JPH0250445B2 - - Google Patents
Info
- Publication number
- JPH0250445B2 JPH0250445B2 JP57174467A JP17446782A JPH0250445B2 JP H0250445 B2 JPH0250445 B2 JP H0250445B2 JP 57174467 A JP57174467 A JP 57174467A JP 17446782 A JP17446782 A JP 17446782A JP H0250445 B2 JPH0250445 B2 JP H0250445B2
- Authority
- JP
- Japan
- Prior art keywords
- lens group
- lens
- focal length
- aberration
- condition
- 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
Links
- 239000011521 glass Substances 0.000 claims description 2
- 239000000463 material Substances 0.000 claims description 2
- 230000005499 meniscus Effects 0.000 claims description 2
- 239000002131 composite material Substances 0.000 claims 1
- 230000004075 alteration Effects 0.000 description 32
- 206010010071 Coma Diseases 0.000 description 8
- 201000009310 astigmatism Diseases 0.000 description 8
- 230000007423 decrease Effects 0.000 description 1
- 238000010586 diagram Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 230000003287 optical effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B13/00—Optical objectives specially designed for the purposes specified below
- G02B13/04—Reversed telephoto objectives
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B9/00—Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or -
- G02B9/34—Optical objectives characterised both by the number of the components and their arrangements according to their sign, i.e. + or - having four components only
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Lenses (AREA)
Description
本発明は画角57度程度、明るさF2.8程度の広角
レンズ、特にデイスクカメラやフアクシミリなど
の比較的小さな画面サイズの光学系に用いられる
広角レンズに関する。
従来、この種のレンズ系は、焦点距離が小さい
ため、レンズのコンパクト化には考慮が払われ
ず、大きい望遠率をもつていた。最近デイスクカ
メラ用レンズとして、非球面を採用することによ
つて望遠率を小さくしたものが現れた。
本発明は4群4枚の構成により、非球面を用い
ることなく、球面のみで望遠率の小さい収差補正
の良好で上述の用途に適した広角レンズを得よう
とするものである。
この目的を達成するために、レンズ系は具体的
には物体側から順に、強い凸面を物体側に向けた
両凸レンズからなる第1レンズ群、強い凹面を像
側に向けた両凹レンズからなる第2レンズ群、両
凸レンズである第3レンズ群および像側に凸面を
向けた負メニスカスである第4レンズ群とにより
構成され、
f:全系の焦点距離
f1.2:第1レンズ群と第2レンズ群との合成焦点
距離
f1.2.3:第1レンズ群から第3レンズ群までの合成
焦点距離
D6:第3レンズ群と第4レンズ群との間隔
R7:第4レンズ群の物体側の曲率半径
Ni:第iレンズ群の硝材の屈折率
とするとき
―0.05/f<1/f1.2<0.15/f ……(1)
1.27/f<1/f1,2,3<1.55/f ……(2)
0.22f<D6<0.36f ……(3)
N1、N2、N4>1.75、N3>1.68 ……(4)
の各条件を満足する広角レンズであり、望遠率は
約1.2以下に押されることが出来る。
本発明のレンズは、軸外光束の条件を良くする
ために絞りを第2レンズ群と第3レンズ群との間
に置いてある。このため、第3レンズ群で発生す
る負の歪曲収差を、第1レンズ群に両凸レンズを
用いることで補正している。
条件(1)(2)は球面収差、コマ収差、歪曲収差を適
正に保つとともに望遠率を小さくするために必要
な条件である。
条件(1)の下限をこえると第1レンズ群の焦点距
離が長くなるか、第2レンズ群の焦点距離が短く
なるため、オーバーのコマフレアと大きなアンダ
ーの歪曲収差が発生する。更に主点位置が像側に
移動するため望遠率が大きくなる。逆に上限をこ
えると、第1レンズ群の焦点距離が短かくなる
か、第2レンズ群の焦点距離が長くなるため、大
きなアンダーの球面収差が発生する。
条件(2)の下限をこえるとオーバーのコマフレア
が発生し、更に望遠率が大きくなる。逆に上限よ
り大となればアンダーのコマフレアと、大きなア
ンダーの歪曲収差、更にアンダーの球面収差が発
生する。
条件(3)は諸収差を適当な範囲に収めながら望遠
率を小さく保つために必要な条件である。
条件(3)が下限をこえると、望遠率を小さく保つ
ためには、1/f1.2を条件(1)の上限より大とする
か1/f1.2.3を条件(2)の上限より大としなければな
らない。逆に条件(3)が上限をこえると、望遠率は
小さくなるが第4レンズ群が第3レンズ群から大
きく離れるため、球面収差とコマ収差の補正が、
困難になる。
条件(4)は全系のペツパール和を適正範囲に保つ
と共に、球面収差、コマ収差を適正範囲に保つた
めに必要な条件であると共に、望遠率を小さく保
つために必要な条件である。凸レンズ群の屈折率
N1、N3が下限より小となる凸レンズ群の曲率半
径が小になるためペツパール和が大きくなり、像
面湾曲が大きくなる。更に、球面収差が補正不足
になる。
逆に凹レンズ群の屈折率N2、N4が条件(4)の下
限より小になると、凹レンズ群の曲率半径が小に
なるため、ペツパール和が小になり、像面が像側
に曲がり非点隔差が大きくなると共にオーバーの
コマフレアが発生する。
各レンズ群の屈折率が条件(4)の下限より小さく
なつても、各収差は良好に補正出来るが、本発明
においては焦点距離の小さいレンズ系を対象とし
ているので、各レンズ群の加工の容易さも考慮し
なければならない。凸レンズ群の屈折率が条件(4)
の下限より小になると前述の収差の悪化を招く。
これは凹レンズ群の屈折率が小になると凸レンズ
群の曲率半径が小になるため、凸レンズの軸上厚
を大きくしないとレンズ加工が困難になる。とこ
ろが凸レンズ群の軸上厚を大きくするとレンズ系
の望遠率を小さく保つことが出来なくなる。
更に、球面収差とコマ収差を適正な範囲に止め
るためには、R7が下記の条件を満すことが望ま
しい。
−0.6f<<R7<−0.32f ……(5)
以下本発明のレンズ系の実施例を示す。
次に本発明の実施例を示す。
実施例において、Rは、曲率半径、Dは、面間
隔、Nは、屈折率、Vは、アツベ数、Tは、望遠
率である。
実施例 1
f=10 FNp=2.87 2W=57゜30′
The present invention relates to a wide-angle lens with an angle of view of about 57 degrees and a brightness of about F2.8, and particularly to a wide-angle lens used in optical systems with relatively small screen sizes such as disk cameras and facsimiles. Conventionally, this type of lens system had a small focal length, so no consideration was given to making the lens compact, and it had a large telephoto ratio. Recently, lenses for disk cameras have appeared that have a reduced telephoto ratio by using an aspherical surface. The present invention uses a configuration of four lenses in four groups to provide a wide-angle lens that uses only spherical surfaces without using any aspherical surfaces, has a small telephoto ratio, has good aberration correction, and is suitable for the above-mentioned applications. In order to achieve this objective, the lens system is constructed in order from the object side: a first lens group consisting of a biconvex lens with a strongly convex surface facing the object side, and a second lens group consisting of a biconcave lens with a strongly concave surface facing the image side. It consists of two lens groups, a third lens group that is a biconvex lens, and a fourth lens group that is a negative meniscus with a convex surface facing the image side, f: focal length of the entire system f 1.2 : the first lens group and the second lens group Combined focal length with the lens group f 1.2.3 : Combined focal length from the first lens group to the third lens group D 6 : Distance between the third lens group and the fourth lens group R 7 : Object in the fourth lens group Radius of curvature Ni: When the refractive index of the glass material of the i-th lens group is -0.05/f<1/f1.2<0.15/f...(1) 1.27/f<1/f1, 2, 3<1.55 /f...(2) 0.22f< D6 <0.36f...(3) N1 , N2 , N4 >1.75, N3 >1.68...It is a wide-angle lens that satisfies each condition of (4). , the telephoto ratio can be pushed to about 1.2 or less. In the lens of the present invention, an aperture is placed between the second lens group and the third lens group in order to improve the conditions for off-axis light flux. Therefore, the negative distortion generated in the third lens group is corrected by using a biconvex lens in the first lens group. Conditions (1) and (2) are necessary to maintain appropriate spherical aberration, coma aberration, and distortion, and to reduce the telephoto ratio. If the lower limit of condition (1) is exceeded, the focal length of the first lens group becomes longer or the focal length of the second lens group becomes shorter, resulting in excessive coma flare and large under distortion. Furthermore, since the principal point position moves toward the image side, the telephoto ratio increases. On the other hand, if the upper limit is exceeded, the focal length of the first lens group becomes shorter or the focal length of the second lens group becomes longer, resulting in large under-spherical aberration. If the lower limit of condition (2) is exceeded, excessive coma flare will occur and the telephoto ratio will further increase. On the other hand, if the value is larger than the upper limit, under-coma flare, large under-distortion aberration, and under-spherical spherical aberration will occur. Condition (3) is necessary to keep the telephoto ratio small while keeping various aberrations within appropriate ranges. If condition (3) exceeds the lower limit, in order to keep the telephoto ratio small, 1/f 1.2 should be greater than the upper limit of condition (1), or 1/f 1.2.3 should be greater than the upper limit of condition (2). Must be. Conversely, when condition (3) exceeds the upper limit, the telephoto ratio decreases, but the fourth lens group is far away from the third lens group, so correction of spherical aberration and coma aberration becomes difficult.
It becomes difficult. Condition (4) is a necessary condition for keeping the Petzpar sum of the entire system within an appropriate range, spherical aberration and coma aberration within an appropriate range, and a necessary condition for keeping the telephoto ratio small. Refractive index of convex lens group
Since the radius of curvature of the convex lens group in which N 1 and N 3 are smaller than the lower limit becomes smaller, the Petz Pearl sum becomes larger and the curvature of field becomes larger. Furthermore, spherical aberration becomes undercorrected. Conversely, when the refractive indices N 2 and N 4 of the concave lens group become smaller than the lower limit of condition (4), the radius of curvature of the concave lens group becomes small, the Petzpar sum becomes small, and the image plane curves toward the image side. As the point distance difference increases, excessive coma flare occurs. Even if the refractive index of each lens group is smaller than the lower limit of condition (4), each aberration can be well corrected, but since the present invention is aimed at a lens system with a small focal length, the processing of each lens group is Ease of use must also be considered. The refractive index of the convex lens group is the condition (4)
If it becomes smaller than the lower limit of , the aberration described above will worsen.
This is because when the refractive index of the concave lens group becomes small, the radius of curvature of the convex lens group becomes small, so lens processing becomes difficult unless the axial thickness of the convex lens is increased. However, if the axial thickness of the convex lens group is increased, it becomes impossible to keep the telephoto ratio of the lens system small. Furthermore, in order to keep spherical aberration and coma within appropriate ranges, it is desirable that R7 satisfy the following conditions. −0.6f<<R 7 <−0.32f (5) Examples of the lens system of the present invention will be shown below. Next, examples of the present invention will be shown. In the examples, R is the radius of curvature, D is the interplanar distance, N is the refractive index, V is the Abbe number, and T is the telephoto ratio. Example 1 f=10 F Np =2.87 2W=57°30′
【表】
T=1.197 1/f1.2=0.0538/f 1/f1.2.3=
1.46811/f
球面収差、非点収差、歪曲収差曲線は第2図に
示す。
実施例 2
f=10 FFp=2.87 2w=57゜24′[Table] T=1.197 1/f 1.2 = 0.0538/f 1/f 1.2.3 =
1.46811/f Spherical aberration, astigmatism, and distortion aberration curves are shown in Figure 2. Example 2 f=10 F Fp =2.87 2w=57°24′
【表】
T=1.198 1/f1.2=0.0415/f 1/f1.2.3=
1.452/f
球面収差、非点収差、歪曲収差曲線は第3図に
示す。
実施例 3
f=10 FNp=2.87 2w=57゜31′[Table] T=1.198 1/f 1.2 = 0.0415/f 1/f 1.2.3 =
1.452/f Spherical aberration, astigmatism, and distortion aberration curves are shown in Figure 3. Example 3 f=10 F Np =2.87 2w=57°31′
【表】
T=1.199 1/f1.2=0.0982/f 1/f1.2.3=
1.4688.f
球面収差、非点収差、歪曲収差曲線を第4図に
示す。
実施例 4
f=10 FNp=2.87 2w=50゜26′[Table] T=1.199 1/f 1.2 = 0.0982/f 1/f 1.2.3 =
1.4688.f Figure 4 shows the spherical aberration, astigmatism, and distortion aberration curves. Example 4 f=10 F Np =2.87 2w=50°26′
【表】【table】
【表】
T=1.195 1/f1.2=0.0181/f 1/f1.2.3=
1.4300/f
球面収差、非点収差、歪曲収差曲線を第5図に
示す。
実施例 5
f=10 FNp=2.87 2w=57゜32′[Table] T=1.195 1/f 1.2 = 0.0181/f 1/f 1.2.3 =
1.4300/f Figure 5 shows the spherical aberration, astigmatism, and distortion aberration curves. Example 5 f=10 F Np =2.87 2w=57°32′
【表】
T=1.199 1/f1.2=0.0312/f 1/f1.2.3=
1.4500/f
球面収差、非点収差、歪曲収差曲線を第6図に
示す。
実施例 6
f=10 FNp=2.87 2w=56゜26′[Table] T=1.199 1/f 1.2 = 0.0312/f 1/f 1.2.3 =
1.4500/f Figure 6 shows the spherical aberration, astigmatism, and distortion aberration curves. Example 6 f=10 F Np =2.87 2w=56°26′
【表】
T=1.188 1/f1.2=0.0681/f 1/f1.2.3=
1.4143/f
球面収差、非点収差、歪曲収差曲線は、第7図
に示す。
実施例 7
f=10 FNp=2.87 2w=56゜12′[Table] T=1.188 1/f 1.2 = 0.0681/f 1/f 1.2.3 =
1.4143/f Spherical aberration, astigmatism, and distortion aberration curves are shown in FIG. Example 7 f=10 F Np =2.87 2w=56°12′
【表】
T=1.156 1/f1.2=0.1241/f 1/f1.2.3=
1.4734/f
球面収差、非点収差、歪曲収差曲線は第8図に
示す。
実施例 8
f=10、FNp=2.87 2w=56゜12′[Table] T=1.156 1/f 1.2 = 0.1241/f 1/f 1.2.3 =
1.4734/f Spherical aberration, astigmatism, and distortion aberration curves are shown in Figure 8. Example 8 f=10, F Np =2.87 2w=56°12′
【表】【table】
【表】
T=1.196 1/f1.2=0.0599/f 1/f1.2.3=
1.3523/f
球面収差、非点収差、歪曲収差曲線は第9図に
示す。[Table] T=1.196 1/f 1.2 = 0.0599/f 1/f 1.2.3 =
1.3523/f Spherical aberration, astigmatism, and distortion aberration curves are shown in Figure 9.
第1図は本発明の1実施例のレンズ断面図、第
2図、第3図、第4図、第5図、第6図、第7
図、第8図、第9図はそれぞれ実施例1、実施例
2、実施例3、実施例4、実施例5、実施例6、
実施例7、実施例8の収差曲線図である。
FIG. 1 is a sectional view of a lens according to an embodiment of the present invention, FIGS. 2, 3, 4, 5, 6, and 7.
, FIG. 8, and FIG. 9 are respectively Example 1, Example 2, Example 3, Example 4, Example 5, Example 6,
FIG. 7 is an aberration curve diagram of Example 7 and Example 8.
Claims (1)
両凸レンズからなる第1レンズ群、強い凹面を像
側に向けた両凹レンズからなる第2レンズ群、両
凸レンズである第3レンズ群および像側に凸面を
向けた負メニスカスである第4レンズ群とにより
構成され、 f:全系の焦点距離 f1.2:第1レンズ群と第2レンズ群との合成焦点
距離 f1.2.3:第1レンズ群から第3レンズ群までの合成
焦点距離 D6:第3レンズ群と第4レンズ群との間隔 R7:第4レンズ群の物体側の曲率半径 Ni:第iレンズ群の硝材の屈折率 とするとき −0.05/f<1/f1.2<0.15/f 1.27/f<1/f1,2,3<1.55/f 0.22f<D6<0.36f N1、N2、N4>1.75N3>1.68 の各条件を満足する広角レンズ[Claims] 1. In order from the object side, a first lens group consisting of a biconvex lens with a strongly convex surface facing the object side, a second lens group consisting of a biconcave lens with a strongly concave surface facing the image side, and a biconvex lens. It is composed of a third lens group and a fourth lens group which is a negative meniscus with a convex surface facing the image side, f: Focal length of the entire system f 1.2 : Combined focal length of the first lens group and the second lens group f 1.2.3 : Composite focal length D from the first lens group to the third lens group 6 : Distance between the third and fourth lens groups R 7 : Radius of curvature on the object side of the fourth lens group Ni: i-th When the refractive index of the glass material of the lens group is -0.05/f<1/f1.2<0.15/f1.27/f<1/f1,2,3<1.55/f0.22f< D6 <0.36f N1 , Wide-angle lens that satisfies the following conditions: N 2 , N 4 >1.75N 3 >1.68
Priority Applications (3)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57174467A JPS5964809A (en) | 1982-10-06 | 1982-10-06 | Wide angle lens |
| GB08326660A GB2131198A (en) | 1982-10-06 | 1983-10-05 | Wide angle lens having four lenses |
| DE19833336433 DE3336433A1 (en) | 1982-10-06 | 1983-10-06 | WIDE-ANGLE LENS |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP57174467A JPS5964809A (en) | 1982-10-06 | 1982-10-06 | Wide angle lens |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5964809A JPS5964809A (en) | 1984-04-12 |
| JPH0250445B2 true JPH0250445B2 (en) | 1990-11-02 |
Family
ID=15978989
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP57174467A Granted JPS5964809A (en) | 1982-10-06 | 1982-10-06 | Wide angle lens |
Country Status (3)
| Country | Link |
|---|---|
| JP (1) | JPS5964809A (en) |
| DE (1) | DE3336433A1 (en) |
| GB (1) | GB2131198A (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US4688906A (en) * | 1985-12-30 | 1987-08-25 | Capitol Records | Three dimensional reflex lens systems |
| JP4233062B2 (en) * | 1997-03-26 | 2009-03-04 | フジノン株式会社 | Imaging lens |
| RU2183341C1 (en) * | 2000-10-26 | 2002-06-10 | Открытое акционерное общество "Красногорский завод им. С.А. Зверева" | Wide-aperture lens |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| GB618360A (en) * | 1946-10-25 | 1949-02-21 | Eastman Kodak Co | Improvements in or relating to photographic objectives |
| US3861799A (en) * | 1973-01-26 | 1975-01-21 | Minnesota Mining & Mfg | Camera |
| JPS5573014A (en) * | 1978-11-28 | 1980-06-02 | Olympus Optical Co Ltd | Photographic lens |
-
1982
- 1982-10-06 JP JP57174467A patent/JPS5964809A/en active Granted
-
1983
- 1983-10-05 GB GB08326660A patent/GB2131198A/en not_active Withdrawn
- 1983-10-06 DE DE19833336433 patent/DE3336433A1/en not_active Withdrawn
Also Published As
| Publication number | Publication date |
|---|---|
| GB2131198A (en) | 1984-06-13 |
| JPS5964809A (en) | 1984-04-12 |
| GB8326660D0 (en) | 1983-11-09 |
| DE3336433A1 (en) | 1984-04-12 |
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