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Star Ware: The Amateur Astronomer's Guide to Choosing, Buying ...

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18 <strong>Star</strong> <strong>Ware</strong><br />

Sir William Herschel, a musician who became interested in astronomy<br />

when he was given a telescope in 1722, ground some of the finest mirrors of his<br />

day. As his interest in telescopes grew, Herschel continued <strong>to</strong> refine the reflec<strong>to</strong>r<br />

by devising his own system. <strong>The</strong> Herschelian design called for the primary<br />

mirror <strong>to</strong> be tilted slightly, thereby casting the reflection <strong>to</strong>ward the front rim<br />

of the oversized tube, where the eyepiece would be mounted. <strong>The</strong> biggest<br />

advantage <strong>to</strong> this arrangement is that with no secondary mirror <strong>to</strong> block the<br />

incoming light, the telescope’s aperture is unobstructed by a second mirror;<br />

disadvantages included image dis<strong>to</strong>rtion due <strong>to</strong> the tilted optics and heat from<br />

the observer’s head. Herschel’s largest telescope was completed in 1789. <strong>The</strong><br />

metal speculum around which it was based measured 48 inches across and<br />

had a focal length of 40 feet. Records indicate that it weighed something in<br />

excess of one <strong>to</strong>n.<br />

Even this great instrument was <strong>to</strong> be eclipsed in 1845, when Lord Rosse<br />

completed the largest speculum ever made. It measured 72 inches in diameter<br />

and weighed in at an incredible 8,380 pounds. This telescope (Figure 2.7),<br />

mounted in Parsons<strong>to</strong>wn, Ireland, is famous in the annals of astronomical his<strong>to</strong>ry<br />

as the first <strong>to</strong> reveal spiral structure in what were then thought <strong>to</strong> be nebulae<br />

and are now known <strong>to</strong> be spiral galaxies.<br />

<strong>The</strong> poor reflective qualities of speculum metal, coupled with its rapid tarnishing,<br />

made it imperative <strong>to</strong> develop a new mirror-making process. That evolutionary<br />

step was taken in the following decade. <strong>The</strong> first reflec<strong>to</strong>r <strong>to</strong> use a<br />

glass mirror instead of a metal speculum was constructed in 1856 by Dr. Karl<br />

Steinheil of Germany. <strong>The</strong> mirror, which measured 4 inches across, was coated<br />

with a very thin layer of silver; the procedure for chemically bonding silver <strong>to</strong><br />

glass had been developed by Justus von Liebig about 1840. Although it apparently<br />

produced a very good image, Steinheil’s attempt received very little attention<br />

from the scientific community. <strong>The</strong> following year, Jean Foucault (crea<strong>to</strong>r<br />

of the Foucault pendulum and the Foucault mirror test procedure, among others)<br />

independently developed a silvered mirror for his astronomical telescope.<br />

He brought his instrument before the French Academy of Sciences, which<br />

immediately made his findings known <strong>to</strong> all. Foucault’s methods of working<br />

glass and testing the results elevated the reflec<strong>to</strong>r <strong>to</strong> new heights of excellence<br />

and availability.<br />

Although silver-on-glass specula proved far superior <strong>to</strong> the earlier metal<br />

versions, this new development was still not without flaws. For one thing, silver<br />

tarnished quite rapidly, although not as fast as speculum metal. <strong>The</strong> twentieth<br />

century dawned with experiments aimed <strong>to</strong> remedy the situation, which<br />

ultimately led <strong>to</strong> the process used <strong>to</strong>day of evaporating a thin film of aluminum<br />

on<strong>to</strong> glass in a vacuum chamber. Even though aluminum is not quite as highly<br />

reflective as silver, its longer useful life span more than makes up for that slight<br />

difference.<br />

Although reflec<strong>to</strong>rs do not suffer from the refrac<strong>to</strong>r’s chromatic aberration,<br />

they are anything but flawless. We have already seen how spherical aberration<br />

can destroy image integrity, but other problems must be dealt with as<br />

well. <strong>The</strong>se include coma, which describes objects away from the center of<br />

view appearing like tiny comets, with their tails aimed outward from the cen-

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