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The ferrotype and how to make it - The Grian Press

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156 THE FERROTYPE. ^<br />

At last, placing my glass where there happened<br />

<strong>to</strong> be a stronger light reflected from <strong>it</strong>s surface,<br />

I found, in a double reflection, the cause of all<br />

my troubles. <strong>The</strong> glass of the mirror <strong>and</strong> also<br />

of the small reflec<strong>to</strong>r being of very thick plate,<br />

<strong>it</strong> gave a reflection from both surfaces—from the<br />

front surface of the glass <strong>and</strong> from the silvered<br />

back surface. Of course, the reflection from the<br />

front or outer surface was faint, <strong>and</strong> only per-<br />

ceptible in the double outlines; yet, by no means<br />

at my comm<strong>and</strong>, could I remove or prevent <strong>it</strong><br />

in consequence, I was forced <strong>to</strong> give up the mir-<br />

ror <strong>and</strong> glass reflec<strong>to</strong>r. My attention was next<br />

turned <strong>to</strong> a finely-polished metallic reflecting<br />

surface, but w<strong>it</strong>h no better success— in conse-<br />

quence, I think, of the difficulty, if not the im-<br />

possibil<strong>it</strong>y, of securing a perfectly plain surface<br />

by which I mean a surface so perfectly even <strong>and</strong><br />

level as <strong>to</strong> reflect all rays of light in a direction<br />

exactly parallel. It will very easily be seen that<br />

any inequal<strong>it</strong>y, <strong>how</strong>ever small, in the reflecting<br />

surface, would destroy the image: <strong>and</strong> this I<br />

found impossible <strong>to</strong> overcome : <strong>and</strong> although I<br />

had been very sanguine when I first attempted<br />

the metallic reflec<strong>to</strong>r, I was forced <strong>to</strong> give <strong>it</strong> up<br />

as unsu<strong>it</strong>able or unf<strong>it</strong> for the purpose.<br />

<strong>The</strong> image reflected by one of these instruments<br />

would often be so blurred as <strong>to</strong> be undistinguish-<br />

able ; again, parts of the image would be perfect,<br />

but not all. This resulted, I found, from the<br />

inequal<strong>it</strong>ies of the metallic surface—such inequal-<br />

:

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