Planck's law states that the energy density of blackbody radiation of wavelength $x$ is given by
$$f(x)=\frac{8 \pi h c x^{-5}}{e^{h c /(k T x)}-1}$$
Use the linear approximation in exercise 44 to show that $f(x) \approx 8 \pi k T / x^{4},$ which is known as the Rayleigh-Jeans law.