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Project Cyclops, A Design... - Department of Earth and Planetary ...

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MAIN SEQUENCE SPECTRAL CLASS<br />

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GIANTS<br />

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MAIN<br />

SEQUENCE<br />

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MASS, SOIOrmosses<br />

Figure 2-4. The mass-luminosity relation.<br />

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SURFACE TEMPERATURE, °KxIO 3<br />

Luminosity Function. This is the generic term applied to<br />

the distribution <strong>of</strong> number <strong>of</strong> stars per unit volume <strong>of</strong><br />

space versus their luminosity or absolute magnitude. The<br />

observed distribution is shown in Figure 2-5. At the high<br />

Figure 2-3. The Hertzsprung-Russell (HR ) diagram.<br />

10 5 - _ ] l r<br />

The significant feature <strong>of</strong> the HR diagram is that<br />

almost all stars fall into the four shaded areas shown.<br />

This grouping indicates a restricted set <strong>of</strong> relationships<br />

between luminosity, temperature, <strong>and</strong> radiusrelationships<br />

that are now understood to represent<br />

different epochs in the life <strong>of</strong> a star. The main sequence<br />

accounts for _bout 90 percent <strong>of</strong> all stars, giants <strong>and</strong><br />

supergiants [or about 1 percent, <strong>and</strong> white dwarfs for<br />

about 9 percent. (see Appendix A).<br />

Mass-Luminosity Relation. The masses <strong>of</strong> binary stars<br />

can be determined by applying Newton's derivation <strong>of</strong><br />

Kepler's Third Law relating mass, mean separation, <strong>and</strong><br />

orbital period. If the luminosities <strong>of</strong> the stars are plotted<br />

against their masses, determined in this way, the<br />

distribution shown in Figure 2-4 is found for main<br />

sequence stars. The stars shown in this plot have the<br />

usual spread <strong>of</strong> chemical composition associated with<br />

different ages <strong>and</strong> populations. Nevertheless, the points<br />

do not depart very far from the dashed line. This<br />

indicates that the luminosity <strong>of</strong> a main sequence star is<br />

determined primarily by its mass. Although the true<br />

relation is more complicated, we can approximate it<br />

quite well over most <strong>of</strong> the range by the simple<br />

expression:<br />

i0 1 I I J I<br />

0 5 _0 15 20<br />

ABSOLUTE MAGNITUDE<br />

Figure 2-5. The luminosity ]im('ti(m

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