Medium Voltage Power Cables Catalogue - AEC Online
Medium Voltage Power Cables Catalogue - AEC Online
Medium Voltage Power Cables Catalogue - AEC Online
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Annex D: Formulas<br />
D.1 Resistance<br />
The values of conductor DC resistance given in the previous<br />
tables are based on 20 °C. In case the DC resistance is required<br />
at any other temperature the following formula is used:<br />
Where;<br />
Conductor DC resistance at θ °C<br />
Conductor DC resistance at 20 °C<br />
Operating temperature<br />
Resistance temperature coefficient<br />
• 0.00393 for Copper<br />
• 0.00403 for Aluminum<br />
To get the AC resistance of the conductor at its operating<br />
temperature the following formula is used:<br />
Where<br />
and are the proximity and skin effect factors, respectively,<br />
which depend on the laying and operating frequency of the cable.<br />
D.2 Inductance<br />
Self and mutual inductance are formulated as follows:<br />
Where;<br />
Inductance<br />
Constant depends on the<br />
conductors’ number of wires<br />
Conductor diameter<br />
• 1 x S in case of trefoil formation<br />
• 1.26 x S in case of flat formation<br />
D.3 Capacitance<br />
Where;<br />
Capacitance<br />
Relative permittivity of insulation<br />
• XLPE = 2.5<br />
Diameter over insulation,<br />
excluding screen, if any<br />
Conductor diameter, including<br />
screen, if any<br />
km<br />
km<br />
km<br />
km<br />
km<br />
km<br />
km<br />
km<br />
D.4 Insulation Resistance<br />
Where;<br />
Insulation resistance<br />
Constant depends on the insulation<br />
material<br />
Inner diameter of the insulation<br />
Outer diameter of the insulation<br />
D.5 Charging Current<br />
The charging current is the capacitive current which flows<br />
when an AC voltage is applied to the cables as a result of the<br />
capacitance between the conductor and earth, and for a multi-core<br />
cable in which cores are not screened, between conductors.<br />
The value can be derived from following the equation:<br />
Where<br />
Charging current<br />
Phase voltage<br />
2 π f<br />
Operating frequency<br />
Capacitance to neutral<br />
D.6 Dielectric Losses<br />
The dielectric losses of an AC cable are proportional to the<br />
capacitance, the frequency, the phase voltage and the power<br />
factor. The value can be derived from the following equation:<br />
Where;<br />
Dielectric Losses<br />
2 π f<br />
Operating frequency<br />
Capacitance to neutral<br />
Phase voltage<br />
Dielectric power factor<br />
km<br />
km<br />
km<br />
km<br />
km<br />
km<br />
km<br />
km<br />
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