An Elementary Text-book of the Microscope: including a description of the methods of preparing and mounting objects, etc.Griffith, J. W. (John William)
Science
An Elementary Text-book of the Microscope: including a description of the methods of preparing and mounting objects, etc.
Griffith, J. W. (John William)
Microscopy
If in a compound lens the chromatic aberration is only partially
corrected, so that the red rays still meet at a focus beyond the violet,
as in a simple uncorrected lens (fig. 20), the lens is said to be
under-corrected, or the aberration to be positive; while if the
correcting action of the plano-concave lens be too great, so that the
violet rays meet before the red, as in a simple concave lens, the lens
is said to be over-corrected, and the aberration is called negative.
Although the positive chromatic aberration of the extreme rays passing
through a convex lens may be corrected by the negative aberration of a
concave lens, there still remains a certain amount of uncorrected
colour, arising from the irrationality of the spectra of the two
refracting media. This evil cannot be overcome, and the remaining colour
is said to arise from the secondary spectrum.
The object-glasses of the microscope, consisting of the compound lenses,
have their aberrations balanced to a considerable extent on the above
principles--the lowest combination being under-corrected, while the
upper combinations are over-corrected; and, by suitable adaptation of
their distance from each other, further correction may be obtained, the
aberration of the object-glass altogether being, however, over-corrected
or negative.
The eye-piece consists of two simple plano-convex lenses, the upper or
eye-glass (fig. 27 _e_) having a shorter focus than the lower (_f_) or
field-glass, and the two placed at the distance of half the sum of their
focal lengths. The object-glass alone would form an enlarged and
reversed image of the object within the body of the microscope, the
cones of rays from each point of the object terminating at the larger
arrows in the figure (fig. 27). But the rays meeting the field-glass are
brought by it to a focus at the position of the smaller arrows, where
they form a reduced image; and, subsequently passing through the
eye-glass, they are so altered in direction as to enter the eye at a
greater angle, and to present a magnified image of the object.
The eye-piece produces several important effects. The refraction being
produced by two less convex lenses instead of one of greater convexity,
the spherical aberration is considerably reduced; and the convexities
of the lenses in the eye-piece being situated in an opposite direction
to that of those in the object-glass, the spherical aberration of the
former reverses and so neutralizes that of the latter. Also the
under-correction of the field-glass compensates the over-correction of
the object-glass--the blue rays which are refracted more than the red by
the field-glass, being thrown upon the eye-glass nearer its centre,
where the refraction is less, and thus the coloured rays become parallel
or nearly so on reaching the eye. Moreover the field-glass collects a
larger number of rays than the eye-glass could do alone, so that it
enlarges the field and increases its brightness.
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Elsewhere in the archive
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account