4

I tried to bilinearize the two equations:

eq = {Laplacian[psi[t, x, y], {x, y}] + 
     6 u[t, x, y] psi[t, x, y] + (x^2 + y^2) u[t, x, y] == 
    I D[u[t, x, y], 
      t], -(I /Sqrt[2] (D[u[t, x, y], x] + D[u[t, x, y], y]) + 
       psi[t, x, y]) == 1/10000 D[psi[t, x, y], t]};

and I have looked at some posts here on stackexchange, but found no posts that considered the matter of bilinearization. Does anyone have a tip of where to start?

nssm2 = NonlinearStateSpaceModel[eq, psi[t,x,y], u[t,x,y], t]

but to no avail. I read also this:

https://library.wolfram.com/infocenter/Articles/2831/

But I couldn't find a hint there either.

Thanks

Vangsnes
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4 Answers4

3

Try

eq1=Normal[Series[eq /. {u -> Function[{t, x, y}, eps u[t, x, y]] ,psi -> Function[{t, x, y}, eps psi[t, x, y]]}, {eps,0,1}]] /.eps -> 1

to get the linearized two odes !

enter image description here

Ulrich Neumann
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3

I assume that by "bilinearize" you mean linearization relative to u[t, x, y] and psi[t, x, y]. This can be achieved using Series. Note, Series relative to more than one variable does does first linearization relative to the first variable. Then, the result is linearized relative to the second variable, e.t.c. That means, we get cross terms, that need to be eliminated. E.g.

eq = {Laplacian[psi[t, x, y], {x, y}] + 
     6 u[t, x, y] psi[t, x, y] + (x^2 + y^2) u[t, x, y] == 
    I D[u[t, x, y], 
      t], -(I /Sqrt[2] (D[u[t, x, y], x] + D[u[t, x, y], y]) + 
       psi[t, x, y]) == 1/10000 D[psi[t, x, y], t]};

To linearize, we do:

ser = Series[eq, {u[t, x, y], 0, 1}, {psi[t, x, y], 0, 1}];

This is a SeriesData object. For further work we need to get rid of the O[..] terms:

ser= ser // Normal;

To eliminate the cross terms, we first need to expand the expression and then set the cross terms to zero:

Expand[ser] /. u[t, x, y] psi[t, x, y] -> 0

enter image description here

Daniel Huber
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1

Hint.

Assuming you have an approximation $(u_k,\psi_k)$ then you can proceed linearly as

$$ \cases{ \mathcal{D}_1[u_{k+1}]+6(u_k \psi_k +u_k(\psi_{k+1}-\psi_k)+\psi_k(u_{k+1}-u_k))+(x^2+y^2)u_{k+1}=i \mathcal{D}_2[u_{k+1}]\\ -\frac{i}{\sqrt{2}}\mathcal{D}_3[u_{k+1}]+\psi_{k+1}=10^{-4}\mathcal{D}_4[\psi_{k+1}] } $$

solving for $(u_{k+1},\psi_{k+1})$ to obtain the next approximation. Here $\mathcal{D}_j[\cdot]$ are differential operators.

Cesareo
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1

Look what @Jens has done:

TaylorSeries[expr_, vars_?ListQ, start_?ListQ, order_?IntegerQ] := 
 Normal[Series[expr /. Thread[vars -> t*(vars - start) + start], {t, 0, order}]] /. t -> 1

eq = {Laplacian[psi[t, x, y], {x, y}] + 6 u[t, x, y] psi[t, x, y] + (x^2 + y^2) u[t, x, y] == I D[u[t, x, y], t], -(I/Sqrt[2] (D[u[t, x, y], x] + D[u[t, x, y], y]) + psi[t, x, y]) == 1/10000 D[psi[t, x, y], t]};

TaylorSeries[eq, {u[t, x, y], psi[t, x, y]}, {0, 0}, 1]

enter image description here

rmw
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