.... <#1062#>1<#1062#><#1062#>1<#1062#>
<#441#>One reviewer expressed surprise at this radius, but Ludwig's paper does indeed verify this rule. This rule actually refers to each polarization, so as Ludwig comments, ``twice surface area rule'' might be a better name. Trueman and Kubina give the same formula for wire radius [#Trueman90##1###, p.21]. Wires of this radius are on the verge of being too thick for the thin-wire treatment in NEC2 (the extended kernel option does not help with a mesh, since it cannot be used for segments with a complex junction), but experience has produced generally acceptable results following this rule.<#441#>
... (yellow<#1077#>2<#1077#><#1077#>2<#1077#>
<#443#>The colours mentioned are used in the graphical display of the model (see Section~#sec:meshing#532>).<#443#>
... taken<#1083#>3<#1083#><#1083#>3<#1083#>
<#283#>Editing major element coordinates, or selecting wire segments for excitation, are exceptions to this rule. In these cases hitting escape ends the editing or selecting session. An element thus incorrectly created is removed by deleting the major element.<#283#>
... element<#1088#>4<#1088#><#1088#>4<#1088#>
<#289#>This eliminates to a certain extent the need to retype node coordinates common to the previous element.<#289#>
... number<#1099#>5<#1099#><#1099#>5<#1099#>
<#312#>Segment numbers start at 1, denoting the segment joined to node 0.<#312#>