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52 p a r t I I : F u n d a m e n t a l s<br />

search the Internet using terms such as “sunspot numbers” and “solar cycle 24”. (Appendix<br />

B includes a bountiful list of propagation-related Web sites.) As this is written,<br />

the current data for today’s date, partway into solar cycle 24, are: SFI = 88; SSN = 51;<br />

A = 12; K = 2.<br />

The ionosphere offers properties that affect radio propagation at different times.<br />

Variations occur not only over the 11-year sunspot cycle, but also diurnally and seasonally.<br />

Obviously, if the sun affects propagation in a significant way, then differences between<br />

nighttime and daytime, as well as between summer and winter, must cause<br />

variations in the propagation phenomena observed.<br />

Ionospheric Layers<br />

The ionosphere is divided, for purposes of radio propagation studies, into multiple layers.<br />

Like the boundary between the ionosphere and the stratosphere, the boundaries<br />

between these layers are well defined only in textbooks. However, even there you will<br />

find varying heights given for the altitudes of the layers above the earth’s surface. In<br />

reality, they don’t have sharply defined boundaries but, rather, blend one into another.<br />

Thus, the division of the ionosphere into layers is quite arbitrary. These layers (Fig. 2.26)<br />

are designated D, E, and F (with F being further subdivided into F1 and F2 sublayers).<br />

D Layer<br />

The D layer is the lowest layer in the ionosphere, at approximately 30 to 50 mi above the<br />

surface. This layer is not ionized as much as the higher layers because all forms of solar<br />

energy that cause ionization are severely attenuated by the higher layers before the<br />

energy reaches down into the D layer. Also, the D layer is much denser than the E and<br />

F layers, causing any positive and negative ions to recombine and form electrically<br />

neutral atoms more quickly than in the higher layers.<br />

The extent of D-layer ionization is proportional to the elevation of the sun, so it<br />

achieves maximum intensity at midday or very shortly thereafter. The D layer exists<br />

mostly during the warmer months of the year because of both the greater height of the<br />

sun above the horizon and the longer hours of daylight. As might be expected, therefore,<br />

the D layer almost completely disappears after local sunset, although some observers<br />

have reported sporadic incidents of D-layer activity for a considerable time past<br />

sunset. The D layer typically is a strong absorber of medium-wave signals (to such an<br />

extent that signals below 3 or 4 MHz are completely absorbed by the D layer). Because<br />

of this, most AM broadcast stations enjoy only local ground-wave coverage during daylight<br />

hours.<br />

E Layer<br />

The E layer exists from approximately 50 to 70 mi above the earth’s surface and is considered<br />

the lowest region of the ionosphere that supports, rather than absorbs, ionospheric<br />

radio communications. Like the D layer, this region is ionized only during the<br />

daylight hours, with ionization levels peaking at midday. The ionization level drops off<br />

sharply in the late afternoon and almost completely disappears after local sunset.<br />

For most of each year, the E layer is absorptive and does not reflect radio signals.<br />

During the summer months, however, E-layer propagation occurs frequently. A phenomenon<br />

called short skip (i.e., less than 100 mi for medium-wave and 1000 mi for shortwave<br />

signals) occurs in the E layer during the summer months and in equatorial regions<br />

at other times, as well.

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