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Field-strength Contour Mapping

Author: Edmund A. Laport

To construct a field-strength contour map of a station, a number of field-strength versus distance curves are measured and plotted for several radials from the antenna out to a distance where the signal approaches the ambient-noise level. The location of various field strengths can then be transcribed on a map and the various signal strength contours drawn in. The choice of contours depends on the region, the population distribution, and the situation with regard to interference, if any, on the channel.

The usual purpose of such a map is to show service areas of different classes served by direct ground wave. These represent the daylight coverage, but not necessarily the nighttime coverage, because interference between ground waves and sky waves causes selective fading that may reduce the satisfactory service range appreciably under some conditions.

A typical example of the manner in which a composite-conductivity radial is computed is the following: A station on 1,000 kilocycles, operating with a power of 10,000 watts with a vertical radiator 60 degrees high and an optimum ground system, is situated on a plain having a conductivity of 7·10-14 electromagnetic unit. In one direction, this conductivity extends for a distance of 6 miles, then becomes fresh water for a distance of 11 miles with a conductivity of 10·10-14. From here on, there is sandy and rocky soil with an average conductivity of 2·10-14.

TABLE 2.1. UNATTENUATED FIELD STRENGTHS AT 1 MILE FROM UNIFORM-CROSS-SECTION VERTICAL RADIATORS HAVING ESSENTIALLY SINUSOIDAL CURRENT DISTRIBUTION, AS FUNCTIONS OF ELECTRICAL HEIGHT G DEGREES AND RADIATED POWER.
(To convert to the basis of 1 kilometer, multiply all values by 1.61. Field strengths in millivolts per meter)
G Power radiated (watts)
degrees 10 25 100 250 1,000 5,000 10,000 50,000 100,000 1,000,000

10

18.6

29.4

58.9

93

186

417

589

1,320

1,860

5,890

20

18.6

29.4

58.9

93

186

417

589

1,320

1,865

5,895

30

18.7

29.6

59.2

93.5

187

419

592

1,327

1,870

5,920

40

18.8

29.7

59.5

94.1

188

421

595

1,333

1,880

5,950

50

18.9

29.9

59.8

94.6

189

423

598

1,341

1,890

5,980

60

19.0

30.1

60.2

95.1

190

426

602

1,350

1,900

6,020

70

19.1

30.2

60.5

95.6

191

428

605

1,357

1,910

6,050

80

19.3

30.5

61.1

96.6

193

432

611

1,369

1,930

6,110

90

19.5

30.8

61.7

97.6

195

437

617

1,384

1,950

6,170

100

19.7

31.2

62.4

98.6

197

442

624

1,400

1,970

6,240

110

20.0

31.6

63.3

100.

200

448

633

1,420

2,000

6,330

120

20.3

32.1

64.3

101.6

203

455

643

1,442

2,030

6,430

130

20.7

32.8

65.5

103.7

207

464

655

1,470

2,070

6,550

140

21.1

33.4

66.8

105.6

211

473

668

1,500

2,110

6,680

150

21.6

34.2

68.4

108.1

216

484

684

1,532

2,160

6,840

160

22.1

35.0

70.0

110.7

221

495

700

1,568

2,210

7,000

170

22.8

36.1

72.2

114

228

511

722

1,620

2,280

7,220

180

23.6

37.4

74.7

118

236

529

747

1,675

2,360

7,470

190

24.5

38.8

77.6

123

245

549

776

1,740

2,450

7,760

200

25.5

40.3

80.8

128

255

571

808

1,810

2,550

8,080

210

26.5

41.9

84.0

133

265

594

840

1,880

2,650

8,400

220

27.3

43.2

86.5

136

273

612

865

1,940

2,730

8,650

230

27.6

43.7

87.5

138

276

618

875

1,958

2,760

8,750

240

26.8

42.4

84.9

134

268

600

849

1,900

2,680

8,490

250

24.4

38.6

77.3

122

244

547

773

1,733

2,440

7,730

260

20.5

32.4

65.0

103

205

459

650

1,453

2,050

6,500

300

6.0

9.5

19.0

30

60

135

190

427

600

1,900

The field at one mile, from Table 2.1, is 602 millivolts per meter. From Fig. 2.2 for 1,000 kilocycles and a conductivity of 7·10-14, we find that the field strength has fallen to 11 percent of the unattenuated value of 1 mile, or to 66 millivolts per meter at 6 miles. In passing over the fresh water a distance of 11 miles, a distance between 6 and 17 miles

from the antenna, the signal is decreased to 23 percent of 66 millivolts per meter, or to a value of 15 millivolts per meter.1 From here on, the conductivity of 2·10-14 attenuates the signal as listed:

Distance from antenna (miles) Ratio of field strength at distance to that at water's edge 17 miles from antenna Expected field strength (millivolts per meter)

17

1.00

15

25

0.42

6.2

50

0.16

2.4

75

0.04

0.6

100

0.02

0.3

150

0.0064

0.096

If the ambient-noise level during daylight hours at a town on this radial at a distance of 150 miles averages 30 microvolts per meter, the signal-to-noise ratio average would be approximately 10 decibels.

In the same way, each radial can be computed, and the service range of the station in terms of signal-to-noise ratios or in terms of actual field strengths can be determined. The same procedure is followed if a directive antenna is used, except that in the latter case the field strength along the ground at 1 mile will vary with the azimuth angle depending upon the directive pattern of the array.

1) This method is adequate for practical purposes when the differences in conductivities for different portions of the ground path are small. The method is subject to errors of importance when, for example, a land path with a conductivity of 2·10-14 changes to sea water. In such cases, more accurate results may be obtained by computing the same path in both directions by the method outlined, interchanging the locations of transmitter and receiver, and averaging the two curves point by Point along the radial.


Last Update: 2011-03-19