7

Shielding of Power Cables

Carl C. Landinger

CONTENTS

7.1    General

7.2    Conductor Shielding

7.3    Insulation Shielding for Medium Voltage Cables

7.3.1    Stress Relief Layer

7.3.2    Metallic Shield

7.3.3    Concentric Neutral Cables

7.4    Shielding for Low Voltage Cables

7.4.1    Electric Fields

7.4.2    Magnetic Fields

References

7.1    GENERAL

Shielding of an electric power cable is accomplished by surrounding the insulation of a single conductor or assembly of insulated conductors with a grounded, conducting medium. This confines the electric field to the inside of this shield. Two distinct types of shields are used: metallic and a combination of nonmetallic and metallic.

The purposes of the insulation shield are to:

1.  Obtain symmetrical radial stress distribution within the insulation.

2.  Eliminate tangential and longitudinal stresses on the surface of the insulation.

3.  Exclude from the electric field those materials such as braids, tapes, and fillers that are not intended as insulation.

4.  Protect the cables from induced or direct over voltages. Shields do this by making the surge impedance uniform along the length of the cable and by helping to attenuate surge potentials.

7.2    CONDUCTOR SHIELDING

In cables rated over 2,000 volts, a conductor shield is required by industry standards. The purpose of the conductor shield, also called conductor screen, over the conductor is to provide a smooth cylinder rather than the relatively rough surface of a stranded conductor in order to reduce the stress concentration at the interface with the insulation.

Conductor shielding has been used for cables with both laminar and extruded insulations. The materials used are either semiconducting materials or ones that have a high dielectric constant and are known as stress control materials. Both serve the same function of stress reduction.

Conductor shields for paper-insulated cables are either carbon black tapes or metalized paper tapes.

The conductor shielding materials were originally made of semiconducting tapes that were helically wrapped over the conductor. Present standards still permit such a tape over the conductor. This is done, especially on large conductors, in order to hold the strands together firmly during the application of the extruded semiconducting material that is now required for medium voltage cables. Experience with cables that only had a semiconducting tape was not satisfactory, so the industry changed their requirements to call for an extruded layer over the conductor.

In extruded cables, this layer is now extruded directly over the conductor and, in the case of semiconducting shields, is bonded to the insulation layer that is applied over this stress relief layer. It is extremely important that there are no voids or extraneous material between those two layers since this is the area of maximum voltage stress in a cable.

Present-day semiconducting extruded layers are made of clean materials (a minimum of undesirable impurities) and are extruded to be very smooth and round. This has greatly reduced the formation of water trees that could originate from irregular surfaces (commonly known as protrusions) because of high electrical stress. By extruding the two layers simultaneously, the conductor shield and the insulation are cured at the same time. This provides the inseparable bond that minimizes the chances of the formation of a void at that critical interface.

For compatibility reasons, the extruded shielding layer is usually made from the same or a similar polymer as the insulation. Special carbon black is used to make the layer over the conductor semiconducting to provide the necessary conductivity. Industry standards require that the conductor semiconducting materials have a maximum resistivity of 1,000 ohm-meter. Those standards also require that this material pass a longtime stability test for resistivity at the emergency operating temperature level to ensure that the layer remains conductive and hence provides a long cable life. This procedure is described in Reference [1].

While not widely done, a water-impervious material can be incorporated as part of the conductor shield to prevent radial moisture transmission. This layer consists of a thin layer of aluminum or lead sandwiched between semiconducting materials. A similar laminate may be used for an insulation shield for the same reason.

There is no definitive standard that describes the class of extrudable shielding materials known as “super smooth, super clean.” As will be described in Chapter 10 (Standards and Specifications), it is not usually practical to use a manufacturer’s trade name or product number to describe any material. The term “super smooth, super clean” is the only way at this time of writing to describe a class of materials that provide a higher quality cable than an earlier version. This is only an academic issue since the older types of material are no longer used for medium voltage cable construction by known suppliers. The point is that these newer materials have tremendously improved cable performance in laboratory evaluations.

7.3    INSULATION SHIELDING FOR MEDIUM VOLTAGE CABLES

The insulation shield for a medium voltage cable is made up of two components:

1.  A semiconducting or stress relief layer

2.  A metallic layer of tape or tapes, drain wires, concentric neutral wires, or a metal tube

They must function as a unit for a cable to achieve a long service life.

7.3.1    STRESS RELIEF LAYER

The polymer layer used with extruded cables has replaced the tape shields that were used many years ago. This extruded layer is called the extruded insulation shield or screen. Its properties and compatibility requirements are similar to that of the conductor shield previously described except that standards require that the volume resistivity of this external layer be limited to 500 ohm-meter. This lower resistivity value, as compared with the conductor shielding value, recognizes that the metallic shield component may not be in continuous contact (such as space between wires) and the fact that it is possible that workers could come in contact with the outer layer while the cable is energized.

The nonmetallic layer is directly over the insulation and the voltage stress at that interface is lower than at the conductor shield interface. Primarily to facilitate splicing and terminating operations, this outer layer is not required to be bonded for cables rated through 46 kV. At voltages above that, it is strongly recommended that this layer be bonded to the insulation.

Since most users want this layer to be easily removable, the Insulated Cable Engineers Association (ICEA) S-94-649-2004 [2] has established strip tension limits. Presently these limits are that a 1/2-inch wide strip cut parallel to the conductor peel off with a minimum of 3 pounds and a maximum of 24 pounds of force that is at a 90° angle to the insulation surface.

7.3.2    METALLIC SHIELD

The metallic portion of the insulation shield or screen is necessary to provide a low resistance path for charging current to flow to ground. It is important to realize that the extruded shield materials will not survive a sustained current flow of more than a few milliamperes. These materials are capable of handling the small amounts of charging current, but cannot tolerate unbalanced or fault currents.

The metallic component of the insulation shield system must be able to accommodate these higher currents. On the other hand, an excessive amount of metal in the shield of a single-conductor cable is costly in two ways. First, additional metal over the amount that is actually required increases the initial cost of the cable. Second, the greater the metal content (conductivity) of the insulation shield, the higher the shield losses that result from the flow of current in the central conductor. This subject is treated completely in Chapter 14 (Ampacity of Cables).

A sufficient amount of metal must be provided in the cable design to ensure that the cable will activate the backup protection in the event of any cable fault over the life of that cable. There is also the concern for shield losses. It therefore becomes essential that:

•  The type of circuit interrupting equipment be analyzed. What is the design and operational setting of the fuse, recloser, or circuit breaker?

•  What fault current will the cable encounter over its life?

•  The level of shield losses that can be tolerated is known. How many times is the shield to be grounded? Will there be shield breaks to prevent circulating currents?

Although there are constructions such as full and one-third neutral listed in ICEA standards for single-conductor, URD and UD cables, these may not be the designs that are the most economical for a particular installation. Studies have been published on the optimum amount of metal to use in the neutral [3,4]. Documents such as these should be reviewed prior to the development of a cable design. In Chapter 14, there is an in-depth discussion of shield losses.

7.3.3    CONCENTRIC NEUTRAL CABLES

When concentric neutral cables are specified, the concentric neutrals must be manufactured in accordance with applicable ICEA standards. These wires must meet ASTM B3 for uncoated wires or B33 for coated wires. These wires are applied directly over the nonmetallic insulation shield with a lay of not less than six or more than ten times the diameter over the concentric wires. These cables are intended to carry the circuit neutral currents in the shield as well as performing the functions presented for cables in which the metallic shield is not intended to carry neutral current. This may result in the need for additional metal in the shield and acceptance of higher shield losses.

A complicating factor is the growing presence of harmonics in circuits where the sine wave is altered. These may, if sufficient harmonic content exists, require additional neutral capacity.

7.4    SHIELDING FOR LOW VOLTAGE CABLES

Shielding of low voltage cables is generally required where inductive interference can be a problem.

In numerous communication, instrumentation, and control cable applications, small electrical signals may be transmitted through the cable conductor and amplified at the receiving end. Unwanted signals (noise) due to inductive interference can be as large as the desired signal. This can result in false signals or audible noise that can affect voice communications.

Across the entire frequency spectrum, it is necessary to separate disturbances into electric field effects and magnetic field effects.

7.4.1    ELECTRIC FIELDS

Electric field effects are those that are a function of the capacitive coupling or mutual capacitance between the circuits. Shielding can be effected by a continuous metal shield to isolate the disturbed circuit from the disturbing circuit. Even semiconducting extrusions or tapes supplemented by a grounded drain wire can serve some shielding function for electric field effects.

7.4.2    MAGNETIC FIELDS

Magnetic field effects are the result of a magnetic field coupling between circuits. This is a bit more complex than for electrical effects.

At relatively high frequencies, the energy emitted from the source is treated as radiation. This increases with the square of the frequency. This electromagnetic radiation can cause disturbances at considerable distance and will penetrate any “openings” in the shielding. This can occur with braid shields or tapes that are not overlapped. The type of metal used in the shield can also affect the amount of disturbance. Any metallic shield material, as opposed to magnetic metals, will provide some shield due to the eddy currents that are set up in the metallic shield by the impinging field. These eddy currents tend to neutralize the disturbing field. Nonmetallic, semiconducting shielding is not effective for magnetic effects. In general, the most effective shielding is a complete steel conduit, but this is not always practical.

The effectiveness of a shield is called the “shielding factor” and is given as:

SF=Induced voltage in shielded circuitInduced voltage in unshielded circuit

(7.1)

Test circuits to measure the effectiveness of various shielding designs against electrical field effects and magnetic field effects have been reported by Gooding and Slade [5].

This subject is also discussed in Chapter 9.

REFERENCES

1.  Insulated Cable Engineers Association Publication T-25-425-2003, “Guide for Establishing Stability of Volume Resistivity for Conducting Polymeric Compounds of Power Cables,” 1981, Global Engineering Documents, 15 Inverness Way East, Englewood, CO 80112, USA.

2.  Insulated Cable Engineers Association Standard S-94-649-2004, “Standard for Concentric Neutral Cables Rated 5,000-46,000 Volts,” Global Engineering Documents, 15 Inverness Way East, Englewood, CO 80112, USA.

3.  EPRI EL-3014 and EL-3102, RP-1286-2: “Optimization of the Design of Metallic Shield/Concentric Neutral Conductors of Extruded Dielectric Cables Under Fault Conditions,” EPRI, P. O. Box 10412, Palo Alto, CA 94303-0813.

4.  EPRI EL-5478, RP-2839-1: “Shield Circulating Current Losses in Concentric Neutral Cables,” EPRI, Palo Alto, CA.

5.  Gooding, F. and Slade, H., July 1955, “Shielding of Communication Cables,” AIEE Transactions, Vol. 74(Part I), pp. 532–579.

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