The diffusion equation and a solution.
@Hunus Problem is found as attachment
In addition to that I need to determine what N0 is. and I know the following relations can help me by looking at it: \[\int\limits_{0}^{\infty}e ^{-a ^{2}x ^{2}}dx=\frac{ 1 }{ 2a }\sqrt{\pi}\] and \[\int\limits_{-\infty}^{\infty}c(x,t)dx=N0\]
\[\Large \frac{\partial c(x,t)}{\partial t} = \frac{D N e^{\frac{-x^2}{4Dt}} (x^2-2 D t)}{8 \sqrt{\pi} (D t)^{5/2}}\]\[\Large \frac{\partial^2 c(x,t)}{\partial x^2} = \frac{ N e^{\frac{-x^2}{4Dt}} (x^2-2 D t)}{8 \sqrt{\pi} (D t)^{5/2}}\]
\[\Large \frac{\partial c(x,t)}{\partial t} = D \frac{\partial^2 c(x,t)}{\partial x^2}\]
So we simply take the partial derivative to the function with respect to the correct variable and see they equal each other?
Or it is a solution to the PDE?
yes
No idea why we where given the expressions I wrote up then.
Perhaps they want you to do it another way?
It is that other way I simply don't understand.
If I had to guess for another way would be to look at the generalized diffusion equation\[\frac{ \partial c }{ \partial t }=D \frac{ \partial ^{2}c }{ \partial x ^{2} }-v \frac{ \partial c }{ \partial x }\] and use that: \[\frac{ \partial c }{ \partial t }=\left\{ c-\left[ c+\left( \frac{ \partial c }{ \partial x } \right)l \right] \right\} \frac{ v }{ l }=-v \frac{ \partial c }{ \partial x }\] Then assume that x=x0 at t=0. But the expression only become longer... god my brain is frying.
Think I go with your way, it show what we want and most be fine :)
Ones again, thank you :)
Do you still have to find N0?
Yup :)
I know it is N0 =n0 Na where n0 is the amount of molecules and Na Avogadro's constant :)
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