The Works of George Berkeley. Vol. 1 of 4: Philosophical Works, 1705-21Berkeley, George
Philosophy
The Works of George Berkeley. Vol. 1 of 4: Philosophical Works, 1705-21
Berkeley, George
Philosophy -- Early works to 1800
35. _Secondly_, Suppose, in the adjacent figures, _NP_ represent an eye
duly framed, and retaining its natural figure. In fig. 1 the rays falling
nearly parallel on the eye, are, by the crystalline _AB_, refracted, so as
their focus, or point of union _F_, falls exactly on the retina. But, if
the rays fall sensibly diverging on the eye, as in fig. 2, then their
focus falls beyond the retina; or, if the rays are made to converge by the
lens _QS_, before they come at the eye, as in fig. 3, their focus _F_ will
fall before the retina. In which two last cases it is evident, from the
foregoing section, that the appearance of the point _Z_ is confused. And,
by how much the greater is the convergency or divergency of the rays
falling on the pupil, by so much the farther will the point of their
reunion be from the retina, either before or behind it, and consequently
the point _Z_ will appear by so much the more confused. And this, by the
bye, may shew us the difference between confused and faint vision.
Confused vision is, when the rays proceeding from each distinct point of
the object are not accurately re-collected in one corresponding point on
the retina, but take up some space thereon—so that rays from different
points become mixed and confused together. This is opposed to a distinct
vision, and attends near objects. Faint vision is when, by reason of the
distance of the object, or grossness of the interjacent medium, few rays
arrive from the object to the eye. This is opposed to vigorous or clear
vision, and attends remote objects. But to return.
36. The eye, or (to speak truly) the mind, perceiving only the confusion
itself, without ever considering the cause from which it proceeds, doth
constantly annex the same degree of distance to the same degree of
confusion. Whether that confusion be occasioned by converging or by
diverging rays it matters not. Whence it follows that the eye, viewing the
object _Z_ through the glass _QS_ (which by refraction causeth the rays
_ZQ_, _ZS_, &c. to converge), should judge it to be at such a nearness, at
which, if it were placed, it would radiate on the eye, with rays diverging
to that degree as would produce the same confusion which is now produced
by converging rays, i.e. would cover a portion of the retina equal to
_DC._ (Vid. fig. 3, _sup._) But then this must be understood (to use Dr.
Barrow’s phrase) “seclusis prænotionibus et præjudiciis,” in case we
abstract from all other circumstances of vision, such as the figure, size,
faintness, &c. of the visible objects—all which do ordinarily concur to
form our idea of distance, the mind having, by frequent experience,
observed their several sorts or degrees to be connected with various
distances.
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