By the separation of variables technique we write u(x,y)=χ(x)ϕ(y) therefore we can rewrite or equation as follows :
χ′(x)ϕ(y)+χ(x)ϕ′(y)=2(x+y)χ(x)ϕ(y)
Now we will divide both parts by u(x,y)=χ(x)ϕ(y) and transfer all functions of a variable x to the left, and these of y to the right:
χ(x)χ′(x)+ϕ(y)ϕ′(y)=2(x+y)
χ(x)χ′(x)−2x=2y−ϕ(y)ϕ′(y)
On the left we have a function of x only and on the right of y only. Therefore both parts of this equality must be a constant (as x,y are independent) that we will call λ . Now let's solve the equations for ϕ(y),χ(x) :
χ(x)χ′(x)−2x=λ
χ′(x)=(2x+λ)χ(x)
χ(x)=Aλex2+λx
2y−ϕ(y)ϕ′(y)=λ
ϕ′(y)=(2y−λ)ϕ(y)
ϕ(y)=Bλey2−λy
uλ(x,y)=ϕλ(y)×χλ(x)=Cλex2+y2+λ(x−y)
The range of possible λ , the constants Cλ are determined by boundary and initial conditions, the general sum can be expressed as a linear (possibly infinite) combination of uλ(x,y) for permitted values of λ .
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