Differential equations MOC

Solving non-homogenous second order ODEs

For any second-order ODE

𝐿[𝑦]=𝑦″+𝑝(𝑑)𝑦′+π‘ž(𝑑)𝑦=𝑔(𝑑)

it is clear that the difference of any two solutions solves the related homogenous ODE. Namely, given 𝐿[π‘Œ1] =𝑔(𝑑) and 𝐿[π‘Œ2] =𝑔(𝑑), it is clear that

𝐿[π‘Œ1βˆ’π‘Œ2]=𝐿[π‘Œ1]βˆ’πΏ[π‘Œ2]=𝑔(𝑑)βˆ’π‘”(𝑑)=0

It follows that given the general solution to the related homogenous ODE 𝑦𝑐(𝑑), called the complimentary solution, and any one particular solution to the full ODE 𝑦𝑝, then

𝑦=𝑦𝑐+𝑦𝑝=𝑐1𝑦1+𝑐2𝑦2+𝑦𝑝

since

𝐿[𝑦𝑐+𝑦𝑝]=𝐿[𝑦𝑐]+𝐿[𝑦𝑝]=𝑔(𝑑)

Finding a particular solution

In practice, a variety of methods may be used to find a particular solution once 𝑦𝑐 has been found


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