| Mercury, 
              July/August 1998 Table of Contents 
              
 As a child I 
              recall all those evenings spent outside and away from my house and 
              its lights. At bedtime I would wander back, all the time noticing 
              how lights at the house and barn would grow in intensity, their 
              anti-darkness pouring over and enveloping the stars.   Light 
              intensity, you see, is a strong function of distance. The closer 
              you are to a source, the brighter, or more intense, that source 
              appears. Nature has even codified this effect for us as the inverse-square 
              law of light: The intensity of incident light-the amount of energy 
              received by your eye or other detector per unit area per unit time-decreases 
              as the square of the distance between you and the emitting source. 
              Floating out around Jupiter (just imagine, okay?), you'd notice 
              the Sun to be only 1/25 as bright as it appears from Earth; the 
              mighty Jovian world is just a little more than five times farther 
              from the Sun than Earth.   And 
              any source of light, be it a porch light or a star 10000 lightyears 
              away, is constrained by this dilution effect. Now, this makes things 
              a little dicey when you start comparing stars. The star second to 
              the Sun in brilliance is Sirius. It is simply impossible to ignore. 
              And while Sirius is larger than Sol, the primary reason behind its 
              brightness in our evening skies is that it's close to us.   Okay, 
              different distances lead to different perceived brightnesses, but 
              there is more. Stars have different intrinsic brightnesses. A 100 
              watt light on my porch dumps out the same energy per time as a 100 
              watt bulb on my neighbor's porch a kilometer away-her's just appears 
              dimmer because it's farther away. But stars are not like identical 
              bulbs: Their varied masses and evolutionary states result in a variety 
              of intrinsic brightnesses.   Recall 
              the magnitude system, passed down to us through a hundred generations 
              of sky watchers, as a means of quantifying stellar brightness ("Accidental 
              Astrophysics," May/June, p. 9). Bright stars have small, even negative, 
              magnitudes; faint ones, larger. This system, as I have described 
              it thus far, has a severe limitation, however. Magnitudes as we've 
              discussed them are based on how bright the stars appear to us. Sirius 
              has a magnitude of †1.46, Rigel, in neighboring Orion, shines at 
              +0.14, but the mighty Sun dominates the sky with a magnitude of 
              †26.72. With this limited information, we correctly conclude that 
              the Sun is apparently the brightest of the three stars. Here's the 
              problem, though: The Sun's intrinsic brightness is by far the lowest 
              of the three! It is brightest to us because it is so near, but compared 
              to Sirius and Rigel, it is truly dimmest.   What 
              are we to do then to extricate ourselves from this confusing situation? 
              Think of your favorite police drama, the setting a line-up room. 
              Before a white wall stand six rough-looking chaps; a police officer 
              tells them to stand with their backs to the wall. Why does the officer 
              want them at the same distance from you? What, for goodness sakes, 
              has this to do with stars? Having them at the same distance from 
              you permits you to see differences between the individuals: The 
              effect of distance, which might make a shorter person standing close 
              to you appear taller, is removed. And this is what we do with stars. 
              We put them in a line up, all at the same distance from us. Now 
              we compare the stars based on their intrinsic brightnesses.   Apparent 
              magnitude is how bright a star or quasar appears to us-what we measure 
              on a CCD image or photographic plate or estimate with our eyes. 
              As a measure of intrinsic brightness, we use absolute magnitude: 
              As in the police line-up, we imagine moving stars or other objects 
              10 parsecs away ("back against the wall, #4!") and then measuring 
              their brightness. The absolute magnitude is, therefore, the apparent 
              magnitude of an object at a distance of 10 parsecs. Recall my examples 
              Sirius, Rigel, and the Sun? Well, even though Rigel appears less 
              bright than Sirius, its absolute magnitude is actually †6.8, while 
              that of Sirius is only +1.4. And Rigel is more than 800 lightyears 
              away! It is incredible. The Sun, however, is a meager star. Its 
              apparent magnitude is an impressive †26.72, yet its absolute magnitude 
              is only +4.8. Viewing Sol from that comparison distance of 10 pc, 
              you'd see a star only slightly brighter than most of its neighbors 
              stars.   Apparent 
              magnitude is a relatively straightforward quantity to obtain. Getting 
              an absolute magnitude is a battle, one that I'll discuss in future 
              columns. But what we have so far is wonderful! Let's say we have 
              a star's apparent magnitude, and, through strenuous means, we've 
              obtained its absolute magnitude as well. What's the difference between 
              these two numbers? Yes, it is a magnitude difference, but that difference 
              is due to the distance between us and the star. Distance, yes! Magnitudes 
              have led us to a means of determining distances in outer space. 
                JAMES 
              C. WHITE II 
              is the editor of Mercury and an associate professor in the Physics 
              and Astronomy Department at Middle Tennessee State University. He 
              admits that his old brightness scale of "dim," "bright, " and "it 
              hurts," is too coarse for good astronomical research. |  |