IEC 60986 pdf download.Short-circuit temperature limits of electric cables with rated voltages from 6 kV ( U m = 7,2 kV) up to 30 kV ( U m = 36 kV)
This International Standard gives guidance on the short-circuit maximum temperature limits of electric cables having rated voltages from 6 kV ( U m = 7,2 kV) up to 30 kV ( U m = 36 kV), with regard to the following: – insulating materials; – oversheath and bedding materials; – conductor and metallic sheath materials and methods of connection. The design of accessories and the influence of the installation conditions on the temperature limits are taken into consideration. The calculation of the permissible short-circuit current in the current-carrying components of the cable should be carried out in accordance with IEC 60949.
2 Normative references
The following normative documents contain provisions which, through reference in this text, constitute provisions of this International Standard. For dated references, subsequent amendments to, or revisions of, any of these publications do not apply. However, parties to agreements based on this International Standard are encouraged to investigate the possibility of applying the most recent editions of the normative documents indicated below. For undated references, the latest edition of the normative document referred to applies. Members of IEC and ISO maintain registers of currently valid International Standards. IEC 60055 (all parts), Paper-insulated metal-sheathed cables for rated voltages up to 18/30 kV (with copper or aluminium conductors and excluding gas-pressure and oil-filled cables) IEC 60141 (all parts), Tests on oil-filled and gas-pressure cables and their accessories IEC 60502-2:1998, Power cables with extruded insulation and their accessories for rated voltages from 1 kV (U m = 1,2 kV) up to 30 kV (U m = 36 kV) – Part 2: Cables for rated voltages from 6 kV (U m = 7,2 kV) up to 30 kV (U m = 36 kV) IEC 60949:1988, Calculation of thermally permissible short-circuit currents, taking into account the non-adiabatic heating effects
3 Factors governing the application of the temperature limits
3.1 General The short-circuit temperatures given in clause 4 are the actual temperatures of the current- carrying component as limited by the adjacent material in the cable and are valid for short- circuit durations of up to 5 s. When calculating the allowable short-circuit current, these temperatures will be obtained if heat loss into the insulation during the short-circuit is taken into account (non-adiabatic heating). If heat loss during the short-circuit is neglected (adiabatic heating), the calculations give short-circuit currents that are on the safe side.NOTE The temperature limits given in clause 4 should also not be exceeded with repeated short-circuits occurring in a short time. The 5 s time period mentioned is the limit for the temperatures quoted to be valid and not for the application of the adiabatic calculation method. The time limit for the use of the adiabatic method has a different definition, being a function of both the short-circuit duration and the cross-sectional area of the current-carrying component. This is dealt with in IEC 60949. The short-circuit temperature limits recommended in this standard are based on the consideration of the range of limits used by various authorities. They are not necessarily the ideal values as very little applicable experimental data are available on actual cables. The values are, however, considered to be on the safe side. The limits for cables in this standard are selected so that the dielectric properties are not impaired. The impairment of dielectric properties will be very dependent on the type of cable, for example adhesion of the semi-conducting screens will most likely set the limits for polymeric insulated cables, whereas the properties of the dielectric itself are of more importance in paper cables (both oil-filled and mass-impregnated cables). Caution may be needed when using the conductor temperatures specified when the cables are sheathed with a lower temperature material, especially for cables with conductor cross- sectional areas of 1 000 mm 2 and above. This is because the high thermal time constant of these cables will cause the oversheath to attain high temperatures for longer times. In addition, the high mechanical forces could result in insulation deformation. Nevertheless, it should be stressed that for conductor cross-sectional areas above 1 000 mm 2 , the permissible short- circuit current is so high that it is not normally attained in common systems.