I have a hollow cylinder with a heat source inside. The generated heat flow is $\dot{Q}_g = 14\ 962 \ \text{W}$ , the cylinder has the radius $r = 20 \ \text{mm}$, the length $l = 50 \ \text{mm}$ and the thickness $t = 5 \ \text{mm}$. The inside temperature is $T_1 = 1300 \ \text{K}$. If the material is for example stainless steel with a conductivity of $\lambda = 30 \ \text{W/(m * K)} $ I get a reasonable outside wall temperature $T_2$:
$T_2 = T_1 - \dot{Q}_g \cdot \frac{\text{ln}(\frac{r + t}{r})}{2 \pi \cdot \lambda \cdot l} = 946 \ \text{K} $
But if I have a material with a low conductivity like $\lambda = 1 \ \text{W/(m * K)}$, the same equations gets me a negative outside wall temperature:
$T_2 = -9328 \ \text{K} $
That doesn't make sense to me. I think I made some stupid mistake, so is there another equation for this case or did I made a false assumption? Or something else? I already checked the units, and it looks all right. The unit for the conductivity is watt per meter kelvin, not milli kelvin. This looked wrong in the first version, sorry.
I would be really happy, if somebody could help me with this. Thanks!