[Code of Federal Regulations]
[Title 47, Volume 2]
[Revised as of October 1, 2007]
From the U.S. Government Printing Office via GPO Access
[CITE: 47CFR73.152]

[Page 38-41]
 
                       TITLE 47--TELECOMMUNICATION
 
        CHAPTER I--FEDERAL COMMUNICATIONS COMMISSION (CONTINUED)
 
PART 73_RADIO BROADCAST SERVICES--Table of Contents
 
                     Subpart A_AM Broadcast Stations
 
Sec.  73.152  Modification of directional antenna data.

    (a) If, after construction and final adjustment of a directional 
antenna, a measured inverse distance field in any direction exceeds the 
field shown on the standard radiation pattern for the pertinent mode of 
directional operation, an application shall be filed,

[[Page 39]]

specifying a modified standard radiation pattern and/or such changes as 
may be required in operating parameters so that all measured effective 
fields will be contained within the modified standard radiation pattern. 
Permittees may also file an application specifying a modified standard 
radiation pattern, even when measured radiation has not exceeded the 
standard pattern, in order to allow additional tolerance for monitoring 
point limits.
    (b) If, following a partial proof of performance, a licensee 
discovers that radiation exceeds the standard pattern on one or more 
radials because of circumstances beyond the licensee's control, a 
modified standard pattern may be requested. The licensee shall submit, 
concurrently, Forms 301-AM and 302-AM. Form 301-AM shall include an 
exhibit demonstrating that no interference would result from the 
augmentation. Form 302-AM shall include the results of the partial 
proof, along with full directional and nondirectional measurements on 
the radial(s) to be augmented, including close-in points and a 
determination of the inverse distance field in accordance with Sec.  
73.186.
    (c) Normally, a modified standard pattern is not acceptable at the 
initial construction permit stage, before a proof-of-performance has 
been completed. However, in certain cases, where it can be shown that 
modification is necessary, a modified standard pattern will be 
acceptable at the initial construction permit stage. Following is a non-
inclusive list of items to be considered in determining whether a 
modification is acceptable at the initial construction permit stage:
    (1) When the proposed pattern is essentially the same as an existing 
pattern at the same antenna site. (e.g., A DA-D station proposing to 
become a DA-1 station.)
    (2) Excessive reradiating structures, which should be shown on a 
plat of the antenna site and surrounding area.
    (3) Other environmental factors; they should be fully described.
    (4) Judgment and experience of the engineer preparing the 
engineering portion of the application. This must be supported with a 
full discussion of the pertinent factors.
    (d) The following general principles shall govern the situations in 
paragraphs (a), (b), and (c) in this section:
    (1) Where a measured field in any direction will exceed the 
authorized standard pattern, the license application may specify the 
level at which the input power to the antenna shall be limited to 
maintain the measured field at a value not in excess of that shown on 
the standard pattern, and shall specify the common point current 
corresponding to this power level. This value of common point current 
will be specified on the license for that station.
    (2) Where any excessive field does not result in objectionable 
interference to another station, a modification of construction permit 
application may be submitted with a modified standard pattern 
encompassing all augmented fields. The modified standard pattern shall 
supersede the previously submitted standard radiation pattern for that 
station in the pertinent mode of directional operation. Following are 
the possible methods of creating a modified standard pattern:
    (i) The modified pattern may be computed by making the entire 
pattern larger than the original pattern (i.e., have a higher RMS value) 
if the measured fields systematically exceed the confines of the 
original pattern. The larger pattern shall be computed by using a larger 
multiplying constant, k, in the theoretical pattern equation (Eq. 1) in 
Sec.  73.150(b)(1).
    (ii) Where the measured field exceeds the pattern in discrete 
directions, but objectionable interference does not result, the pattern 
may be expanded over sectors including these directions. When this 
``augmentation'' is desired, it shall be achieved by application of the 
following equation:

E([phis],[thetas])aug = [radic] { E([phis],[thetas])std {time} \2\+ 
    A{g([thetas]) cos (180 DA/S {time} \2\

where:

E([phis],[thetas])std is the standard pattern field at some particular 
azimuth and elevation angle, before augmentation, computed pursuant to 
Eq. 2, Sec.  73.150(b)(1)(i).
E([phis],[thetas])aug. is the field in the direction specified above, 
after augmentation.
A=E([phis], O)\2\aug-E([phis], O)\2\std in which [phis] is the central 
azimuth of augmentation. E([phis], O)aug

[[Page 40]]

and E([phis], O)std are the fields in the horizontal plane at the 
central azimuth of augmentation.

    Note: ``A'' must be positive, except during the process of 
converting non-standard patterns to standard patterns pursuant to the 
Report and Order in Docket No. 21473, and in making minor changes to 
stations with patterns developed during the conversion. However, even 
when ``A'' is negative, ``A'' cannot be so negative that 
E([phis],[alpha])aug is less than E([phis],[thetas])th at any azimuth or 
vertical elevation angle.

g([thetas]) is defined in Sec.  73.150(b)(1)(i).
S is the angular range, or ``span'', over which augmentation is applied. 
The span is centered on the central azimuth of augmentation. At the 
limits of the span, the augmented pattern merges into the unaugmented 
pattern. Spans may overlap.
DA is the absolute horizontal angle between the azimuth at 
which the augmented pattern value is being computed and the central 
azimuth of augmentation. (DA cannot exceed 1/2 S.)


In the case where there are spans which overlap, the above formula shall 
be applied repeatedly, once for each augmentation, in ascending order of 
central azimuth of augmentation, beginning with zero degrees 
representing true North. Note that, when spans overlap, there will be, 
in effect, an augmentation of an augmentation. And, if the span of an 
earlier augmentation overlaps the central azimuth of a later 
augmentation, the value of ``A'' for the later augmentation will be 
different than the value of ``A'' without the overlap of the earlier 
span.
    (iii) A combination of paragraphs (d)(2)(i) and (d)(2)(ii), of this 
section, with (d)(2)(i) being applied before (d)(2)(ii) is applied.
    (iv) Where augmentation is allowable under the terms of this 
section, the requested amount of augmentation shall be centered upon the 
measured radial and shall not exceed the following:
    (A) The actual measured inverse distance field value, where the 
radial does not involve a required monitoring point.
    (B) 120% of the actual measured inverse field value, where the 
radial has a monitoring point required by the instrument of 
authorization.

Whereas some pattern smoothing can be accommodated, the extent of the 
requested span(s) shall be minimized and in no case shall a requested 
augmentation span extend to a radial azimuth for which the analyzed 
measurement data does not show a need for augmentation.
    (3) A Modified Standard Pattern shall be specifically labeled as 
such, and shall be plotted in accordance with the requirements of 
paragraph (b)(2) of Sec.  73.150. The effective (RMS) field strength in 
the horizontal plane of E([phis],[alpha])std, E([phis],[alpha])th, and 
the root sum square (RSS) value of the inverse fields of the array 
elements (derived from the equation for E([phis],[alpha])th), shall be 
tabulated on the page on which the horizontal plane pattern is plotted. 
Where sector augmentation has been employed in designing the modified 
pattern, the direction of maximum augmentation (i.e., the central 
azimuth of augmentation) shall be indicated on the horizontal plane 
pattern for each augmented sector, and the limits of each sector shall 
also be shown. Field values within an augmented sector, computed prior 
to augmentation, shall be depicted by a broken line.
    (4) There shall be submitted, for each modified standard pattern, 
complete tabulations of final computed data used in plotting the 
pattern. In addition, for each augmented sector, the central azimuth of 
augmentation, span, and radiation at the central azimuth of augmentation 
(E([phis],[alpha])aug) shall be tabulated.
    (5) The parameters used in computing the modified standard pattern 
shall be specified with realistic precision. Following is a list of the 
maximum acceptable precision:
    (i) Central Azimuth of Augmentation: to the nearest 0.1 degree.
    (ii) Span: to the nearest 0.1 degree.
    (iii) Radiation at Central Azimuth of Augmentation: 4 significant 
figures.
    (e) Sample calculations for a modified standard pattern follow. 
First, assume the existing standard pattern in Sec.  73.150(c). Then, 
assume the following augmentation parameters:

------------------------------------------------------------------------
                                                               Radiation
                                             Central               at
            Augmentation number              azimuth    Span    central
                                                                azimuth
------------------------------------------------------------------------
1..........................................      110       40      1,300
2..........................................      240       50         52
3..........................................      250       10        130
------------------------------------------------------------------------


[[Page 41]]

    Following is a tabulation of part of the modified standard pattern:

------------------------------------------------------------------------
                                                                Vertical
           Azimuth                0          30         60       angle
------------------------------------------------------------------------
0...........................      28.86      68.05      72.06  .........
105.........................   1,299.42     872.14     254.21  .........
235.........................      39.00      35.74      38.71  .........
247.........................     100.47      66.69      32.78  .........
------------------------------------------------------------------------


[46 FR 11992, Feb. 12, 1981, as amended at 56 FR 64862, Dec. 12, 1991; 
66 FR 20756, Apr. 25, 2001]