NEHER–MCGRATH RESOURCE LIBRARY

Calculation Example

Equations, thermal terms, and a worked Neher–McGrath calculation.

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Neher-McGrath Equation

The Neher–McGrath method is used to calculate underground cable temperatures and cable ampacity ratings. The method comes from J. H. Neher and M. H. McGrath, "The Calculation of the Temperature Rise and Load Capability of Cable Systems", AIEE Transactions, Part III, Volume 76, pp. 752–772, October 1957. This paper considers the heat transfer issues associated with underground system ampacities. The paper cites the following basic equation for calculating cable ampacity:

Basic Neher–McGrath ampacity equation

However, this single equation masks the great complexity involved in these procedures (see the calculation example). There are scores of complicated equations involved in developing the terms in this equation and those required for temperature calculations. (The paper defines over 80 variables and contains in excess of 70 formulas excluding appendices.) To solve for unique ampacities or temperatures at each cable position, a set of simultaneous equations must be developed to take into account interference heating from every position in the system, and a matrix technique must be used to solve them. Many of the ampacity calculations we use today are based on a 1957 paper by J. H. Neher and M. H. McGrath. Later work by CIGRE (INTERNATIONAL COUNCIL ON LARGE ELECTRIC SYSTEMS) documented an ampacity procedure into an international standard (IEC-287 and IEC-853) that provides a stepwise approach to calculating ampacity based upon cable construction. The two calculation approaches give similar results, although their treatment of daily load cycles is different. The paper by Neher and McGrath assumes a sinusoidal load shape and uses a 24-hour (daily) loss factor to account for an overall "averaging" effect of heat output from the cable beyond a certain diameter (called DX). Within this diameter, the temperature rise across the thermal resistances in the cable and nearby soil is proportional to the peak heat output from the cable. At distances greater than this diameter away from the cable center, the temperature rise is proportional to the average daily heat output. Many system planners are familiar with a "load factor" which relates the peak load to the average daily load. In cable systems, we are interested in heat output, a function of I²R, so we use the daily "loss factor", which is essentially the load factor of the losses as defined by the following equation:

Daily loss factor equation

Concept of ampacity. An underground cable circuit rating, or “ampacity”, is the solution to a basic heat transfer problem. Heat generated in the cable is removed by thermal conduction to ambient earth and, ultimately, air. Engineers familiar with Ohm’s Law know that electrical current flowing through a resistance will produce a voltage drop according to the following relationship: Neher-McGrath ampacity equation

Ohm’s law relationship

An analogous relationship may be used to describe thermal conduction where heat flowing
through a thermal resistance produces a temperature drop (or rise) according to the following:

Thermal conduction relationship

This basic concept is extended to model heat flow out of a buried cable through the various cable
layers, trench backfill, and native earth.

Dielectric Heating

Dielectric heating comes from charging and discharging the insulating dielectric at 50 or 60
times per second. The dielectric heat loss, WDielectric, can be found from the following equation:

Dielectric heat-loss equation

The AC resistance increment for conductor skin effect, YCS, can be found from the following
equation, where kS is the skin effect factor based on the conductor construction.

AC resistance increment for conductor skin effect

The AC resistance increment for conductor proximity effect, YCP, can be found from the
following equation, where kP is the proximity effect factor based on the conductor construction.

AC resistance increment for conductor proximity effect

Shield Loss Increments for Eddy Currents

Eddy current losses occur when a continuous concentric metallic layer exists around the cable
core (e.g., a corrugated or extruded metal sheath or longitudinally taped metallic shield, but not
to stranded shields). Also, eddy currents are negligible for pipe-type cables.
The process for calculating eddy current losses is somewhat onerous but not particularly
complicated. The equations to perform these calculations were derived empirically and are listed
below. For a more detailed explanation, please see IEC-287.

Shield loss equations for eddy currents

Terms

Definitions of terms in the heating calculations
Linear heat-transfer diagram

Neher-McGrath Calculation Example

Worked Neher–McGrath example, sheet 1
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