The relaxation behavior of spin glasses has been analyzed in the framework of the critical fractal-cluster model. It is found that the relaxation rate of the magnetization can be expressed as $\frac{\ensuremath{\partial}m}{\ensuremath{\partial}\mathrm{ln}t}\ensuremath{\propto}{t}^{\ensuremath{-}\frac{\ensuremath{\beta}}{z\ensuremath{\nu}}}\mathrm{exp}[\ensuremath{-}{(\frac{t}{{\ensuremath{\tau}}_{\ensuremath{\xi}}})}^{\frac{\ensuremath{\beta}\ensuremath{\delta}}{z\ensuremath{\nu}}}]$, where $\ensuremath{\beta}$, $\ensuremath{\delta}$,
z, $\ensuremath{\nu}$ are standard static and dynamic critical exponents and ${\ensuremath{\tau}}_{\ensuremath{\xi}}$ is the relaxation time of a characteristic cluster which diverges at the spin-glass freezing temperature
Tg. The expression is valid through
Tg and is found to describe excellently the fundamental features of the relaxation in real spin glasses.