I checked one of the other questions on this - and I still seem to have a different equation than they offer (as far as I can tell). I'll use the notation the books used, btw.
In one of my reference books, they first derived the Rayleigh-Jeans formula (I can include how they derived it, if that will help):
$$u(v,T) = \frac{8\pi v^2}{c^3}k_BT,$$
($k_B$ - Boltzmann constant, $v$ - frequency, $T$ - temperature)
Then they "re-derived" Planck's formula by replacing the integral with the summation and ended up with:
$$u(v,T) = \frac{8\pi v^2}{c^3} \frac{hv}{e^{\frac{hv}{kT}}-1}$$
($h$ - Planck constant)
However, the next book I looked at puts Planck's Law in terms of $\lambda$:
$$u(\lambda) = \frac{8 \pi hc\lambda^{-5}}{e^{\frac{hc}{\lambda kT}}-1} = \frac{8\pi}{\lambda^5}\frac{hc}{e^{\frac{hc}{\lambda kT}}-1}$$
By the way, the Rayleigh-Jeans law the second book derived is:
$$u(\lambda) = \frac{8\pi kT}{\lambda^{-4}}$$
My questions are:
If both functions are valid, why are only one of them mentioned in each book? Why can't I find the function with $v^2$ on Wiki, or PSE... is the first book wrong?