ess refracting Power. For in the Confine of Air and Sal-gem 'tis
stronger than in the Confine of Air and Water, and still stronger in the
Confine of Air and common Glass or Crystal, and stronger in the Confine
of Air and a Diamond. If any of these, and such like transparent Solids,
be immerged in Water, its Reflexion becomes, much weaker than before;
and still weaker if they be immerged in the more strongly refracting
Liquors of well rectified Oil of Vitriol or Spirit of Turpentine. If
Water be distinguish'd into two parts by any imaginary Surface, the
Reflexion in the Confine of those two parts is none at all. In the
Confine of Water and Ice 'tis very little; in that of Water and Oil 'tis
something greater; in that of Water and Sal-gem still greater; and in
that of Water and Glass, or Crystal or other denser Substances still
greater, accordingly as those Mediums differ more or less in their
refracting Powers. Hence in the Confine of common Glass and Crystal,
there ought to be a weak Reflexion, and a stronger Reflexion in the
Confine of common and metalline Glass; though I have not yet tried
this. But in the Confine of two Glasses of equal density, there is not
any sensible Reflexion; as was shewn in the first Observation. And the
same may be understood of the Superficies interceding two Crystals, or
two Liquors, or any other Substances in which no Refraction is caused.
So then the reason why uniform pellucid Mediums (such as Water, Glass,
or Crystal,) have no sensible Reflexion but in their external
Superficies, where they are adjacent to other Mediums of a different
density, is because all their contiguous parts have one and the same
degree of density.

PROP. II.

_The least parts of almost all natural Bodies are in some measure
transparent: And the Opacity of those Bodies ariseth from the multitude
of Reflexions caused in their internal Parts._

That this is so has been observed by others, and will easily be granted
by them that have been conversant with Microscopes. And it may be also
tried by applying any substance to a hole through which some Light is
immitted into a dark Room. For how opake soever that Substance may seem
in the open Air, it will by that means appear very manifestly
transparent, if it be of a sufficient thinness. Only white metalline
Bodies must be excepted, which by reason of their excessive density seem
to reflect almost all the Light incident on their first Superficies;
unless by solution