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| United States Patent | 4324461 |
| Link to this page | http://www.wikipatents.com/4324461.html |
| Inventor(s) | Salvatori; Anthony L. (Sarasota, FL) |
| Abstract | A contact lens for the correction of astigmatism or presbyopia and for the
correction of "high riding" lenses being of lenticular construction. This
invention avoids unwanted increase in center thickness of the lens and
unwanted prism in the central area. The curved lenticular carrier portion
of the lens, the non-visual portion, is constructed with a concentric
curve cut which produces a thick lens edge. The lenticular carrier is also
provided with a second eccentric curve cut, with respect to the visual
axis of the lens, to provide a thickness disparity between the superior
and inferior portions of the lens and to provide an offset center of
gravity and a desirable rotational positioning of the lens in the eye of a
wearer, particularly when the lens is of astigmatic or bifocal type. |
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Title Information  |
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Drawing from US Patent 4324461 |
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Contact lens for non-rotational orientation |
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| Publication Date |
April 13, 1982 |
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| Filing Date |
November 26, 1979 |
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Title Information  |
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Claims  |
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What is claimed is:
1. A contact lens for non-rotational orientation in the eye of a wearer,
comprising a substantially circular lenticular carrier having a central
concentric optical portion surrounded by a generally annular non-visual
portion, and said non-visual portion having a thicker part at the lower
part of said lenticular carrier when in the eye of a wearer and having a
thinner part at the upper part of said lenticular carrier when in the eye
of a wearer, there being no additional prism in the optical lens area.
2. A contact lens for non-rotational orientation in the eye of a wearer as
defined in claim 1, wherein said optical portion contains a
sphero-cylindrical correction for the eye, whereby said thicker portion of
said lenticular carrier prevents rotational movement of said lens in the
eye of a wearer.
3. A contact lens for non-rotational orientation in the eye of a wearer as
defined in claim 1, wherein said optical portion has a central circular
zone powered on the anterior surface for distance vision thereof and has
an annular zone surrounding said circular zone powered for near vision
with respect to the cornea of the eye of a wearer, whereby said thicker
portion of said lenticular carrier serves to allow vertical displacement
of said power zones without unwanted prism in said optical portion.
4. A contact lens for non-rotational orientation in the eye of a wearer as
defined in claim 1, wherein said optical portion has an upper optical zone
powered on the anterior surface for distance vision thereof with respect
to the cornea of the eye of a wearer, and said optical portion has a lower
optical zone powered on the anterior surface for near vision with respect
to the cornea of the eye of a wearer as customary in bifocal lenses,
whereby said thicker portion of said lenticular carrier serves to maintain
said upper and lower optical zones in the proper position relative to the
cornea of the eye of a wearer, without unwanted prism in said optical
portion.
5. A contact lens for non-rotational orientation in the eye of the wearer
as defined in claim 1 wherein said optical portions contain a sphere
correction for the eye whereby said thicker portion of said lenticular
carrier provides a downward weight imbalance to correct "high riding"
lenses. |
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Claims  |
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Description  |
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FIELD OF THE INVENTION
This invention relates to optic article shaping or treating, especially to
provide an astigmatic and multifocal type of contact lens or blank.
DESCRIPTION OF THE PRIOR ART
Other types of contact lenses for the correction of astigmatism or
presbyopia are well-known. They employ various designs for maintaining
non-rotational positioning. For example: A non-rotational position can be
achieved by truncating the lens horizontally. In another method, the
periphery of the lens is shaped eccentrically. In still another, more
common, method the lens is constructed with prism ballast. Lenses of this
type do not form a part of the present invention.
With the advent of soft contact lenses, greatly increased use of contact
lenses has occurred. Up until the present time, both hard and soft contact
lenses for the correction of astigmatism or presbyopia have used one or
more of the aforementioned methods to maintain non-rotational positioning.
Each of these methods has known drawbacks. As an example: When a lens is
truncated, it frequently becomes dislodged from the eye with eye
movements. In another type, where the periphery of the lens is shaped
eccentrically, the lens frequently decenters downward causing a visual
disparity between the optical axis of the lens and the visual axis. In the
prism balast which is by far the more popular type, additional lens
thickness is required over the thickness necessary for the prescription
itself without prism.
This is a very important drawback since plastic materials today are
formulated with the main thought of supplying more oxygen to the cornea to
maintain the cornea's normal metabolism. As an example: Cellulose acetate
butyrate is gaining widespread use as a hard contact lens material over
PMMA, poly methyl methacrylate, because of its increased oxygen
transmission. In soft lenses, HEMA, hydroxy ethyl methacrylate, lenses
transmit more oxygen depending on the water contant of the material and
lens thickness. However, where these materials are constructed in
non-rotational lenses for the correction of astigmatism or presbyopia, in
the prior art added center thickness is required for the more popular
prism ballast construction.
Other ballast type lenses are shown in the following U.S. Pat. Nos.:
3,279,878; 3,339,997; 3,431,327; 3,962,505 and 4,071,293.
SUMMARY OF THE INVENTION
It is well-known that the effect of added thickness has an adverse effect
on oxygen transmission and that this added thickness can negate the
increased oxygen transmission of the material. For the foregoing reason
and for other reasons and because of the shortcomings of certain prior art
constructions in fulfilling the desired characteristics of non-rotating
lenses for the correction of astigmatism or presbyopia, it is the object
of the present invention to provide an improved nonrotating contact lens
characterized by constructing the lens to provide non-rotational
positioning and provide thickness throughout the optical zone equal to the
center thickness of spherical or single vision lenses. This is
accomplished by cutting the lenticular carrier for the lens arcuately at
the top to provide a thin structure there, and providing an arcuate
thicker section at the bottom.
A further object is to maintain coincidence between the optical center of
the lens and the optical center of the visual axis.
A further object is to maintain the periphery of the lens geometrically
centered with the optical zone.
A further object is to provide a non-rotating lens with the means for
vertical displacement when bivisual or bifocal construction is required
for presbyopia.
A further object of this invention is to provide a solution to a common
problem of "high riding lenses". Quite often because of the irregular
shape of the eye and/or the configuration of the lids, a contact lens will
fix itself superiorly. The common solution is to introduce prism in the
prescription to create a downward weight imbalance. In the present
invention, this problem is readily solved without unwanted increase in
center thickness and without unwanted prism in the visual area.
Although the principles of the present invention are applicable to a
variety of optical devices, the invention will be described with reference
to non-rotating contact lenses for the correction of astigmatism or
bifocal use and constructed of any material suitable to be worn on the
eye.
It is not the intention here to describe the methods used to produce
astigmatic or presbyopic lenses. The methods are well-known to those
versed in the art.
BRIEF DESCRIPTION OF THE DRAWINGS
Referring now to the drawings:
FIG. 1 shows a front plan view of one embodiment;
FIG. 2 shows a side elevational view taken on line 2--2 of FIG. 1 showing
the present invention in minus power form;
FIG. 3 shows a side elevational view showing this invention in plus power
form;
FIG. 4 shows a front plan view of the present invention in common bifocal
form;
FIG. 5 is a side elevational view taken on the line 5--5 of FIG. 4;
FIG. 6 shows a front plan view of the present invention in annular bifocal
form;
FIG. 7 is a side elevational view taken along the line 7--7 of FIG. 6.
Referring now to FIG. 1 in which this invention is constructed in sphere or
sphero-cylinder form, the lens is first constructed with a minus 13.00 D
lenticular carrier in an annulus 11 completely around the lens area 10
although any power carrier can be used that will give a thickness
equivalent to the amount of ballast desired. Normally, the amount of
thickness at the edge, marked "BALLAST" in FIGS. 1, 4 and 6, is equivalent
to one to two diopters of prism although, in practice, we have found that
the center of gravity in this invention is lower than prism ballast lenses
and requires less prism effect. The lens is then placed eccentrically so
the vertical axis 12 of the lens has its upper end opposite the desired
lower portion with respect to the viewer.
Next, an area 13 of shorter curvature (for instance, a -3.00 D) is cut in
the lenticular carrier outside the lens area and cutting the upper portion
of the previously constructed annulus as seen at 13a in FIGS. 2 and 3, to
provide a thinner area of the carrier in a crescent shape extending from a
widest portion 13a on said axis occupying a major portion of said annulus
outside said lens area, and extending at 13b about both sides of said
annulus downwardly so that said crescent shape terminates toward the lower
portion of said annulus, thus producing the configuration referred to in
FIG. 1 as "slab-off". This produces a thickness disparity in the carrier
portion of the lens and lowers the center of gravity allowing for a
pendulum effect for the lens to orientate to a fixed position with the
lens axis vertical.
The lenticular carrier is about 0.05 mm to 0.10 mm thick at the upper edge
14, shown in the drawings, so that the eyelid of a wearer will easily
slide down over the lens edge 14.
It is understood that the amount of eccentric displacement and curvature
used to produce the "slab-off" is interrelated and both these functions
can be varied to achieve the most desirable lens configuration.
As an example: The more the lens is displaced eccentrically, a flatter
curvature can be used for the "slab-off". Conversely, the less the lens is
displaced eccentrically the steeper the curve for the "slab-off" to
achieve the same effect as in the foregoing example.
In FIGS. 6 and 7, the same lenticular carrier surrounds a bifocal lens 16
of target type, having a central portion 16a for distance vision
surrounded by an annular portion 16b for reading vision. The portions 16
and 16b would fit the patient's prescription.
In FIGS. 4 and 6 the principal axis of vision is 12 which is also the
vertical center line of the lenticular carrier.
Example of thickness saving: If we consider two lenses of the same
characteristics--one of the present invention and one of prism ballast
construction, it can be shown that a 33% savings in center thickness is
achieved by the present invention.
Consider in the present invention lens characteristics of:
7.00 mm base curve
+5.00-2.00 astigmatic and/or +3.00 +2.00 bifocal
7.50 mm optical zone
0.10 mm optical zone thickness
In FIGS. 4 and 5 there is shown an embodiment of a lenticular carrier
having a heavier "ballast" area and a lighter "slab-off" area, as
described in FIGS. 1, 2 and 3, surrounding a bifocal lens 15 of known
character, having a portion 15a for distance vision which might be between
+20.00 to -20.00 diopters, and having an add portion 15b for reading
vision which might be anywhere between +1.00 to +3.50 diopters.
By the formula (Creighton's contact lens tables), when S=sagittal depth,
r+radius, and D=lens diameter,
##EQU1##
it can be found that in order to obtain a 0.10 mm optical zone juncture
thickness, the center thickness will be 0.18 mm.
##EQU2##
Base curve or posterior curve of lens is 7.00 mm.
##EQU3##
Therefore, because the power curve is steeper than the base curve, we know
that 1.17-1.089=0.081 the difference between the sagittal of power curve
and sagittal of base curve gives us the center thickness 0.08 mm when the
edge is at 0. Therefore, if you wanted a juncture thickness of 0.10 mm the
center would have to be 0.18 mm thick.
Using the same example, if you were going to incorporate prism we would use
the prism formula
##EQU4##
where
T is thickness of the base of the prism in mm
d is the diameter
P is the prism added
##EQU5##
Therefore, one-half of this thickness would give the center thickness of
0.0765 or about 0.08 mm. This would have to be added to the thickness
calculated above 0.18 which plus 0.08=0.26 mm which is a greater center
thickness. Thus we find that center thickness must be increased by 0.08
mm, in which case this lens will have a center thickness of 0.26 mm.
The present invention saves considerable thickness and provides a
considerable increase in oxygen transmission for a given lens material.
According to Fick's Law of Diffusion where
J=(DK/L) .DELTA.p
DK=lens permeability
L=lens thickness
it follows that either a large "DK" or a small "L" will result in higher
oxygen transmission (DK/L).
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Description  |
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