JPH08122505A - Optical member - Google Patents
Optical memberInfo
- Publication number
- JPH08122505A JPH08122505A JP28918594A JP28918594A JPH08122505A JP H08122505 A JPH08122505 A JP H08122505A JP 28918594 A JP28918594 A JP 28918594A JP 28918594 A JP28918594 A JP 28918594A JP H08122505 A JPH08122505 A JP H08122505A
- Authority
- JP
- Japan
- Prior art keywords
- joint
- optical
- function
- optical member
- optical component
- 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.)
- Pending
Links
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- Optical Elements Other Than Lenses (AREA)
Abstract
Description
【0001】[0001]
【産業上の利用分野】本発明は光学部材に関し、特に所
定の曲率の第1の面を有した第1の光学部品と第1の面
の延長面と異なる面を有する第2の光学部品を一体化し
た光学部材に関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an optical member, and more particularly to a first optical component having a first surface having a predetermined curvature and a second optical component having a surface different from an extension surface of the first surface. The present invention relates to an integrated optical member.
【0002】[0002]
【従来の技術】近年、光学設計技術の進歩に伴い複雑な
曲面を含んだ光学系で構成される光学装置が広く使用さ
れるようになった。それらの中の1つに、幾つかの光学
部品が共通の光軸上に配置されていない複数の光軸を含
む光学系を使用しているものがある。これらの光学系の
場合は、共通の光軸を持つ共軸光学系に比べて組み立て
時に十分な精度を確保することが難しい。又、反射鏡を
用いる光学系の場合、或る光学部品を別の光学部品に対
してその光軸と垂直な方向の近傍に配置することがあ
る。ここで、精度確保の方法として、近傍に位置する複
数の部品を一体として製作して精度を維持することが考
えられる。この様にすれば部品数も減り、組み立ても容
易になる。例えばUSP5,253116 号では、2枚の反射鏡
(光学部品)が一つのミラーで構成しているフライトシ
ミュレーター用の表示装置が開示されている。2. Description of the Related Art In recent years, with the progress of optical design technology, optical devices composed of optical systems including complicated curved surfaces have been widely used. One of them uses an optical system that includes multiple optical axes, where some optical components are not arranged on a common optical axis. In the case of these optical systems, it is difficult to secure sufficient accuracy during assembly, as compared with the coaxial optical system having a common optical axis. Further, in the case of an optical system using a reflecting mirror, one optical component may be disposed near another optical component in the direction perpendicular to the optical axis. Here, as a method of ensuring accuracy, it is conceivable to integrally manufacture a plurality of parts located in the vicinity to maintain accuracy. This reduces the number of parts and facilitates assembly. For example, USP 5,253116 discloses a display device for a flight simulator in which two reflecting mirrors (optical parts) are configured by one mirror.
【0003】このような一体成形の技術としては、例え
ば軽量化にも有利な技術として成形材料に合成樹脂等を
用いる圧縮成形、射出成形加工が頻繁に用いられてい
る。As a technique for such integral molding, for example, compression molding using a synthetic resin or the like as a molding material and injection molding are frequently used as a technique advantageous for weight reduction.
【0004】射出成形加工は最も生産性に富む加工方法
であり、合成樹脂を用いた成形は成形加工が比較的容易
であるという長所を持っている。更に、曲面として非球
面レンズ等の機械加工が著しく困難な光学部材でも一個
の型を作れば、多数の光学部材が容易に成形製作出来
る。Injection molding is the most productive processing method, and molding using a synthetic resin has the advantage that molding is relatively easy. Further, even if an optical member such as an aspherical lens which is extremely difficult to machine as a curved surface is formed into a single mold, a large number of optical members can be easily molded and manufactured.
【0005】[0005]
【発明が解決しようとする課題】しかし、合成樹脂を用
いる加工においては、その熱膨張率が無機材料より一桁
大きい為に成形時の収縮、使用環境における寸法変化を
考慮する必要がある。光学特性との関連では、金型精度
の他に成形収縮と分子配向の配慮が重要である。成形収
縮が成形物全体の寸法精度に影響することは勿論である
が、冷却時の局部的な収縮は残留歪み、変形として現れ
る。However, in the processing using a synthetic resin, it is necessary to consider shrinkage at the time of molding and dimensional change in the use environment because its coefficient of thermal expansion is an order of magnitude higher than that of an inorganic material. In terms of optical characteristics, it is important to consider mold shrinkage and molecular orientation in addition to mold precision. Needless to say, the molding shrinkage affects the dimensional accuracy of the entire molded product, but the local shrinkage during cooling appears as residual strain and deformation.
【0006】又、成形材料が金型内で固化するとき、一
般には自由に収縮出来ない為収縮しようとする応力が残
ってしまう。軟質材料では金型から成形物を取り出した
時、このような応力は解放され、ソリとなって現れる
が、ポリスチレン、ポリメチルメタクリレート、ポリカ
ーボネート等の硬質材料では応力は解放されず、応力を
残してそのままの形状を保っている。この場合の応力を
内部応力といい、例えば溶剤などに触れるとクラックを
発生し易く、又使用中に自然に壊れることさえある。Further, when the molding material is solidified in the mold, it cannot generally shrink freely, so that the stress for shrinking remains. For soft materials, when the molded product is taken out of the mold, such stress is released and appears as warps, but for hard materials such as polystyrene, polymethylmethacrylate, and polycarbonate, the stress is not released and leaves stress. It retains its original shape. The stress in this case is called internal stress, and cracks are likely to occur when exposed to a solvent, for example, and even spontaneously break during use.
【0007】ところで、複数の光学部品を一体成形によ
り一つの光学部材として製作しようとする場合、接合す
る光学部品の面夫々が一つの面の一部、もしくはそれに
近い面形状ならば、そのまま接合してもそれほど問題に
はならない。しかしながら一つの滑らかな面の上に乗っ
ていない2つの光学面を接合しようとする場合には、光
学面と光学面との間の面(接合面)の面形状を適切に設
計しないと種々の問題点が発生する。By the way, when a plurality of optical components are to be integrally molded into one optical member, if the surfaces of the optical components to be joined are part of one surface or have a surface shape close to that, they are directly joined. But it doesn't really matter. However, when two optical surfaces that are not on one smooth surface are to be joined together, various surface shapes of the surfaces (joint surfaces) between the optical surfaces must be properly designed. Problems occur.
【0008】即ち、射出成形等では面と面の接合部に段
差があったり、面形状が不連続であったりすると、固化
して金型から抜く際に、この部分に力が加わり変形する
ことがある。又、内部応力として残る可能性も大きくな
る。単純に断面と断面とを繋げば良いという訳ではな
い。That is, in injection molding or the like, if there is a step at the surface-to-surface joint or if the surface shape is discontinuous, a force is applied to this portion when it is solidified and removed from the mold, and is deformed. There is. In addition, the possibility that it will remain as an internal stress also increases. It is not just a matter of connecting cross sections.
【0009】USP5,253,116号公報で開示された技術には
接合部の面形状を求める手段が示されておらず、実際に
製作するにあたって接合部分の面形状を定めることが出
来ない。即ちUSP5,253,116号公報では接合面を構成する
具体的な方法が開示されておらず、実施することが事実
上大変困難である。The technique disclosed in US Pat. No. 5,253,116 does not show a means for determining the surface shape of the joint portion, and the surface shape of the joint portion cannot be determined in actual manufacturing. That is, USP 5,253,116 does not disclose a specific method for forming a joint surface, and it is practically very difficult to carry out the method.
【0010】本発明の目的は、曲率の異なる曲面を有す
る複数の光学部品を1つの光学部材として一体成形する
際に、複数の光学部品を接合する接合部分の繋ぎ面形状
を適切に構成し、光学部品と接合部分との境界におい
て、2つの面を滑らかに繋ぎ、これによって成型加工時
の光学部材への残留応力を減少して製造誤差の発生を少
なくした光学部材の提供にある。この他に部品数を削減
し、組み立て作業の工数を削減して、コストダウンを実
現する高精度の光学部材の提供にある。An object of the present invention is to appropriately form a joint surface shape of a joint portion for joining a plurality of optical components when integrally molding a plurality of optical components having curved surfaces having different curvatures as one optical member, An object of the present invention is to provide an optical member in which two surfaces are smoothly connected at a boundary between an optical component and a joint portion, thereby reducing residual stress on the optical member at the time of molding and reducing manufacturing errors. In addition, the number of parts is reduced, the number of assembling steps is reduced, and a highly accurate optical member that realizes cost reduction is provided.
【0011】[0011]
【課題を解決するための手段】本発明の光学部材の構成
は、 (1−1) 所定の曲率の面1aを有する第1の光学部
品と、該面1aの延長面と異なる面2aを有する第2の
光学部品とが、接合部分を介して繋がっており、更に該
面1a及び該面2aと該接合部分の境界は滑らかに繋が
っており、且つ条件 f1a(xt1)=fta(xt1) 、 f2a(xt2)=fta(xt2) f1a'(xt1)=fta'(xt1)、 f2a'(xt2)=fta'(xt2) 但し、 f1a(x) :第1の光学部材の面1aを記述する関数 x>x
t1 f2a(x) :第2の光学部材の面2aを記述する関数 x<xt2 fta(x) :接合部分の面taを記述する関数 xt2<x<xt1 f1a'(x)、 f2a'(x)、 fta'(x):面の傾きを表す関数 xt1 、xt2 : 接合部の位置ベクトル を満たした、一体成形によって製作されたものであるこ
とを特徴としている。The structure of the optical member of the present invention comprises (1-1) a first optical component having a surface 1a having a predetermined curvature, and a surface 2a different from the extension surface of the surface 1a. The second optical component is connected via a joint portion, and further, the surface 1a and the boundary between the surface 2a and the joint portion are smoothly connected, and the condition f 1a (x t1 ) = f ta ( x t1 ), f 2a (x t2 ) = f ta (x t2 ) f 1a '(x t1 ) = f ta ' (x t1 ), f 2a '(x t2 ) = f ta ' (x t2 ), where f 1a (x): Function x> x describing the surface 1a of the first optical member
t1 f 2a (x): Function describing surface 2a of the second optical member x <x t2 f ta (x): Function describing surface ta of the joint part x t2 <x <x t1 f 1a '(x ), F 2a '(x), f ta ' (x): Functions representing the inclination of the surface x t1 , x t2 : characterized by being manufactured by integral molding that satisfies the position vector of the joint There is.
【0012】特に、(1−1−1) 前記第1の光学部
品は所定の曲率の面1bを有し、前記第2の光学部品は
該面1bの延長面と異なる面2bを有し、該面1bと該
面2bとが、前記接合部分を介して繋がっており、更に
該面1b及び該面2bと該接合部分の境界は滑らかに繋
がっており、且つ条件 f1b(xt3)=ftb(xt3) 、 f2b(xt4)=ftb(xt4) f1b'(xt3)=ftb'(xt3)、 f2b'(xt4)=ftb'(xt4) 但し、 f1b(x) :第1の光学部材の面1bを記述する関数 x>x
t3 f2b(x) :第2の光学部材の面2bを記述する関数 x<xt4 ftb(x) :接合部分の面tbを記述する関数 xt4<x<xt3 f1b'(x)、 f2b'(x)、 ftb'(x):面の傾きを表す関数 xt3 、xt4 : 接合部の位置ベクトル を満たしたこと等を特徴としている。In particular, (1-1-1) the first optical component has a surface 1b having a predetermined curvature, and the second optical component has a surface 2b different from an extension surface of the surface 1b, The surface 1b and the surface 2b are connected to each other via the joint portion, and further, the boundary between the surface 1b and the surface 2b and the joint portion is smoothly connected, and the condition f 1b (x t3 ) = f tb (x t3 ), f 2b (x t4 ) = f tb (x t4 ) f 1b '(x t3 ) = f tb ' (x t3 ), f 2b '(x t4 ) = f tb ' (x t4 ) Where f 1b (x): Function x> x that describes the surface 1b of the first optical member
t3 f 2b (x): Function describing the surface 2b of the second optical member x <x t4 f tb (x): Function describing the surface tb of the junction x t4 <x <x t3 f 1b '(x ), F 2b '(x), f tb ' (x): Functions representing the inclination of the surface x t3 , x t4 : The position vector of the joint is satisfied.
【0013】又、本発明の光学部材の構成は、 (1−2) 所定の曲率の面1aを有する第1の光学部
品と、該面1aの延長面と異なる面2aを有する第2の
光学部品とが、ベジェ曲線を利用した滑らかな接合面を
有する接合部分で繋がっており、且つ一体成形によって
製作されたものであることを特徴としている。Further, the structure of the optical member of the present invention includes (1-2) a first optical component having a surface 1a having a predetermined curvature and a second optical member having a surface 2a different from an extension surface of the surface 1a. The parts are connected to each other at a joint part having a smooth joint surface using a Bezier curve, and are manufactured by integral molding.
【0014】特に、(1−2−1) 前記第1の光学部
品は所定の曲率の面1bを有し、前記第2の光学部品は
該面1bの延長面と異なる面2bを有し、該面1bと該
面2bとが、ベジェ曲線を利用した滑らかな接合面で繋
がっていること等を特徴としている。In particular, (1-2-1) the first optical component has a surface 1b having a predetermined curvature, and the second optical component has a surface 2b different from an extension surface of the surface 1b, The surface 1b and the surface 2b are connected by a smooth joint surface using a Bezier curve.
【0015】[0015]
【実施例】図1は本発明の実施例1の斜視図である。本
実施例は所定の曲率の反射面1a(第1面)を持つ反射
部品(第1の光学部品)Aと、反射面1aの延長面と異
なる反射面2a(第2面)を持つ反射部品(第2の光学
部品)Bとを接合部分Tを介して一体に接合した形状の
光学部材を示している。本実施例の光学部材は例えば画
像表示装置の反射光学系の一部を構成している。EXAMPLE 1 FIG. 1 is a perspective view of Example 1 of the present invention. In this embodiment, a reflective component (first optical component) A having a reflective surface 1a (first surface) having a predetermined curvature, and a reflective component having a reflective surface 2a (second surface) different from the extended surface of the reflective surface 1a. An optical member having a shape in which (second optical component) B and a second portion are integrally joined via a joint portion T is shown. The optical member of this embodiment constitutes, for example, a part of the reflective optical system of the image display device.
【0016】本実施例において第1面1aと第2面2a
とを滑らかに接合する接合面taの構成について説明す
る。座標系を図2のようにとり、第1面1aの形状をf
1a(x,y)、第2面2aの形状をf2a(x,y)、接合面taの
形状をfta(x,y)なる関数で表わす。これらの関数として
は例えば球面、回転対象非球面、回転非対称非球面等が
考えられる。なお、 f1a(x,y)の有効領域(使用領域)は x>x1 f2a(x,y)の有効領域(使用領域)は x<x2 である。In this embodiment, the first surface 1a and the second surface 2a
The structure of the joint surface ta for smoothly joining and will be described. The coordinate system is set as shown in Fig. 2, and the shape of the first surface 1a is f
1a (x, y), the shape of the second surface 2a is f 2a (x, y), and the shape of the joint surface ta is f ta (x, y). Examples of these functions include a spherical surface, an aspherical surface to be rotated, and a rotationally asymmetrical aspherical surface. The effective area (used area) of f 1a (x, y) is x> x1 The effective area (used area) of f 2a (x, y) is x <x2.
【0017】図3(A)は第1面1aと第2面2aのy=
0 断面の境界付近の拡大図である。このx-z 断面図で見
ても関数f1a(x,0)と関数f2a(x,0)は高さ(z 値)がずれ
ているだけでなく、面の傾きも大きく異なっている。そ
して面1aを面2aの方向へ延長した場合、面2aは面
1aの延長線には乗っておらず、面2aは面1aの延長
線と明らかに異なっている。もし仮に関数f1a(x,y)、f
2a(x,y)を延長して接合部領域で交わったとしても、そ
の交点において不連続になる。更に、図3(B)はx=x
1,x2 でのy-z 断面図を示すものである。この断面図で
も2つの曲線は位置形状共に異なっている。In FIG. 3A, y = 1 on the first surface 1a and the second surface 2a.
It is an enlarged view near the boundary of 0 cross section. Even in this xz cross-sectional view, not only the height (z value) of the function f 1a (x, 0) and the function f 2a (x, 0) are different, but also the inclination of the surface is greatly different. When the surface 1a is extended in the direction of the surface 2a, the surface 2a is not on the extension line of the surface 1a, and the surface 2a is clearly different from the extension line of the surface 1a. If the function f 1a (x, y), f
Even if 2a (x, y) is extended and intersects at the junction area, it becomes discontinuous at the intersection. Furthermore, in FIG. 3B, x = x
It shows the yz cross section at 1, x2. Also in this cross-sectional view, the two curves have different position shapes.
【0018】そこでx=x1に於いて第1面1aと接合面t
aを、又x=x2に於いて接合面taと第2面2aを、x-z
、y-z 両断面とも滑らかに繋ぐ接合面taの関数f
ta(x,y)を決定する。接合面taの関数fta(x,y)が第1
面1aと第2面2aとに滑らかに繋がる為に、この接合
面taは f1a(x1,y)= fta(x1,y) f2a(x2,y)= fta(x2,y)Therefore, at x = x1, the first surface 1a and the joint surface t
a, and the joint surface ta and the second surface 2a at x = x2, xz
, Yz Function f of joint surface ta that smoothly connects both cross sections
Determine ta (x, y). The function f ta (x, y) of the joint surface ta is the first
This joint surface ta is f 1a (x1, y) = f ta (x1, y) f 2a (x2, y) = f ta (x2, y) in order to smoothly connect the surface 1a and the second surface 2a.
【0019】[0019]
【数1】 の条件を満たすようにしている。[Equation 1] I am trying to meet the condition of.
【0020】図4は上記の条件を満たして決定した接合
面taの関数fta(x,y)により繋がれた2つの反射面のy=
0 におけるx-z 断面図である。図5は接合面taの付近
の拡大図でる。両図よりわかる如く第1面1aと第2面
2aとはx=x1,x2 において接合面taと滑らかに繋がっ
ている。FIG. 4 shows y = 2 of two reflecting surfaces connected by the function f ta (x, y) of the joint surface ta determined by satisfying the above conditions.
It is a xz sectional view in 0. FIG. 5 is an enlarged view of the vicinity of the joint surface ta. As can be seen from both figures, the first surface 1a and the second surface 2a are smoothly connected to the joint surface ta at x = x1, x2.
【0021】次に2つの反射面の裏側,即ち第1の光学
部品Aの面1bと第2の光学部品Bの面2bを繋ぐ。夫
々の面を表す関数をf1b(x,y)、f2b(x,y)とすると、反射
面側で決定したと同じ方法で接合部分Tの接合面tbの
関数ftb(x,y)を求め、これによって面1b,面tb、面
2bを滑らかに繋いで、光学部材の両面を決定してい
る。Next, the back sides of the two reflecting surfaces, that is, the surface 1b of the first optical component A and the surface 2b of the second optical component B are connected. If the functions representing the respective surfaces are f 1b (x, y) and f 2b (x, y), the function f tb (x, y) of the joint surface tb of the joint portion T is determined by the same method as that determined on the reflecting surface side. ) Is obtained, and the surface 1b, the surface tb, and the surface 2b are smoothly connected to determine both surfaces of the optical member.
【0022】このようにして決定した光学部品は、その
両面とも全面が滑らかな曲線で構成される為、成型加工
で製作する際にも、部品の接合部分に応力が残らず、加
工後の変形、破損等も生じない精度の良い光学部材を得
ることができる。Since the entire surface of the optical component determined in this way is composed of smooth curves on both sides, no stress remains at the joint portion of the component even when it is manufactured by molding, and deformation after processing occurs. Thus, it is possible to obtain an optical member with high accuracy that does not cause damage or the like.
【0023】又、本発明においては第1面と第2面との
接合面をベジェ曲線を利用して滑らかな曲線で結合して
も良い。例えば、図6に示すようにx<x1の範囲では関数
f1a(x)で定義され、 x>x2 の範囲では関数f2a(x)で定義
される2つの面を有する光学部材に於いて、x1<x<x2 の
範囲を接合面として記述する場合、図6に示す関数w
1(x),w2(x) ,例えば余弦関数 w1=[1+cos{(x-x1)
/(x2-x1)*π}]/2 w2=[1+cos{(x-x2)/(x2-x1)*π}]/2 を考え、接合面の関数をfta(x)=f1a(x)* w1(x)+f2a(x)*
w2(x)とすれば関数f1a(x)と関数f2a(x)とを滑らかに繋
ぐことが出来る。接合面をベジェ曲線で繋げば、接合面
の設計が容易になるという利点が生じる。Further, in the present invention, the joining surface of the first surface and the second surface may be joined by a smooth curve using a Bezier curve. For example, as shown in Fig. 6, the function is in the range of x <x1.
When describing a range of x1 <x <x2 as a cemented surface in an optical member that has two surfaces defined by f 1a (x) and a function f 2a (x) in the range of x> x2 , The function w shown in FIG.
1 (x), w 2 (x), eg cosine function w 1 = [1 + cos {(x-x1)
Considering / (x2-x1) * π}] / 2 w 2 = [1 + cos {(x-x2) / (x2-x1) * π}] / 2, the function of the interface is f ta (x) = f 1a (x) * w 1 (x) + f 2a (x) *
If w 2 (x), the function f 1a (x) and the function f 2a (x) can be smoothly connected. Connecting the joining surfaces with a Bezier curve has the advantage of facilitating the design of the joining surfaces.
【0024】[0024]
【発明の効果】本発明によれば以上の構成により、複数
の光学部品を1つの光学部材として一体成形する際に、
複数の光学部品を接合する接合部分の繋ぎ面形状を適切
に構成し、光学部品と接合部分との境界において、2つ
の面を滑らかに繋ぎ、これによって成型加工時の光学部
材への残留応力を減少して製造誤差の発生を少なくす
る。これによって部品数を削減し、組み立て作業の工数
を削減して、コストダウンを実現する高精度の光学部材
を達成することができる。According to the present invention, with the above configuration, when integrally molding a plurality of optical components as one optical member,
Appropriately configure the joint surface shape of the joint part that joins multiple optical parts, and smoothly connect the two surfaces at the boundary between the optical part and the joint part, which reduces residual stress on the optical member during molding. This reduces the number of manufacturing errors. As a result, it is possible to reduce the number of parts, reduce the number of assembling steps, and achieve a highly accurate optical member that realizes cost reduction.
【図1】 本発明の実施例1の斜視図FIG. 1 is a perspective view of a first embodiment of the present invention.
【図2】 図1の実施例の第1面、第2面及び座標系を
示す図FIG. 2 is a diagram showing a first surface, a second surface, and a coordinate system of the embodiment of FIG.
【図3】 図1の実施例の第1面、第2面の接合部付近
の拡大断面図FIG. 3 is an enlarged cross-sectional view in the vicinity of a joint between the first surface and the second surface of the embodiment shown in FIG.
【図4】 図1の実施例の第1面、第2面、接合面の断
面図FIG. 4 is a cross-sectional view of the first surface, the second surface, and the bonding surface of the embodiment of FIG.
【図5】 図1の実施例の接合面付近の断面図5 is a cross-sectional view of the vicinity of the joint surface of the embodiment of FIG.
【図6】 本発明の光学部材の第1面と第2面とをベジ
ェ曲線で繋ぐ概念図FIG. 6 is a conceptual diagram in which the first surface and the second surface of the optical member of the present invention are connected by a Bezier curve.
A 反射部品(光学部品) B 反射部品(光学部品) T 接合部分 1a 反射面(第1面)、面形状の関数f1a(x,y) 2a 反射面(第2面)、面形状の関数f2a(x,y) 1b 面1aの裏面、 面形状の関数f1b(x,y) 2b 面2aの裏面、 面形状の関数f2b(x,y) ta 接合面、面形状の関数fta(x,y) tb 接合面、面形状の関数ftb(x,y)A reflective component (optical component) B reflective component (optical component) T joint part 1a reflective surface (first surface), surface shape function f 1a (x, y) 2a reflective surface (second surface), surface shape function f 2a (x, y) 1b Backside of surface 1a, surface shape function f 1b (x, y) 2b Backside of surface 2a, surface shape function f 2b (x, y) ta Join surface, surface shape function f ta (x, y) tb Joint surface, surface shape function f tb (x, y)
Claims (4)
部品と、該面1aの延長面と異なる面2aを有する第2
の光学部品とが、接合部分を介して繋がっており、更に
該面1a及び該面2aと該接合部分の境界は滑らかに繋
がっており、且つ条件 f1a(xt1)=fta(xt1) 、 f2a(xt2)=fta(xt2) f1a'(xt1)=fta'(xt1)、 f2a'(xt2)=fta'(xt2) 但し、 f1a(x) :第1の光学部材の面1aを記述する関数 x>x
t1 f2a(x) :第2の光学部材の面2aを記述する関数 x<xt2 fta(x) :接合部分の面taを記述する関数 xt2<x<xt1 f1a'(x)、 f2a'(x)、 fta'(x):面の傾きを表す関数 xt1 、xt2 : 接合部の位置ベクトル を満たした、一体成形によって製作されたものであるこ
とを特徴とする光学部材。1. A first optical component having a surface 1a having a predetermined curvature, and a second optical component having a surface 2a different from an extension surface of the surface 1a.
Of the optical components are connected via a joint portion, and the surfaces 1a and 2a and the boundary between the joint portion are smoothly connected, and the condition f 1a (x t1 ) = f ta (x t1 ), F 2a (x t2 ) = f ta (x t2 ) f 1a '(x t1 ) = f ta ' (x t1 ), f 2a '(x t2 ) = f ta ' (x t2 ), where f 1a (x): Function x> x describing the surface 1a of the first optical member
t1 f 2a (x): Function describing surface 2a of the second optical member x <x t2 f ta (x): Function describing surface ta of the joint part x t2 <x <x t1 f 1a '(x ), F 2a '(x), f ta ' (x): Functions representing the inclination of the surface x t1 , x t2 : It is characterized by being manufactured by integral molding that satisfies the position vector of the joint. Optical member to do.
bを有し、前記第2の光学部品は該面1bの延長面と異
なる面2bを有し、該面1bと該面2bとが、前記接合
部分を介して繋がっており、更に該面1b及び該面2b
と該接合部分の境界は滑らかに繋がっており、且つ条件 f1b(xt3)=ftb(xt3) 、 f2b(xt4)=ftb(xt4) f1b'(xt3)=ftb'(xt3)、 f2b'(xt4)=ftb'(xt4) 但し、 f1b(x) :第1の光学部材の面1bを記述する関数 x>x
t3 f2b(x) :第2の光学部材の面2bを記述する関数 x<xt4 ftb(x) :接合部分の面tbを記述する関数 xt4<x<xt3 f1b'(x)、 f2b'(x)、 ftb'(x):面の傾きを表す関数 xt3 、xt4 : 接合部の位置ベクトル を満たしたことを特徴とする請求項1の光学部材。2. The first optical component is a surface 1 having a predetermined curvature.
b, the second optical component has a surface 2b different from the extension surface of the surface 1b, the surface 1b and the surface 2b are connected to each other through the joint portion, and the surface 1b is further provided. And the surface 2b
And the boundary of the joint are smoothly connected, and the conditions f 1b (x t3 ) = f tb (x t3 ), f 2b (x t4 ) = f tb (x t4 ) f 1b '(x t3 ) = f tb '(x t3 ), f 2b ' (x t4 ) = f tb '(x t4 ), where f 1b (x): Function x> x describing the surface 1b of the first optical member.
t3 f 2b (x): Function describing the surface 2b of the second optical member x <x t4 f tb (x): Function describing the surface tb of the junction x t4 <x <x t3 f 1b '(x ), F 2b '(x), f tb ' (x): a function x t3 , x t4 representing the inclination of the surface: x t4 : a position vector of the joint, The optical member according to claim 1.
部品と、該面1aの延長面と異なる面2aを有する第2
の光学部品とが、ベジェ曲線を利用した滑らかな接合面
を有する接合部分で繋がっており、且つ一体成形によっ
て製作されたものであることを特徴とする光学部材。3. A first optical component having a surface 1a having a predetermined curvature, and a second optical component having a surface 2a different from an extension surface of the surface 1a.
The optical member is connected with a joint portion having a smooth joint surface using a Bezier curve, and is manufactured by integral molding.
bを有し、前記第2の光学部品は該面1bの延長面と異
なる面2bを有し、該面1bと該面2bとが、ベジェ曲
線を利用した滑らかな接合面で繋がっていることを特徴
とする請求項3の光学部材。4. The first optical component is a surface 1 having a predetermined curvature.
b, the second optical component has a surface 2b different from the extension surface of the surface 1b, and the surface 1b and the surface 2b are connected by a smooth joint surface using a Bezier curve. The optical member according to claim 3, wherein
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28918594A JPH08122505A (en) | 1994-10-27 | 1994-10-27 | Optical member |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP28918594A JPH08122505A (en) | 1994-10-27 | 1994-10-27 | Optical member |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH08122505A true JPH08122505A (en) | 1996-05-17 |
Family
ID=17739878
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP28918594A Pending JPH08122505A (en) | 1994-10-27 | 1994-10-27 | Optical member |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH08122505A (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1271188A2 (en) * | 2001-06-26 | 2003-01-02 | Canon Kabushiki Kaisha | Reflecting optical element, projection type image display apparatus, and method for fabricating said reflecting optical element |
US6637899B2 (en) | 1998-09-25 | 2003-10-28 | Canon Kabushiki Kaisha | Optical element and optical system having the same |
JP2016038515A (en) * | 2014-08-08 | 2016-03-22 | Japan 3D Devices株式会社 | Glass substrate for concave mirror |
-
1994
- 1994-10-27 JP JP28918594A patent/JPH08122505A/en active Pending
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
US6637899B2 (en) | 1998-09-25 | 2003-10-28 | Canon Kabushiki Kaisha | Optical element and optical system having the same |
EP1271188A2 (en) * | 2001-06-26 | 2003-01-02 | Canon Kabushiki Kaisha | Reflecting optical element, projection type image display apparatus, and method for fabricating said reflecting optical element |
EP1271188A3 (en) * | 2001-06-26 | 2003-07-02 | Canon Kabushiki Kaisha | Reflecting optical element, projection type image display apparatus, and method for fabricating said reflecting optical element |
JP2016038515A (en) * | 2014-08-08 | 2016-03-22 | Japan 3D Devices株式会社 | Glass substrate for concave mirror |
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