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Submarine power cable

QuickField simulation example

A three phase submarine power cable is buried in the sea bed.*

Problem Type
Plane-parallel problem of AC magnetics

Geometry
Cable length is 10 km.
Submarine power cable Calculate currents in the sheaves and armor and the magnetic flux density in the water above the cable C B A XLPE Armor Sheath Water Sand Air Submarine cable 1 m 20 m 40 m 11 m Ø172.8 mm

Given
Conductor current (r.m.s. value) I = 700 A, frequency 50 Hz.
Media conductivity: copper 58 MS/m, lead 5 MS/m, steel 1.1 MS/m, sea water 5 S/m, sand 1 S/m.
Armor (steel wire) relative magnetic permeability 300.

Task
Calculate the currents in the sheaves and armour and the magnetic flux density in the water above the cable.

Solution
Real cable includes many thin layers of semiconducting tape, used to eliminate local electric field disturbances, caused by the conductor surface irregularities. In this example we do not study these irregularities, the conductors are modelled as solid bodies with smooth surfaces, so the semiconducting layers are simulated as a part of main insulation.
In QuickField we should specify the peak values of currents that are √2 times more than r.m.s. values.
The armor and sheaths are grounded on each side and thewater and the sea-bed provide the natural return path for the currents. The conductor's connection is specified in the electric circuit.

Result
Induced current in the sheath is 381 A, induced current in the armor is 325 A. Voltage drop in phase conductor is 11.1 kV per 10 km.
Submarine power cable currents

Magnetic flux density in the water above the cable does not exceed 0.3 mT (root mean square value).
Undersea power cable magnetic field

Reference
*The idea of this example is inspired by the paper: Andrew B Gill, Yi Huang, Joe Spencer, and Ian Gloyne-Philips Electromagnetic Fields emitted by High Voltage Alternating Current Offshore Wind Power Cables and interactions with marine organisms