 e^-3 T.1463

We can not find a second solution because our other root is also -3, let me write that down.1491

But we can not find a second solution that is independent of our first solution that was e^-3T, left a little space here after the word "can't" because this is actually the subject of a later lectures, I'm going to say we can't, I will put that in red.1504

We can't yet find a second solution because a couple lectures later we will figure out what to do with repeated roots but in the meantime we do not know how to solve that.1546

I will say a common student mistake would be to write the general solution as well if you just can not blindly look at these 2 roots, you would say C1 e^-3T + C2 e^-3T because you just copy your 2 roots into the exponents here.1560

If you wrote that, that would be incorrect, that is not the general solution and the reason is because you really have 2 copies of the same solution there, you need to find a second independent solution.1597

We have not learned how to do that yet, in the meantime all we can offer as a solution is just the C1 e^ -3 T, there is another way to solve these equations with repeated root and we will learn how to do that, learn how to solve this in a later lecture.1607

You have to peek at a couple more lectures down the line and you will see one called repeated roots.1642

And that one we will learn how to find a second independent solution to an equation when we do have repeated roots, just to recap here, we started out with a characteristic equation where we converted it into a polynomial in r with exponents instead of derivatives.1661

We factored it down just like the others, we found the roots and then the new wrinkle in this example was that both the roots were the same, we were able to form one solution, C1 e^-3T but we can not find a second independent solution.1679

So we cannot tack on a C2 e^-3T because that would just be a copy of the first solution, in order to find the second solution we will have to come back and study this in more detail on our later lecture on repeated roots.1696

That is the end of our lecture on distinct roots, we will come back later and start talking about complex roots and repeated roots, these are the lectures on differential equations, my name is Will Murray and you are watching www.educator.com, thanks.1711

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