Theory of Linear Equations
II.1 Theory of Linear Equations
1. Introduction to Linear Differential Equations
This lecture extends the understanding of differential equations, specifically focusing on linear differential equations with initial conditions.
2. Initial Value Problem (IVP)
Definition:
An nth order linear initial value problem can be expressed as:
With initial conditions:
$y(x0) = y0$
$y'(x0) = y1$
…
$y^{(n-1)}(x0) = y{n-1}$
Where I is an open interval such that $x_0 \in I$.
Functions $an(x), a{n-1}(x), …, a_0(x), g(x)$ are continuous on I.
2.1 Existence and Uniqueness of Solutions
The problem has a unique solution on interval I that satisfies the corresponding initial conditions.
Uniqueness is guaranteed under the following conditions:
The functions involved are continuous.
The equality holds.
The initial conditions are specified at one point.
2.2 Example 1
Example Problem:
Initial Conditions:
$y(1) = 0$, $y'(1) = 0$, $y''(1) = 0$
This represents a third-order linear initial value problem. Unique solution: $y = 0$ (the only solution).
2.3 Example 2
Example Problem:
Initial Conditions:
$y(0) = 0$, $y'(0) = 1$
Here this is a second-order linear IVP with all functions continuous on some interval containing $x_0 = 0$. There is a unique solution.
3. Boundary Value Problems (BVP)
Definition:
A common type of problem where the values of $y$ and its derivatives are specified at different points, rather than at a single point.
General formulation:
With conditions defined at boundary points $x = a$ and $x = b$.
3.1 Example of BVP
Example Problem:
General formulation of a classic BVP:
Conditions specified at points other than just one:
This means we have specified not just $y(a)$ but also $y'(b)$ and potentially other values.
BVP can result in:
No solution
One solution
Infinitely many solutions depending on the specific equations and conditions.
3.2 Example of Periodic Boundary Conditions
Example Boundary Problem: Consider $y'' + 16y = 0$
If we take conditions such as:
$y(0) = 0$
$y( rac{
ho}{2}) = 0$
Leads to infinitely many solutions due to conditions in the periodic boundary setup.
4. Homogeneous Differential Equations and Superposition
4.1 Definition
A linear differential equation of the form:
Called homogeneous if $g(t) = 0$, and non-homogeneous if $g(t) \neq 0$.
4.2 Previous Unit Recap
Previously studied linear, inhomogeneous problems can be represented generally as:
General solution can be written as:
Where $y_h(t)$ is the complementary solution to the associated homogeneous equation.
4.3 Associated Homogeneous Problem
Dividing the expression by $a_n(t)$ gives the associated homogeneous problem:
Results in a solution set.
4.4 Property of Homogeneous Codes
If $y1(t)$ and $y2(t)$ are solutions to the homogeneous equation, so is:
This applies to any linear combination of solutions, showcasing linearity and superposition.
5. Linearly Independent Functions
Definition:
Functions $f1(t), f2(t), …, fk(t)$ are linearly independent if the only solution to the equation:
Is $C1 = C2 = … = C_k = 0$.
Conversely, if nontrivial linear combinations exist, the functions are linearly dependent.
5.1 Example of Linear Independence
Example:
Consider functions:
$f_1(t) = 3 ext{cos}(t) + 5x^2$
$f_2(t) = 5x^2 + 3x$
These are dependent as they result in nontrivial solutions.
6. Wronskian Determinant
To check linear independence, use the Wronskian determinant defined as follows:
If $f1, f2, ext{…}, f_k$ are functions, prepare the Wronskian:
$$ W(f1, f2, …, fk)(x) = egin{vmatrix} f1 & f2 & … & fk \ f'1 & f'2 & … & f'k \ … & f^{(k-1)}1 & f^{(k-1)}2 & … & f^{(k-1)}k \ ext{…} \ ext{…}egin{vmatrix} ext{determinant here} ext{determinant section} \ ext{…}\