The solution in the previous slide consists of two parts: the first term is where is a particular integral of ; the second term is , where is an arbitrary constant. Note that the second term is just the general solution to the equation !
The linear differential equation is homogeneous if and inhomogeneous otherwise.
For an arbitrary first-order linear differential equation , we say that the corresponding homogeneous equation is .
The general solution to the equation can always be written as the sum of a particular integral (PI) and the complementary function (CF), which is the general solution to the corresponding homogeneous equation.