- #1
mhill
- 189
- 1
Studying a problem of difussion i came across the PDE (first order)
[tex] \partial _{t} U(x,t) = U(x,t)^{2} [/tex]
with initial condition [tex] \partial _{t} U(x,0) = \delta (x) [/tex]
i have found the solution [tex] U(x,t)= \frac{ \delta (x) }{ t \delta (x) -1} [/tex]
however does this make sense ? from the definition of delta function the only values that U(x,t) can have for different positions 'x' are just 0 or infinity , and if i use a Taylor expansion i get
[tex] U(x,t)= - \delta (x) ( t\delta (x) +t^{2} (\delta (x) )^{2}+...) [/tex]
which makes no sense for me
[tex] \partial _{t} U(x,t) = U(x,t)^{2} [/tex]
with initial condition [tex] \partial _{t} U(x,0) = \delta (x) [/tex]
i have found the solution [tex] U(x,t)= \frac{ \delta (x) }{ t \delta (x) -1} [/tex]
however does this make sense ? from the definition of delta function the only values that U(x,t) can have for different positions 'x' are just 0 or infinity , and if i use a Taylor expansion i get
[tex] U(x,t)= - \delta (x) ( t\delta (x) +t^{2} (\delta (x) )^{2}+...) [/tex]
which makes no sense for me