Order - order of the highest derivative
of the dependent variable with respect
to the independent variable
Linear - only if the unknown function and its derivatives
appear to the power 1 Non-linear - otherwise
Homogeneous - If f(x) is a solution, so is cf(x), where c is an arbitrary
(non-zero) constant. Note that in order for this condition to hold, each term in
a linear differential equation of the dependent variable y must contain y or
any derivative of y. Simply said, the are no constant terms in the equation.
They are usually recognized because the RHS is 0
Degree - the power to which one of the derivatives is raised
First Order Linear ODEs
Example: a falling object subject to linear
air resistance
Solution Method
1) Multiply through by integrating factor
"IF", which can be always found
2)Recall the formula for calculating the
integrating factor : IF = e^(int f(x)dx )
NOTE
Some non-linear equations can be
transformed into linear ones by change of
variable
y' + f(x)y = g(x)
2nd and higher order - Linear ODEs
with constant coefficients
Solution Method
The general solution is the sum of the complementary function and the
particular integral. i.e. GS = CF + PI
Complementary function
General solution to the corresponding
homogeneous equation
Particular Integral
Any solution of the
inhomogeneous equation
Educated Guess
The trial solutions used to find the PI are usually of the
same form of the Complementary Function: most
commonly constants, polynomials, sine/cosine and
exponentials
The Wronskian
If the wronskian of n functions f1(x),
f2(x) ... fn(x) is zero, then the functions
are linearly indipendent
The wronskian is the determinant of the matrix which has f1(x), f2(x) ...
fn(x) has elements of the first row, the first derivative of the functions in the
second raw, the second derivative in the third raw and so on up to the
(n-1)th derivative of the functions in the last raw
Series Solutions of ODEs
We can use a power series solution if the function is analytic at
that point - i.e. if the function is locally given by a convergent
power series
Method
Write each term as a power series
in terms of the independent variable
Find the recurrence relation between the
coefficients equating the sum of the power series to
zero
Legendre's Equation
Equation which is often met when solving PDEs (particularly ones which
involve the Laplacian) in spherical polar coordinates when seeking a
separable solution of form u(r,θ,φ) = R(r)T(θ)F(φ)
Can be solved with
the "series solution"
technique
Power series only converge if k, which is the
coefficient of y in the equation, is equal to
L(L+1), where L = 0,1,2,3 and so k = 0,2,6,12
Legendre polynomials
The solutions are Legendre
polynomials, which are defined
recursively - important for Quantum
Mechanics
The equation has regular singular points at x = ±1 so, in general, a
series solution about the origin will only converge for |x| < 1.
Frobenius Method
(Generalised power
series)
Technique to find an infinite series solution for a second-order ordinary
differential equation of the form z^2u''+p(z)zu'+q(z)u=0
p(z) and q(z) have to be analytic at 0
Use y = sum Cn(x-x0)^(r+n) to find ...
... Indicial Equation
recurrence equation
The general solution
will be y = A_pJ_p
+A_-pJ_-p
Jp is Bessel's function of first kind
four classes of solutions
Three important linear PDEs
Laplace's equation (see
Legendre's equation and
separation of variables)
Wave equation
Diffusion equation
Solution of PDEs by separation of variables
Define boundary and initial conditions
Use separation of variable to reduce to ODE eigenvalue problem.
For example, to solve Laplace's equation in 2 dimensions, use the
trial solution T(x,y) = X(x)Y(y) and generate two couples ODEs:
X"=SX and Y"=SY
Use homogeneous boundary conditions to find eigenvectors and eigenfunctions
Apply initial conditions and other boundary conditions