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The Normal (Emmetropic) Eye
An eyeglass lens supplements the eye. It helps the eye perform
functions that the eye cannot do itself. Therefore, to understand
the function of lenses, you must understand how the normal eye
works. Figure 3-1 shows the parts of the normal, or emmetropic
(em i TROP ic), eye. Study it carefully before you proceed.

Figure 3-1 The
Normal Emmetropic Eye
Figure 3-1 also shows light as it enters the eye from distant
objects. Rays of light from distant objects proceed to the eye along
parallel lines. When they reach the eye they are bent, or refracted,
by the cornea. These rays of light are refracted even further by the
crystalline lens, and are sharply focused on the retina at the back
of the eye.
The Farsighted Eye
There are a variety of reasons why light will not focus precisely on
the retina. Some of these reasons have to do with the shape of the
eyeball itself. For example, people who have little problem with
distance vision, but do have problems close-up are called far-sighted,
or hyperopes (HY pe rop). The hyperopic (hy per O pik)
eye may be thought of as an optically weak power system. The
result is that light comes to a focus behind the retina, causing an
image to blur. This problem is illustrated in Figure
3-2.

Figure 3-2 The
Farsighted Eye
Figure 3-3 shows an eye which has been corrected for hyperopia
(hi pe RO pe a) by adding a converging lens. The lens adds convergence
to the optical system of the eye by redirecting the focus of
the light forward to the retina to produce a clear image. Converging
lenses are also called convex, or plus, lenses. With the normal
accommodation of the crystalline lens, and the help of the corrective
lens, the eye can now focus clearly upon near and distant
objects with little eye strain.

Figure 3-3 The
Farsighted Eye - Corrected
The Nearsighted Eye
The other common condition which causes blurred vision is
near-sightedness,
or myopia (mi O pe a). The nearsighted eye may be
considered to be optically too strong to allow light to focus on the
retina. The nearsighted eye is shown in Figure
3-4.

Figure 3-4 The
Nearsighted Eye
Although a nearsighted person may be able to see clearly objects
held close to the eye, objects in the distance will appear blurred.
Nearsightedness is corrected using a diverging lens (concave or
minus) as shown in Figure
3-5. The diverging lens spreads the rays
of light farther apart so that they converge on the retina rather
than in front of it.

Figure 3-5 The
Nearsighted Eye Corrected
Astigmatism
Up to this point, the lenses in our sample eyeballs have been
spherical in nature. Spherical lenses have the same curvature in
all directions. However, it is not uncommon for the cornea of the
eye to have slightly varying curvature. This produces a condition
called astigmatism (a STIG ma tism) which cannot be corrected
with a simple spherical eyeglass lens. The uncorrected eye of a
patient with astigmatism will not bring light rays to a sharp,
well-defined focus on the retina, Figure
3-6. Objects may appear out of focus
differently
at right angles.
To correct for astigmatism, a cylindrical surface is ground with a
spherical surface to produce a lens with maximum and minimum
refractive powers 90 degrees from each other. This
sphero-cylinder
lens, when properly oriented before the eye, will cancel the
eye’s
astigmatic refractive power error.

Figure 3-6
Astigmatism
Presbyopia
The two lens types considered so far produce a correction
primarily
for distant objects. Such lenses are called single-vision lenses. They rely upon the eye’s own crystalline lens to produce clear
images of near objects.
The crystalline lens may be stretched or relaxed by the eye
muscles. This process is called accommodation. Accommodation
allows the normal eye to produce clear images on the retina of
objects that are relatively near to the eye as well as those that are
distant. The process works in much the same way as the focusing
action of a camera.
As people approach middle age, their crystalline lenses lose some
elasticity and they begin to have difficulty focusing on books,
newspapers, etc. This condition is called Presbyopia (prez be O pe a).
To solve this condition, lenses with more than one viewing range
are used. These lenses are called bifocals, trifocals, progressives,
or,
more generally, multifocals (Figure 3-7). A bifocal lens is really two
lenses combined into one. The lens provides a distance-viewing
area and a near-viewing area. A trifocal provides three viewing
areas: distance, intermediate and near. A progressive lens provides
a continuous increase in lens power as the eye moves down from
the distance viewing to the near viewing range. Progressive lenses
are sometimes called "no-line" bifocals. You will learn more
about
lenses in another unit of this course.

Figure 3-7
Bifocal, Trifocal and Progressive Lenses
Review of Simple Lenses
Figure 3-8 is an illustration of a plus lens, also called a converging
lens, because in hyperopes it causes light to converge to a point on
the retina rather than behind it.

Figure 3-8
The Plus (Converging) Lens
The Spherical (Minus)
The minus lens causes light to diverge. Remember, the minus lens
is used for people who are nearsighted. The light rays are pushed
apart (diverged) so that they focus upon the retina rather than in
front. Figure 3-9 shows a spherical minus lens. See how parallel
light rays are pushed apart.

Figure 3-9 The
Minus (Diverging) Lens
In order to make ophthalmic lenses more optically correct, and
more attractive, their outside surfaces are made convex and their
inside surfaces are made concave. See Figure 3-10, Modern Lens
Form.

Figure 3-10
Modern Lens Form
Sphero-cylinder Lens
The lens to correct astigmatism is sometimes called a
sphero-cylinder. The front surface is spherical while the back surface is
cylindrical. This combination of front and back surfaces creates a
lens prescription of spherical power with a cylinder amount
ground on the back surface to correct the two focus points created
by the astigmatism. The cylinder amount on the back surface is
ground in the required position, called the axis. Figure 3-11 shows
a sphero-cylinder lens.

Figure 3-11 Sphero-cylinder Lens
Astigmatism Corrected
Index of Refraction
The subject of index of refraction is complex and will only be
introduced here. It will be covered in more detail in the course
which deals with surface room operations. For now, simply remember
that the four quantities which control the refractive power of
an ophthalmic lens are:
• the curvature of the front surface (closest to the object being
viewed);
• the curvature of the rear surface (closest to the eye);
• index of refraction of the material from which the lens is
made;
and
• the thickness of the lens.
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