The English works of Thomas Hobbes of Malmesbury, Volume 07 (of 11)
Thomas Hobbes · en
_B._ I confess it. Therefore I think we must take in gravity to a share
in the production of this refraction. For I never considered refraction
but in glass, because my business then was only to find the causes of
the phenomena of telescopes and microscopes. Let therefore A B (in fig.
7) be a hard, and consequently, a heavy body; and from above, as from
the sun, let C A be the line of incidence, and produced to D; and draw A
E perpendicular to A B. It is manifest that the hardness in A B shall
turn the stream of the light inwards toward A E, suppose in the line A
_e_. It is also evident that the endeavour in B, which is, being heavy,
downward, shall turn the stream again inward, towards A E, as in A _b_.
Thus it is in refraction from the sun downwards. In like manner, if the
light come from below, as from a candle in the point D, the line of
incidence will be D A, and produced will pass to C. And the resistance
of the hardness in A will turn the stream A C inward, suppose into A
_l_, and make C _l_ equal to D _e_. For passing into a thinner medium,
it will depart from the perpendicular in an angle equal to the angle D A
_e_, by which it came nearer to it in A _e_. So also the resistance of
the gravity in the point A shall turn the stream of the light into the
line A _i_, and make the angle _l_ A _i_ equal to the angle _e_ A _b_.
And thus you see in what manner, though not in what proportion, hardness
and gravity conjoin their resistance in the causing of refraction.
_A._ But you proved yesterday, that a heavy body does not gravitate upon
a body equally heavy. Now this A B has upper parts and lower parts; and
if the upper parts do not gravitate upon the lower parts, how can there
be any endeavour at all downward to contribute to the refraction?
_B._ I told you yesterday, that when a heavy body was set upon another
body heavier or harder than itself, the endeavour of it downward was
diverted another way, but not that it was extinguished. But in this
case, where it lieth upon air, the first endeavour of the lowest part
worketh downward. For neither motion nor body can be utterly
extinguished by a less than an omnipotent power. All bodies, as long as
they are bodies, are in motion one way or other, though the farther it
be communicated, so much the less.
_A._ But since you hold that motion is propagated through all bodies,
how hard or heavy soever they be, I see no cause but that all bodies
should be transparent.