Using 3D Models to Investigate Inductive Effects in a Submarine Cable

July 9, 2020

Replacing a faulty submarine cable can be extremely costly (potentially over 100 million US dollars), so the typical design is built to last for over forty years. To ensure a good return on investment, the industry typically acts on the conservative side: relying heavily on rules of thumb, safety margins, life-cycle analysis, and standards such as those provided by the International Electrotechnical Commission (IEC). However, these margins and standards tend to result in an overestimation of the required dimensions and materials. In a competitive market, cable suppliers are looking for more cost-effective solutions.

Note that in this blog post, we go over the final two parts of the 8-part Cable Tutorial Series, which focus on 3D cable modeling. The series discusses many aspects of cable modeling — in 2D, 2.5D, and 3D — using COMSOL Multiphysics® and the AC/DC Module. The first six parts of the tutorial series have been showcased in a previous blog post: Modeling Cables in COMSOL Multiphysics®: An 8-Part Tutorial Series.

Rapidly Advancing Capabilities in Cable Modeling

Just a few years ago, detailed 3D cable models were available only to experts running dedicated codes on large cluster systems. Nowadays, anyone with access to a modern desktop computer is able to run a 3D cable model with twisted magnetic armor in about half an hour. The geometry handling, meshing, solving, and postprocessing are all done within the user-friendly desktop environment of the COMSOL Multiphysics® software.

A submarine cable modeled in COMSOL Multiphysics, showing the resistive and magnetic loss density.
The resistive and magnetic loss density in the phases, screens, and armor of a three-core lead-sheathed XLPE HVAC submarine cable at a nominal phase temperature of 90°C.

Consequently, in the power cable industry, 3D cable models are slowly replacing empirical models such as those provided by the IEC series of standards. For typical use cases, these standards allow manufacturers to meet certain specifications. For users of cable systems, they allow for assessing the required operating conditions, the resulting system limitations, and so on.

While the standards rely on empirical models and decades of experience, numerical models actually solve Maxwell’s equations in full detail. The obvious advantage is that it allows for investigating devices for which there is no official standard. Furthermore, numerical models provide a means to get a detailed insight in the physical phenomena at play, and so go beyond the standards. This will allow for cutting down on material and manufacturing costs and increase system efficiency, while still keeping a sufficiently large safety margin. Within the competitive cable market, numerical analysis is considered a vital asset.

Geometry and Meshing Considerations for 3D Twisted Cable Models

For large 3D FEM models, setting up the geometry and mesh can easily take up the majority of your modeling time — that is; your man-hours, not your machine-hours — especially for twisted cable models with separate lay lengths, like the one featured here. Even when using twisted periodicity conditions, the geometry will include extreme aspect ratios. This means that if you would just use a general-purpose, isotropic, free tetrahedral mesh, the amount of degrees of freedom (DOFs) would easily rise to over thirty million!

An iterative solver might be able to handle this without too much memory consumption, but finding one that can reliably and efficiently solve the model is easier said than done. Using a direct solver proves to be a better option, but for it to work smoothly on reasonably cheap hardware — like a desktop machine with 32 GB of RAM and several hundred gigabytes of SSD swap drive capacity — the DOF count will need to be lowered to about 2–4 million. Fortunately, direct solvers are more forgiving than iterative ones when it comes to anisotropic meshes.

A model geometry of a three-core lead-sheathed cable with a twisted armor shown in 3D.
Image of the swept mesh for the three-core cable model in COMSOL Multiphysics.

Left: The 3D geometry of a three-core lead-sheathed cable with twisted armor. Right: The swept mesh in the phases, screens, and armor (the void region between the screens and the armor uses a stretched tetrahedral mesh).

Consequently, the challenge is to find a mesh that can properly resolve the cable geometry and the physics, with a DOF count low enough so that the model can be solved in a reasonable amount of time on an average desktop machine. The Geometry & Mesh 3D tutorial (Part 7 of the tutorial series) shows you how to tackle this challenge efficiently. The tutorial discusses various geometry- and meshing-related topics, including how to:

  1. Create the helical conductors using the COMSOL geometry sequence
  2. Make use of clever selection filters for the domains and boundaries to greatly ease the model setup
  3. Set up an efficient and robust meshing strategy

When setting up the geometry, geometrical correction factors are used, such as slant- and truncation correction factors. This is to get the best possible accuracy for the least amount of computational effort. Furthermore, swept meshes are discussed, as well as stretched tetrahedral meshes, boundary layer meshes, and mesh conformity.

Using 3D Models to Investigate Inductive Effects in a Submarine Cable

The Inductive Effects 3D tutorial (the final part of the series) gives you a comprehensive overview of the topics involved when modeling a XLPE HVAC submarine cable in 3D. Although 2D and 2.5D models are very valuable for cable engineering, they cannot capture the precise, intricate interactions between the phases, screens, and armor the same way that a 3D model can. Why? Typically, the phases and armor are twisted with different lay lengths, in opposite directions. The opposite twist causes the magnetic flux density to develop a longitudinal component in the armor: The magnetic flux will follow a helical path, rather than a circular one (see image below). This phenomenon — and related effects — can only be investigated using full 3D twist models.

An image of the path of the magnetic flux lines from wire to wire in the submarine coil.
A plot of the longitudinal magnetic flux density resulting from the magnetic flux line path.

Left: The path taken by the magnetic flux lines (they follow the armor wires for a certain distance, and hop from wire to wire). Right: The resulting longitudinal magnetic flux density.

Now, let’s go over some of the topics discussed in part 8 of the Cable Tutorial Series…

The Extruded 2D Model

This section explains how to build a 3D cable model that should be completely equivalent to the 2D one: A plain extrusion, without twist. At first glance, the exercise may not seem useful, but it actually provides you with a great deal of information! The 3D model has been heavily simplified as compared to the 2D one, and uses first-order shape functions instead of second-order ones (meaning the solution will be piecewise linear instead of quadratic). These measures are necessary to keep the 3D model manageable, but they come at a cost. By creating a 3D model that should — in theory — produce the same results as the 2D one, you can investigate the effect of the used simplifications. It provides you with a lower bound of how accurate the 3D models really are (around 0.2–0.5%), without even the need for an actual measurement (those come with a limited accuracy too, by the way).

Another big advantage of this modeling step is that it allows you to test your model before going full-scale: Since at this point, the geometry is not twisted, there is no specific length required to follow the twisted periodicity. While the twisted model will need to have a length equal to the cable’s cross pitch, the extruded 2D model is chosen to be ten times shorter. It solves in a minute rather than half an hour, helping you to quickly do some tests and sanity checks. When done, the fully parameterized geometry will allow you to proceed to a full 3D twist geometry at the flip of a switch.

It is a good modeling practice to test and validate your models at a small scale (preferably 2D), before going full-scale. You should first convince yourself that your numerical simulation is robust, efficient, and accurate enough to serve its purpose. Already at that stage, you will learn a lot about the basic behavior of your device — and where to cut costs, for example. After that, you can easily take your models beyond the point that you can cover with ordinary prototypes or measurements, including parametric sweeps and automated optimization.

The 3D Twist Model

With the twist included, you enter a different level of cable modeling. First of all, you will need to have the right kind of periodicity. The periodic length of the cable is determined by the lay length of the phases and the armor (in this case, it is about 1.6 meters). The periodicity is not a straight projection from one periodicity plane to another, though. Instead, it includes a twist. The cable’s straight (untwisted) periodicity may be as much as forty meters! This is why the twisted periodicity has been a reoccurring topic in recent cable papers.

 

Animation of the phase currents, screen currents, armor currents, armor flux, armor losses, temperature distribution, and mesh structure.

Now, the cable’s behavior changes. The magnetic flux develops a longitudinal component in the armor, and the induced armor currents develop small eddies encircling the armor wire’s centerline. The twist suppresses the total longitudinal current per armor wire to zero, but it does not constrain the currents locally. Consequently, the currents will flow in the positive longitudinal direction on the inside of the armor (where the phases and screens are), and flow back on the outside (where the electromotive force from the phases is weaker). This effect is successfully reproduced by the 2.5D models shown in Part 4 of the series. The circular eddies, however, can only be seen in 3D.

 

The transverse currents form eddies in the cross section of the wire (the cones); the longitudinal currents flow back and forth and are zero on average (the gradients).

Linearized Resistivity in 3D

Thermal effects are an important part of cable modeling. Submarine cables typically operate at temperatures around 80–90°C, and the cable’s material properties are temperature dependent. A very efficient way to deal with thermal effects in 3D is to take the temperatures from a 2D induction heating model (as demonstrated in Part 6 of the series) and use those to specify your temperature-dependent material properties in 3D. This can be seen as a first-order temperature correction. If you like, you can repeat the procedure:

  1. Compute the average phase-, screen-, and armor losses in 3D
  2. Use those as a heat source in a 2D thermal model
  3. Solve for the temperature, and…
  4. Use the average phase-, screen-, and armor temperatures to update your material properties in 3D

In COMSOL Multiphysics, you can even go for a fully coupled, hybrid 3D/2D induction heating model if you like — or a full 3D one, for that matter. Either way, you will find that the temperatures converge very quickly: The first-order temperature correction is more than enough in most cases. It reduces an initial error of about 10–20% to as little as 0.2%.

2D Fully Coupled Induction Heating 3D Twist Model
(No Heating)
3D Twist with First-Order Temperature Correction
Phase Losses (kW/km) 58 48 59
Screen Losses (kW/km) 11 18 15
Armor Losses (kW/km) 6.8 2.8 2.8
Phase AC Resistance (mΩ/km) 59 53 59
Phase Inductance (mH/km) 0.43 0.44 0.45

Results from the 3D twist model with first-order temperature correction, as compared to the 3D twist and 2D fully coupled induction heating models.

The change in resistivity causes the cable to rebalance itself. The active conductors are current driven, causing the local losses to increase. The passive conductors are voltage driven, however, causing the local induced currents and losses to decrease. In addition to this, there are a number of waterbed effects. To illustrate: Due to the reduced eddy currents in the armor, the magnetic flux penetrates the armor wires more easily, and the magnetic losses increase. At a nominal phase temperature of 90°C, they comprise about 75% of the total armor losses.

A plot of the volumetric loss density in the armor and screens of the submarine cable.
A plot of the average longitudinal current density in the cable armor.

Left: The volumetric loss density in the armor and screens after applying a first-order temperature correction. Right: The average longitudinal current density in the armor, before applying the compensation term.

Compensated Stabilization

Electrical conductivity is likely to be one of the material properties with the largest range of naturally occurring values. The cross-linked polyethylene (XLPE) in the cable has an electrical conductivity with a value around 1e-18 S/m, while the copper has a value of 6e+7 S/m — a contrast of 6e+25! In order to keep the model numerically stable, the insulators are given an artificial conductivity of 50 S/m. For an inductive model like this, 50 S/m turns out to be a perfectly reasonable approximation of zero (giving a good “insulator”) — just as for capacitive models, 1 S/m may already give a good approximation of a “conductor” (for more on the capacitive properties of the cable, see Part 2 of the tutorial series).

In order to demonstrate that 50 S/m is a reasonable value, the model is solved using a procedure that compensates for the resulting current leakage. First, the total longitudinal armor currents (integrated over the armor wire’s cross section) are evaluated to show there is indeed a leakage between the wires (see image above). Then, the model is solved a second time. The second time, an artificial current is added that is equal to “minus the leakage” (a bit like installing a pump, to compensate). As a result, the artificial insulator losses go down from 0.1 kW/km (which is already insignificant compared to the overall loss) to 0.0002 kW/km. Just like higher-order temperature corrections, this procedure can typically be omitted. Still, it is a useful tool if you wish to do some additional verification.

Note: These insulator losses are related to numerical stabilization. They are different from the typical tan(δ) dielectric losses used in capacitive models. Also note that alternative numerical approaches are available that do not require this amount of stabilization. Those will typically require much more computational resources though, giving you a less cost-effective workflow. So the goal is not to have a model that is as accurate as possible, but to have a model that gives you a good return on investment.

Additional Ways to Use the Cable Tutorial Series

Believe it or not, the Cable Tutorial Series is not just “all about cables” — It is about electromagnetics and numerical analysis, good engineering practices, understanding and applying theory, validating results, and presenting your results to be both visually appealing and informative.

The example of the three-phase cable with twisted magnetic armor is ideal for illustrating various electromagnetic and numeric phenomena in courses given at the university, or within the industry. Many cables are standardized, which means their physical properties are available from literature, allowing you to validate your modeling results. At the same time, cables are subject to ongoing research, which makes them an intriguing subject for engineering students and academic students alike.

Next Steps

Try out the 8-part Cable Tutorial Series by clicking the button below. You can skip to parts 7 and 8 to study inductive effects in the 3D cable model. Note that you must be logged into a COMSOL Access account with a valid software license to download the MPH-files.

Read about parts 1–6 of the tutorial series here: Modeling Cables in COMSOL Multiphysics®: 8-Part Tutorial Series


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Jean-Marc Petit
Jean-Marc Petit
July 31, 2020 COMSOL Mitarbeiter

Great blog ! Explanations are worthfull. Thanks !

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