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6.27 Homogeneous and inhomogeneous equation

The solution in the previous slide consists of two parts: the first term is g⁢(x)⁢ek⁢xg(x)e^{kx} where g⁢(x)g(x) is a particular integral of q⁢(x)⁢e-k⁢xq(x)e^{-kx}; the second term is c⁢ek⁢xce^{kx}, where cc is an arbitrary constant. Note that the second term is just the general solution to the equation d⁢yd⁢x-k⁢y=0\frac{dy}{dx}-ky=0!

Definition.

The linear differential equation d⁢yd⁢x+p⁢(x)⁢y=q⁢(x)\frac{dy}{dx}+p(x)y=q(x) is homogeneous if q⁢(x)=0q(x)=0 and inhomogeneous otherwise.

For an arbitrary first-order linear differential equation d⁢yd⁢x+p⁢(x)⁢y=q⁢(x)\frac{dy}{dx}+p(x)y=q(x), we say that the corresponding homogeneous equation is d⁢yd⁢x+p⁢(x)⁢y=0\frac{dy}{dx}+p(x)y=0.

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.