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Exploring the Unknown - NASA's History Office

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180<br />

OBSERVING THE EARTH FROM SPACE<br />

Such a vehicle is one which is located at 2•01 Earth’s radii from <strong>the</strong> Earth’s centre or<br />

about 4,000 miles from <strong>the</strong> Earth’s surface and which has a period of rotation about <strong>the</strong><br />

Earth of exactly 4 hours. If <strong>the</strong> Earth were not rotating <strong>the</strong> vehicle would move in <strong>the</strong> same<br />

meridional plane through <strong>the</strong> North and South Poles. But since <strong>the</strong> Earth does rotate as<br />

<strong>the</strong> vehicle moves, its path relative to <strong>the</strong> Earth’s surface is a series of curves.<br />

Let us assume that at noon on March 21 <strong>the</strong> vehicle is directed poleward from <strong>the</strong><br />

Equator at <strong>the</strong> 95th meridian west, at “0” hour. Assuming no external perturbations, <strong>the</strong><br />

orbit of <strong>the</strong> vehicle is always maintained in a plane parallel to its initial orbitary plane, but<br />

attached to <strong>the</strong> centre of <strong>the</strong> Earth in its motion through space. The Earth rotates under<br />

<strong>the</strong> vehicle in such a way that as <strong>the</strong> vehicle proceeds northwards, it crosses all latitudes at<br />

exactly noon and after one hour it passes over <strong>the</strong> North Pole; afterwards it <strong>the</strong>n moves<br />

southward at all latitudes at exactly midnight. At 2 hours it is at <strong>the</strong> Equator, at 3 at <strong>the</strong><br />

South Pole, after which it enters into <strong>the</strong> daylight hemisphere again crossing all latitudes<br />

at exactly noon in its northward passage. At 4 hours, it crosses <strong>the</strong> [273] Equator at <strong>the</strong><br />

155th meridian, west, and repeats a similar path on <strong>the</strong> Earth’s surface, but displaced westward<br />

from its initial path. In 24 hours it returns to its initial point of departure after having<br />

made both a daylight (noon-time) and night (midnight) surveillance of <strong>the</strong> entire<br />

Earth’s surface.<br />

Twenty minutes after its departure on its first leg, when <strong>the</strong> vehicle has moved over<br />

Amarillo, Texas, its horizon will enclose an area almost identical to <strong>the</strong> wea<strong>the</strong>r chart used<br />

in preparation of wea<strong>the</strong>r forecasts for North America and adjacent oceans.<br />

What would be seen from <strong>the</strong> vehicle at some 4,000 miles above Amarillo, Texas, at<br />

exactly noon on June 21? An attempt has been made to portray <strong>the</strong> scene below under <strong>the</strong><br />

assumption that <strong>the</strong> Sun is directly overhead. In drawing a chart before sketching in <strong>the</strong><br />

clouds, an attempt was made to indicate <strong>the</strong> surface features of <strong>the</strong> Earth, taking into<br />

account its normal colour and reflectivity (albedo) of sunlight, and <strong>the</strong> scattering and<br />

depleting effects on <strong>the</strong> passage of light through <strong>the</strong> Earth’s atmosphere in <strong>the</strong> following<br />

way:—<br />

(a) Normal illumination values at <strong>the</strong> surface were first entered in <strong>the</strong> chart according<br />

to zenith distance of <strong>the</strong> Sun.<br />

(b) Next, values of <strong>the</strong> apparent illumination or “brightness” were obtained by taking<br />

<strong>the</strong> product of <strong>the</strong> surface albedoes and <strong>the</strong> illuminations. For simplicity only two<br />

albedo figures were used: 4 per cent. for water and 15 per cent. for land. This<br />

<strong>the</strong>n gives <strong>the</strong> brightness field of <strong>the</strong> Earth before passage of <strong>the</strong> light up through<br />

<strong>the</strong> atmosphere.<br />

(c) Next <strong>the</strong> Earth’s surface brightness was computed after depletion by <strong>the</strong> atmosphere,<br />

values for which are known from <strong>the</strong> incoming sunlight.<br />

(d) Next was computed <strong>the</strong> atmospheric contribution to <strong>the</strong> brightness field at <strong>the</strong><br />

vehicle. This was done by estimating from available observations, <strong>the</strong> portion of<br />

radiation coming from <strong>the</strong> sky to <strong>the</strong> ground (i.e. <strong>the</strong> downward radiation or “skylight”)<br />

and by assuming that <strong>the</strong> same fraction of illumination is scattered<br />

upward. This procedure assumes that <strong>the</strong> atmosphere is a “uniform diffuse reflector”<br />

of <strong>the</strong> brightness shown.<br />

(e) The two brightness values—from <strong>the</strong> Earth’s surface and from <strong>the</strong> atmosphere—<br />

are added toge<strong>the</strong>r to give a total brightness.<br />

To distinguish <strong>the</strong> over-all brightness contrast between ocean and land, for example,<br />

<strong>the</strong> fractional contrast F = 2_______ BL – BO must be larger than 1/10. The computed values<br />

BL + BO of F (not shown) are considerably larger than this value, except near <strong>the</strong> periphery, indicating<br />

that for most of <strong>the</strong> observed area land can be readily distinguished from ocean.

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