In this chapter we will solve the Maxwell’s equations for a radiating wire and by analyzing the solution we will define the nearfield and the farfield. The electromagnetic field radiating from a wire can be calculated by solving Maxwell’s equations for a short current element and then placing the current elements endtoend.
Figure 3 A small current element or an electric dipole.
To be able to derive the field of a conducting element acting as an electrical dipole, the current in the element is defined to flow along an axis z. This gives that the magnetic vector potential can be expressed as (see Equation 26):
Equation 31 
where:
Equation 32 
It is wise to use spherical coordinates when deriving the field of a small current element that can be approximated with a point source
Equation 33 
If A is then expressed in the form
Equation 34 
it can apparently be divided into the spherical components:
Equation 36 

Equation 37 
The intensity of the magnetic field is then (using Equation 27):
Equation 38 
According to Equation 30 above E can be determined when H is known:
Equation 39 
Which results in:
Equation 40 

Equation 41 

Equation 42 
By rewriting those equations we can identify the wavelength and get the following equations in Table 3. A summation of the theory above states that:
If the length of one element is much less than a wavelength (dl << l ) and the element is considered as an oscillating dipole the electric and magnetic fields for one element can, with the use of some algebra, be expressed as:
Table 3 The electric and magnetic field equations for a small oscillating electric dipole
Electric and Magnetic Field Equations for an Electric Dipole 

where:
Analyzing these equations (Equation 43 to Equation 45) we can divide the terms into three different basic terms:
Figure 4 The significance of the different terms for the electric field strength
Notice that all these terms with the coefficients , and will all be equal (=1) at the distance . This distance is in this report said to be the boundary between nearfield and farfield and the contributions from the radiation, induction and the electrostatic term are all of the same magnitude.
When r << only the first term in each equation is significant and will in this case mean that the wave impedance will be:
Equation 46 
that is much greater than the free space impedance Z_{0} i.e. we will have a high Efield and a low Hfield. If the current element had been a current loop with a low circuit impedance instead of the high circuitimpedance of the current element, the first term, or the electrostatic term, in the first two equations (Equation 43 and Equation 44) would disappear and a similar equation would appear in Equation 45. In this case the wave impedance would be:
Equation 47 
representing a high Hfield and a low Efield in the nearfield.
When r >> the last term proportional to r^{1} in Equation 43 and Equation 45 will dominate and the wave impedance will approach the free space impedance Z_{0} = 377W . This is called the farfield or radiation field. The Eq and the Hf fields will then be in phase and orthogonal to each other producing plane waves. This is illustrated in Figure 5 below:
Figure 5 Wave impedance at different distances from either an electric source or a magnetic source
When such current elements are placed endtoend to produce a model of a radiating wire, the charge at the ends of the elements will cancel and the term due to the electrostatic field (the one proportional to r^{3}) will disappear. This is however only true with a constant current distribution on the line. With a varying current distribution the electrostatic fields will not cancel entirely. However, if the wire is divided into a sufficient number of segments per wavelength then this error will be small.
The length of telecommunication lines and the size of telecommunication systems are often greater than one wavelength, D ³ l . If the dimension of the field source D is greater than a wavelength the nearfield/farfield boundary is said to be at the distance [5]:
Equation 48 
At a shorter distance maxima and minima would appear due to interference caused by different distances to different parts of the source.
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EMC of Telecommunication Lines
A Master Thesis from the Fieldbusters © 1997
Joachim Johansson and Urban Lundgren