Thermodynamic foundations of the thermal entropy production are rested on the concept of lost heat, (Q/T) ST. The thermomechanical entropy production is shown to be in terms of the lost heat and the lost work as ,s where the second term in brackets denotes the lost (dissipated) work into heat. The dimensionless number II, describing the local entropy production s" in a quenched flame is found to be l-Is-(Per °)-2, where Yl, = s M 12/k, I = ~/Su ° (a characteristic length), k thermal conductivity, c~ thermal diffusivity, Su ° the adiabatic laminar flame speed at the unburned gas temperature, Per ° = Su°D/t~ the flame Peclet number, and