A very remarkable case concerning refraction.]

183. In all observations, to have the true altitude of the Sun, Moon, or

Stars, the refraction must be subtracted from the observed altitude. But

the quantity of refraction is not always the same at the same altitude;

because heat diminishes the air’s refractive power and density, and cold

increases both; and therefore no one table can serve precisely for the

same place at all seasons, nor even at all times of the same day; much

less for different climates: it having been observed that the horizontal

refractions are near a third part less at the Equator than at _Paris_,

as mentioned by Dr. SMITH in the 370th remark on his Optics, where the

following account is given of an extraordinary refraction of the

sun-beams by cold. “There is a famous observation of this kind made by

some _Hollanders_ that wintered in _Nova Zembla_ in the year 1596, who

were surprised to find, that after a continual night of three months,

the Sun began to rise seventeen days sooner than according to

computation, deduced from the Altitude of the Pole observed to be 76°:

which cannot otherwise be accounted for, than by an extraordinary

quantity of refraction of the Sun’s rays, passing thro’ the cold dense

air in that climate. KEPLER computes that the Sun was almost five

degrees below the Horizon when he first appeared; and consequently the

refraction of his rays was about nine times greater than it is with us.”

184. The Sun and Moon appear of an oval figure as _FCGD_, just after

their rising, and before their setting: the reason is, that the

refraction being greater in the Horizon than at any distance above it,

the lowermost limb _G_ appears more elevated than the uppermost. But

although the refraction shortens the vertical Diameter _FG_, it has no

sensible effect on the horizontal Diameter _CD_, which is all equally

elevated. When the refraction is so small as to be imperceptible, the

Sun and Moon appear perfectly round, as _AEBF_.

[Sidenote: Our imagination cannot judge rightly of the distance of

inaccessible objects.]

185. We daily observe, that the objects which appear most distinct are

generally those which are nearest to us; and consequently, when we have

nothing but our imagination to assist us in estimating of distances,

bright objects seem nearer to us than those which are less bright, or

than the same objects do when they appear less bright and worse defined,

even though their distance in both cases be the same. And as in both

cases they are seen under the same angle[44], our imagination naturally

suggests an idea of a greater distance between us and those objects

which appear fainter and worse defined than those which appear brighter

under the same Angles; especially if they be such objects as we were

never near to, and of whose real Magnitudes we can be no judges by

sight.

[Sidenote: Nor always of those which are accessible.]

186. But, it is not only in judging of the different apparent Magnitudes

of the same objects, which are better or worse defined by their being

more or less bright, that we may be deceived: for we may make a wrong

conclusion even when we view them under equal degrees of brightness, and

under equal Angles; although they be objects whose bulks we are

generally acquainted with, such as houses or trees: for proof of which,

the two following instances may suffice.

[Sidenote: The reason assigned.

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