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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 />

143

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