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CHAPTER 7 • Astronomical Control of Solar Radiation  123


                                                            today. Leverrier discovered these variations in the
                                                            1840s. The shape of an ellipse can be described by ref-
                           Tilt
                                                            erence to its two main axes: the “major” (or longer) axis
                      22˚ 23˚ 24˚                           and the “minor” (or shorter) axis (Figure 7-6). The
                     0.0
                                                            degree of departure from a perfectly circular orbit can
                                       One                  be described by
                                    41,000–year
                                       cycle                                        2  2
                                                                                   ————
                                                                                   a – b
                                                                                 = ––––––
                                                                                    a
                     0.5
                                                            where   is the eccentricity of the ellipse and a and b are
                   Myr ago                                  half of the lengths of the major and minor axes (called
                                                            the “semimajor” and “semiminor” axes).
                                                               The eccentricity of the elliptical orbit increases as
                                                            these two axes become more unequal in length. At
                     1.0
                                                            the extreme where the two axes become exactly equal
                                                            (a = b), the eccentricity drops to zero because the orbit
                                                                       2
                                                            is circular (a – b = 0). Eccentricity ( ) has varied over
                                                                          2
                                                            time between values of 0.005 and 0.0607 (Figure 7-7).
                                                            The present value (0.0167) lies toward the lower (more
                     1.5                                    circular) end of the range.
                                                               Changes in orbital eccentricity are concentrated
                                                            mainly at two periods. One eccentricity cycle shows up
        FIGURE 7-4 Long-term changes in tilt Changes in the tilt  as variations at intervals near 100,000 years (see Figure
        of Earth’s axis have occurred at a regular 41,000-year cycle.  7-7). This cycle actually consists of four cycles of nearly
                                                            equal strength and periods ranging between 95,000 and
                                                            131,000 years, but these cycles blend into a cycle near
           Decreases in tilt have the opposite effect: they  100,000 years.
        diminish the amplitude of seasonal differences. Smaller  The second eccentricity cycle has a wavelength of
        tilt angles put the Earth slightly closer to the configura-  413,000 years. This longer cycle is not as obvious, but it
        tion shown in Figure 7-3A, which has no seasonal    shows up as alternations of the 100,000-year cycles
        differences at all.
                                                            between larger and smaller peak values. Larger ampli-
                                                            tudes can be seen near 200,000, 600,000, 1,000,000, and
          IN SUMMARY, changes in tilt mainly amplify or     1,400,000 years ago (see Figure 7-7). A third eccentric-
          suppress the seasons, particularly at the poles.
                                                            ity cycle also exists at a period of 2.1 Myr, but this cycle
                                                            is much weaker in amplitude.
        7-4 Changes in Earth’s Eccentric Orbit through Time

        The shape of Earth’s orbit around the Sun has also var-
        ied in the past, becoming at times more circular and at
        other times more elliptical (or “eccentric”) than it is


                                                                                      b
             Summer                          Winter
             June 21                      December 21
                  N                              N
                                                                                             a




              S                             S
                                                                                     2
                                                                                  2
              Winter                        Summer                              (a – b ) 1 / 2
                                                                   Eccentricity ε =  a
        FIGURE 7-5 Effects of increased tilt on polar regions  FIGURE 7-6 Eccentricity of an ellipse The eccentricity of
        Increased tilt brings more solar radiation to the two summer  an ellipse is related to half of the lengths of its longer (major)
        season poles and less radiation to the two winter season poles.  and shorter (minor) axes.
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