JPS601604B2 - eyeglass lenses for astigmatism - Google Patents
eyeglass lenses for astigmatismInfo
- Publication number
- JPS601604B2 JPS601604B2 JP3906078A JP3906078A JPS601604B2 JP S601604 B2 JPS601604 B2 JP S601604B2 JP 3906078 A JP3906078 A JP 3906078A JP 3906078 A JP3906078 A JP 3906078A JP S601604 B2 JPS601604 B2 JP S601604B2
- Authority
- JP
- Japan
- Prior art keywords
- lens
- astigmatism
- value
- degree
- tables
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Expired
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- Eyeglasses (AREA)
Description
【発明の詳細な説明】
本発明は、乱視用眼鏡レンズの外面及び内面の両面をト
リック面にすることにより、面形状決定の自由度を増し
、鞄外の乱視度が軸上の乱視度に等しくなるように収差
の改善をはかったものである。DETAILED DESCRIPTION OF THE INVENTION The present invention increases the degree of freedom in determining the surface shape by making both the outer and inner surfaces of the spectacle lens for astigmatism into trick surfaces, and the degree of astigmatism outside the bag becomes the degree of astigmatism on the axis. This is an attempt to improve aberrations so that they are equal.
従来より、外面または内面のどちらか一方の面をトリッ
ク面として、その面形状を適当に設定することにより、
収差特に乱視度に対応する非点収差の改善をはかったも
のが考えられている。Conventionally, by setting either the outer or inner surface as a trick surface and appropriately setting the surface shape,
There are plans to improve aberrations, especially astigmatism, which corresponds to astigmatism.
例えば一面をトリック面、他の面を球面として軸外の妥
当な角度(眼鏡レンズにおいては有効視野等の関係から
通常30o近傍を補正角とする)における二つの主経線
方向の非点収差(乱視度)の値を等しくする、いわゆる
Equal−偽tigmatismの条件を満足するよ
うにレンズの面形状を設定することが可能である。この
ようにして面形状を設定することによりEq雌1一As
tigmatSmの条件を満足する補正角度のレンズ論
帯状の部分においては、ほぼ等しい乱視度が得られるが
、残念ながらこの乱視度の値は、かならずしもこのレン
ズの正規の乱視度である軸上及びその近傍の乱視度の値
に等しくならない。For example, one surface is a trick surface and the other surface is a spherical surface, and astigmatism (astigmatism) in the two principal meridian directions is corrected at a reasonable off-axis angle (for eyeglass lenses, the correction angle is usually around 30 degrees due to the effective field of view, etc.). It is possible to set the surface shape of the lens so as to satisfy the condition of so-called Equal-false tigmatism, which equalizes the values of the chromaticity (power). By setting the surface shape in this way, Eq female 11 As
A lens with a correction angle that satisfies the condition of tigmatSm In the belt-shaped part, approximately the same degree of astigmatism can be obtained, but unfortunately, the value of this degree of astigmatism is not always on the axis and its vicinity, which is the normal degree of astigmatism of this lens. is not equal to the astigmatism value.
これを実例で示すと、表1、表2のようになる。表1、
2より明らかなように、補正角30o及びその近傍の乱
視度の値は、内面トリックにおいては負レンズの弱度部
分及び正しンズ全体、外面トリックにおいては負レンズ
及び正しンズ全体にわたり、車由上との誤差は特に大き
い。例えば内面トリックで球面度数5.00ディオプト
リ−・乱視度数2.00ディオプトリーのレンズにおい
ては、角度30oにおける乱視度の鞠上の乱視度との差
は0.260ディオプトリーであり、通通この度数付近
の眼鏡レンズが乱視度0.25ディオプトリーステツプ
で製品化されていることを考えると、このレンズのこの
部分の乱視度はワンステップ次のレンズの乱視度をこえ
ており、明らかに度数不良といえる。Examples of this are shown in Tables 1 and 2. Table 1,
As is clear from 2, the value of the correction angle 30o and the degree of astigmatism in its vicinity covers the weak part of the negative lens and the entire correct lens in the inner trick, and the entire negative and correct lenses in the outer trick, and The error with Yugami is particularly large. For example, in a lens with a spherical power of 5.00 diopters and an astigmatic power of 2.00 diopters with an inner trick, the difference between the astigmatism at an angle of 30o and the astigmatism on the ball is 0.260 diopters; Considering that eyeglass lenses are commercialized with astigmatism in 0.25 diopter steps, the astigmatism of this part of this lens exceeds the astigmatism of the next lens in one step, and it is clearly a poor dioptric power. I can say that.
また、眼鏡レンズにおいては、レンズの屈折率やレンズ
の厚みは量産性や重量・形状などの制約によって決定さ
れてしまい、通常、光学性能向上のための自由度とはな
りえない。Further, in eyeglass lenses, the refractive index and thickness of the lens are determined by constraints such as mass production, weight, shape, etc., and usually do not provide a degree of freedom for improving optical performance.
従って外面または内面のどちらか一方をトリック面、他
方を球面としたレンズにおいては、与えられたレンズ度
数を満足するようにレンズ形状を決定しうる自由度はた
だ一つであり、この自由度を利用して乱視度を補正する
ためには、前記Equal−船tigmatjsmの条
件を満足させるか、または軸上どちらか一方の主経線で
の補正すべき角度の乱視度を等しくすることが可能であ
るが、前記Equal−Astigmatismの条件
を満足した補正以外のいずれの補正の場合においても、
補正されない主経線の方向の乱視度がくずれる。Therefore, in a lens where either the outer or inner surface is a trick surface and the other is a spherical surface, there is only one degree of freedom in determining the lens shape to satisfy a given lens power, and this degree of freedom is In order to correct the degree of astigmatism using the above equation, it is possible to satisfy the condition of Equal-ship tigmatjsm, or to equalize the degrees of astigmatism of the angles to be corrected in either principal meridian on the axis. However, in the case of any correction other than the correction that satisfies the conditions of Equal-Astigmatism,
The degree of astigmatism in the direction of the uncorrected principal meridian is distorted.
(表3〜6参照)本発明においてはこの欠点を改善する
ために、外面及び内面の両面をトリック面として自由度
を2つにし、この2つの自由度によって軸外の補正角度
の乱視度が等しくなるように補正し(Eq雌1一Ast
igmatSmの条件)、かつ同時に鞠上の正規の乱視
度に等しくなるように補正したものである。即ち、レン
ズ単体の後頂点屈折力Pが正しンズの範囲で、レンズの
d−lheの屈折率Nを1.522ミNSI.254と
し、乱視レンズの符号も含めて大きい方の後頂点屈折力
Dv(ディオプトリー)がDv<2.75(デイオプト
リー)のときはレンズ中心厚dが1.6十0.1Dv≦
dS2.2十0.1Dv、2.75(ディオプトリー)
≦Dvのときは最小コバ厚t(肋)が0.5(側)St
SI.1(柵)とし、外面の互いに直交する2つの主蚤
線での面屈折力Ps、PCが・)。(See Tables 3 to 6) In order to improve this drawback, the present invention uses both the outer and inner surfaces as trick surfaces to have two degrees of freedom, and these two degrees of freedom reduce the degree of astigmatism of the off-axis correction angle. Correct it so that it is equal (Eq Female 1 - Ast
igmatSm conditions), and at the same time, the degree of astigmatism is corrected to be equal to the normal degree of astigmatism on the ball. That is, within the range of a lens in which the rear apex refractive power P of the lens alone is correct, the refractive index N of the lens d-lhe is 1.522 miNSI. 254, and when the larger rear vertex refractive power Dv (dioptres) including the sign of the astigmatic lens is Dv<2.75 (dioptres), the lens center thickness d is 1.6 + 0.1 Dv≦
dS2.20.1Dv, 2.75 (diopters)
When ≦Dv, the minimum edge thickness t (rib) is 0.5 (side) St
S.I. 1 (fence), and the surface refractive powers Ps and PC at two mutually orthogonal main fleas on the outer surface are .).
≦i辛旨3Aijxlyi<Ps<。≦i章j≦3Bi
jxlyJ2)。≦i羊j≦3CijX1y1<RC〈
〇≦i牢j≦3DiiX1をJ但し、x:Pの値
y:乱視度の値(>0)
各係数Aii、Bji、Cij、Dijは次の表のよう
な値をとるを満足するものである。≦ispicy3Aijxlyi<Ps<. ≦i chapter j≦3Bi
jxlyJ2). ≦i sheep j≦3CijX1y1<RC〈
〇≦i j≦3Dii be.
更に、レンズ単体の後頂点屈折力Pが負レンズの範囲で
、レンズのd−1中eの屈折率Nを1.522SNSI
.524とし、レンズの中心厚d(柳)をDvミー1(
デイオプトリー)のときは1.3十0.10vミdSI
.9十0.1Dv、一1(デイオプトリー)≦Dvのと
きは1.6十0.1Dv≦dS2.2十0.1Dvとし
、外面の互いに直交する主経線での面屈折力Ps、Pc
が、前記‘1}、■の制約式において各係数が次の表の
ような値をとることを満足するものである。Furthermore, within the range where the rear apex refractive power P of the lens alone is negative, the refractive index N of the lens at e in d-1 is set to 1.522 SNSI.
.. 524, and the center thickness d (willow) of the lens is Dv me 1 (
diopter) is 1.300.10v middSI
.. When 900.1Dv, 11 (diopters)≦Dv, 1.600.1Dv≦dS2.200.1Dv, and the surface refractive powers Ps and Pc at the mutually orthogonal principal meridians of the outer surface.
is satisfied that each coefficient in the constraint expressions '1} and (2) takes values as shown in the following table.
このようにして補正することにより、軸外の補正角度(
30o)の2つの主経線方向の乱視度が等しく、かつ鞄
上の正規の乱視度に等しくなることはもちろんのこと、
その他の角度においてもEq雌1−AstigmatS
mの条件などで補正したものに比べて大中に改善されて
いる。(表7参照)条件‘11式及び【21式は、補正
角30o、的物体として、このような補正のなされる関
係を式で表わしたものであり、例として乱視度数1ディ
オブトリー、2デイオプトリー、4デイオブトリーの場
合をグラフに表わしたものが第3,4,5図である。図
における実線が角度30oにおいて完全に補正された曲
線を示し、破線が○ー式及び■式で示された上下境界線
を表わす。すなわち完全な補正である実線を含むこの上
下境界線内においても十分に本発明の目的を達成できる
ものである。尚、第1図はしンズと眼球との幾何学的位
置を示す断面図で、本発明におけるレンズの後頂点と目
の回転中心点までの距離25肌と補正角a=300を示
したものである。By correcting in this way, the off-axis correction angle (
It goes without saying that the degree of astigmatism in the two principal meridian directions of 30o) is equal and equal to the regular degree of astigmatism on the bag.
Eq female 1-AstigmatS also at other angles
This is significantly improved compared to the one corrected under the conditions of m. (See Table 7) Conditions Equations 11 and 21 express the relationship in which such correction is made using a correction angle of 30o and a target object.For example, the astigmatism power is 1 dioptre, 2 dioptre, Graphs of the case of 4 days of trees are shown in Figures 3, 4, and 5. The solid line in the figure represents a curve completely corrected at an angle of 30o, and the broken line represents the upper and lower boundary lines indicated by the ◯ and ◯ equations. That is, the object of the present invention can be sufficiently achieved even within this upper and lower boundary line including the solid line, which is a complete correction. FIG. 1 is a sectional view showing the geometrical position of the lens and the eyeball, and shows the distance between the rear apex of the lens and the center of rotation of the eye of 25 skin and the correction angle a=300 in the present invention. It is.
又、第2図はしンズの正面図で、乱視レンズの2つの主
径線(Tan袋ntblmerjdもnとSagtta
lmerjdねn)を示す。但し、DHは符号も含めて
小さい方の後頂点屈折力である。次に前述してきた表1
〜表7を示す。Also, Figure 2 is a front view of the lens, and shows the two main meridians of the astigmatic lens (n and Sagtta).
lmerjdnen). However, DH is the smaller rear vertex refractive power including the sign. Next, Table 1 mentioned above
~ Table 7 is shown.
尚これらの表においては、レンズの屈折率は1.523
とし、レンズの中心厚d(側)は、Dv≦−1のときd
=1.6十0.1Dv、一1≦Dv<2.75のときd
=1.9十0.1Dvであり、2.75≦Dvのときは
最小コバ厚が0.7側となるようにとった。Equal
−Astigmatismの条件で補正した場合表I(
乱視度2ディオプトリー)
雛上乱視度との誤差(内面T.C)
午物体,単位 ディォブトリ一
表2
(乱視度2ディオプトリ−)
軸上乱視度との誤差(内面T.C) ら物体,
単位 ディォプトリ−軸上乱視度と鞘外(角度300)
T山船ENTIALM旧RIDIANの乱視度を等しく
した場合表3
(乱視度2ディォブトリ一)鞘上乱視度
との誤差(内向・章.C)表4
(舌し不測度2ディオプトリー)
軸上乱視度との誤差(外面T.C)
軸上と軸外(角度30o)SAGITTALMERID
IANの乱視度を等しくした場合表5
(乱棚夏2デ
ィオプトリー)軸上乱視度との誤差(内面T.C)表6
(乱視度2ディォブトリ−、)軸上乱視度との誤差(
外面T.C)本発明の実施例
・ 7
(乱視度2ディォフ。In these tables, the refractive index of the lens is 1.523.
The center thickness d (side) of the lens is d when Dv≦-1.
= 1.6 0.1Dv, d when 1≦Dv<2.75
= 1.9 + 0.1 Dv, and when 2.75≦Dv, the minimum edge thickness was set to be on the 0.7 side. Equal
- When corrected under Astigmatism conditions Table I (
(2 diopters of astigmatism) Error with the astigmatism on the axis (inner T.C.) Object, unit Diopter Table 2 (2 diopters of astigmatism) Error with the axial astigmatism (inner T.C.)
Unit diopter - axial astigmatism and extrasheath (angle 300)
Table 3 when the astigmatism of T-yamafune ENTIALM old RIDIAN is made equal
(Astigmatism: 2 diopters) Error with on-sheath astigmatism (inward, Chapter C) Table 4 (Tongue contingency: 2 diopters) Error with on-axis astigmatism (outer surface T.C) On-axis and off-axis ( Angle 30o) SAGITTALMERID
Table 5 when the degree of astigmatism of IAN is made equal
(Random shelf summer 2 diopters) Error with axial astigmatism (inner T.C) Table 6
(Astigmatism 2 db,) Error with on-axis astigmatism (
External T. C) Example 7 of the present invention
(Astigmatism level 2 Diof.
トリー)畑上乱視皮との誤差Tory) Error with Hatakami astigmatic skin
第1図はしンズと眼球との幾何学的位置を示した断面図
である。
第2図はしンズの正面図で、乱視レンズの2つの主経線
(Tan袋ntもI MeridianとSagt側M
er幻もn)を示す。第3図〜第5図はそれぞれ本発明
に依る乱視度1ディオプトリー・2ディオプトリー・4
ディオプトリーにおける実施例をグラフに表わしたもの
である。第′図
第2図
弟ぅ図
第4図
第ぶ図FIG. 1 is a sectional view showing the geometrical positions of the lenses and the eyeball. Figure 2 is a front view of the lens, showing the two principal meridians of the astigmatic lens (Tan sac nt also I Meridian and Sagt side M
er illusion also shows n). Figures 3 to 5 show astigmatism levels of 1 diopter, 2 diopter, and 4 according to the present invention, respectively.
1 is a graphical representation of an example in diopters. Figure 'Figure 2 Figure 2 Little brother Figure 4 Figure 4
Claims (1)
トリツク面で構成し、レンズ単体の後頂点屈折力Pが正
レンズの範囲で、レンズのd−lineの屈折率Nを1
.522≦N≦1.524とし、乱視レンズの符号も含
めて大きい方の後頂点屈折力Dv(デイオプトリー)が
Dv<2.75(デイオプトリー)のときはレンズ中心
厚dが1.6+0.1Dv≦d≦2.2+0.1Dv、
2.75(デイオプトリー)≦Dvのときは最小コバ厚
t(mm)が0.5(mm)≦t≦1.1(mm)とし
、前記外面の互いに直交する2つの主径線での面屈折力
Ps、Pcが▲数式、化学式、表等があります▼ 但し、 x:Pの値 y:乱視度の値(>0) 各係数Aij、Bij、Cij、Dijは次の表のよ
うな値をとる▲数式、化学式、表等があります▼ を満足することを特徴とする乱視用眼鏡レンズ。 2 乱視用眼鏡レンズにおいて、外面及び内面の両面を
トリツク面で構成し、レンズ単体の後頂点屈折力Pが負
レンズの範囲で、レンズのd−lineの屈折率Nを1
.522≦N≦1.524とし、レンズの中心厚d(m
m)は乱視レンズの符号も含めて大きい方の後頂点屈折
力Dv(デイオプトリー)がDv≦−1(デイオプトリ
ー)のときは1.3+0.1Dv≦d≦1.9+0.1
Dv、−1(デイオプトリー)≦Dvのときは1.6+
0.1Dv≦d≦2.2+0.1Dvとし、前記外面の
互いに直交する2つの主径線での面屈折力Ps、Pcが
▲数式、化学式、表等があります▼ 但し、 x:Pの値 y:乱視度の値(>0) 各係数Aij、Bij、Cij、Dijは次の表のよ
うな値をとる▲数式、化学式、表等があります▼ を満足することを特徴とする乱視用眼鏡レンズ。[Claims] 1. In a spectacle lens for astigmatism, both the outer and inner surfaces are made up of trick surfaces, and the rear apex refractive power P of the lens alone is within the range of a positive lens, and the d-line refractive index N of the lens is within the range of a positive lens. 1
.. 522≦N≦1.524, and when the larger rear vertex refractive power Dv (dioptres) including the sign of the astigmatic lens is Dv<2.75 (dioptres), the lens center thickness d is 1.6+0.1Dv≦ d≦2.2+0.1Dv,
2.75 (diopters)≦Dv, the minimum edge thickness t (mm) is 0.5 (mm)≦t≦1.1 (mm), and the surface of the two main meridians perpendicular to each other on the outer surface The refractive powers Ps and Pc are ▲ There are mathematical formulas, chemical formulas, tables, etc. ▼ However, x: value of P y: value of degree of astigmatism (>0) Each coefficient Aij, Bij, Cij, Dij is a value as shown in the following table A spectacle lens for astigmatism that satisfies the following: ▲ There are mathematical formulas, chemical formulas, tables, etc. ▼ 2. In a spectacle lens for astigmatism, both the outer and inner surfaces are made up of trick surfaces, and the d-line refractive index N of the lens is set to 1 within the range where the rear apex refractive power P of the lens alone is negative.
.. 522≦N≦1.524, and the center thickness of the lens d(m
m) is 1.3+0.1 when the larger rear vertex refractive power Dv (dioptres) including the sign of the astigmatic lens is Dv≦-1 (dioptres) Dv≦d≦1.9+0.1
Dv, -1 (diopter) ≦ 1.6+ when Dv
0.1Dv≦d≦2.2+0.1Dv, and the surface refractive powers Ps and Pc at the two mutually orthogonal principal meridians of the outer surface are ▲There are mathematical formulas, chemical formulas, tables, etc.▼ However, the value of x: P y: Value of degree of astigmatism (>0) Each coefficient Aij, Bij, Cij, Dij takes a value as shown in the following table ▲ There are mathematical formulas, chemical formulas, tables, etc. ▼ Glasses for astigmatism characterized by satisfying the following. lens.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3906078A JPS601604B2 (en) | 1978-04-03 | 1978-04-03 | eyeglass lenses for astigmatism |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP3906078A JPS601604B2 (en) | 1978-04-03 | 1978-04-03 | eyeglass lenses for astigmatism |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS54131950A JPS54131950A (en) | 1979-10-13 |
JPS601604B2 true JPS601604B2 (en) | 1985-01-16 |
Family
ID=12542581
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP3906078A Expired JPS601604B2 (en) | 1978-04-03 | 1978-04-03 | eyeglass lenses for astigmatism |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS601604B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0561121B2 (en) * | 1990-05-25 | 1993-09-03 | Sumitomo Rubber Ind |
Families Citing this family (8)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US5479220A (en) * | 1991-10-09 | 1995-12-26 | Seiko Epson Corporation | Eyeglass lens |
US5767939A (en) * | 1991-10-09 | 1998-06-16 | Seiko Epson Corporation | Eyeglass lens |
US6012813A (en) * | 1997-06-19 | 2000-01-11 | Hoya Corporation | Aspherical spectacle lens |
JP2006178245A (en) * | 2004-12-24 | 2006-07-06 | Tokai Kogaku Kk | Spectacle lens for for astigmatism correction |
EP2369972B1 (en) | 2008-12-01 | 2017-06-07 | Perfect Vision Technology (HK) Ltd. | Methods and devices for refractive correction of eyes |
US9649032B2 (en) | 2008-12-01 | 2017-05-16 | Perfect Vision Technology (Hk) Ltd. | Systems and methods for remote measurement of the eyes and delivering of sunglasses and eyeglasses |
US9277863B2 (en) | 2008-12-01 | 2016-03-08 | Perfect Vision Technology (Hk) Ltd. | Methods and systems for automated measurement of the eyes and delivering of sunglasses and eyeglasses |
US10444539B2 (en) | 2016-05-11 | 2019-10-15 | Perect Vision Technology (Hk) Ltd. | Methods and systems for determining refractive corrections of human eyes for eyeglasses |
-
1978
- 1978-04-03 JP JP3906078A patent/JPS601604B2/en not_active Expired
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0561121B2 (en) * | 1990-05-25 | 1993-09-03 | Sumitomo Rubber Ind |
Also Published As
Publication number | Publication date |
---|---|
JPS54131950A (en) | 1979-10-13 |
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