Linear Differential Equations#
Linear ODEs#
Definition. An ODE is linear if it is of the form \(\mathcal{L}_x[u] = f\), where \(\mathcal{L}_x\) is the linear differential operator
Linear ODEs of the form \(\mathcal{L}[u] = 0\) are termed homogeneous, otherwise inhomogeneous.
We will often want to work with the linear operator in standard form, meaning that the factor multiplying the highest derivative is \(1\):
Solutions#
Solutions of a homogeneous ODE satisfy the superposition principle (or linearity principle): if \(u_1\) and \(u_2\) are solutions of a linear ODE \(\mathcal{L}[u] = 0\) then any linear combination \(\alpha u_1 + \beta u_2\) is also a solution:
A general solution of an ODE is a solution \(u = \alpha u_1 + \beta u_2\) where \(u_1\) and \(u_2\) are linearly independent and they are called a basis of the set of solutions. A particular solution is obtained by assigning specific values to constants.
Every element of the general solution of an ODE is a function of the form \(u = u_p + u_h\), where \(u_h\) is an element of the general solution of the homogeneous ODE and \(u_p\) is a particular integral, the solution of the inhomogeneous problem:
Solution methods#
Separation of variables when we can algebraically transform the equation to the form \( f(u) du = g(x) dx \) which we can integrate directly
Variation of parameters where we find the solution to the homogeneous problem and use it as solution ansatz for a particular solution by allowing constants to become new unknown functions which we then seek
Undetermined coefficients
Green’s functions
Numerical methods