Account of the Skerryvore lighthouse : $b with notes on the illumination of lighthousesStevenson, Alan
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Account of the Skerryvore lighthouse : $b with notes on the illumination of lighthouses
Stevenson, Alan
Skerryvore Lighthouse (Hebrides, Scotland)
The tests generally applied for examining the lenses used in
Lighthouses, is to find the position of the conjugate focus _behind_
the lens, due to a given position of a lamp in _front_ of it. This
test depends on the following considerations:--Draw a line from an
object O in front of a lens, to any point Q in the lens; and from A,
the centre of the lens, draw AR parallel to OQ, and cutting a line
RF _r_ which passes through the principal focus F, at right angles
to the axis of the lens; then join the points Q and R, and produce
the line joining them: I, the image of O must be in that line. In
the same way, draw a line from O to _q_, another point in the lens
on the other side of its axis, and parallel to it draw A _r_ from
the centre of the lens, cutting the plane of the principal focus in
_r_. Join _q_ _r_, in which line the image will lie; and hence the
intersection of OR and _q_ _r_, in I, will be the point in which the
image of O is formed, or will be the conjugate focus of the lens due
to the distance OA. This mode will serve to give the distance of
the conjugate focus of a lens (_neglecting its thickness_) for rays
falling on its surface at any angle.
[Illustration: Fig. 61.]
We shall suppose QA (fig. 61) to represent the half of a lens, and
remembering the conditions described in reference to the last figure,
we shall at once perceive the truth of the following analogy (fig.
62):--
[Illustration: Fig. 62.]
OA ∶ AF ∷ AQ ∶ FR ∷ AI ∶ FI, and putting OA = δ, AI = φ′, and AF
= φ, we have δ ∶ φ ∷ φ′ ∶ φ′ - φ, and, consequently, δ φ′ - δ φ =
φ φ′; and hence the following equations, which express the relations
subsisting between the principal focus of the lens and the distance
of any object and its corresponding image:
1_st_, To find the principal focal distance of a lens from the
measured position of its object and its image refracted through it,
we have,
δ φ′
φ = ------.
δ + φ′
2_d_, For the distance of the object, when that of the image is
known, we have,
φ φ′
δ = ------.
φ′ - φ
3_d_, For the position of the image, when that of the object is
known, we have,
δ φ
φ′ = -----.
δ - φ
[Illustration: Fig. 63.]
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