The filled elastomers are used very wide in many regions of modern technique. The members of the construction from similar materials can be used in the stress state in a long time. On many occasion the normal operation of the construction members from the filled elastomers is defined by the stress level in the material that can change with the time as a result of the relaxation processes. The intensity of the stress relaxation in the filled elastomers dependes substantially on the temperature. The temperature range of the service of the part from the filled elastomers can lap the range from 20 to 150oC. To obtain the adequate estimaitions of the influence of the relaxation processes on the normal operation of the part from the filled elastomers it is need to take into account the temperature effects on the material properties. As a rule the temperature increasing causes to monotone change the relaxation behavior of the most polymeric materials: the decreasing of the relaxation modulus or the increasing of the creep compliance. Many filled elastomers exhibit the anomalous dependence of the relaxation behavior on the temperature. These dependence is a topic of the given article. On the base of the analyses of the obtained experimental data for the stress relaxation at the tension it was shown that the filled elastomer on the base of hydrogenated nitryl-butyl rubber exhibit the traditional decreasing of the relaxation modulus by the temperature increasing to 50oC. At the following rise of the temperature to 125oC the relaxation modulus of these material increases anomalously. To account of the anomalous effects of the temperature on the relaxation properties of the elastomer it was proposed to use the method of the time-temperature superposition. The experimental shift function was defined by using the relaxation curves for the investigated elastomer. The generalized dependence of the relaxation modulus on the reduced time was obtained. The predicted dependences of the relaxation modulus on the temperature for long period of the relaxation were obtained with the application of the equation of the linear theory of the viscoelastisity and the experimentally defined function of the time-temperature shift.