JPH0793670B2 - Image reader - Google Patents

Image reader

Info

Publication number
JPH0793670B2
JPH0793670B2 JP1259483A JP25948389A JPH0793670B2 JP H0793670 B2 JPH0793670 B2 JP H0793670B2 JP 1259483 A JP1259483 A JP 1259483A JP 25948389 A JP25948389 A JP 25948389A JP H0793670 B2 JPH0793670 B2 JP H0793670B2
Authority
JP
Japan
Prior art keywords
original
document
light source
reading
condenser lens
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 - Fee Related
Application number
JP1259483A
Other languages
Japanese (ja)
Other versions
JPH03121653A (en
Inventor
求 深澤
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Canon Inc
Original Assignee
Canon Inc
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Canon Inc filed Critical Canon Inc
Priority to JP1259483A priority Critical patent/JPH0793670B2/en
Publication of JPH03121653A publication Critical patent/JPH03121653A/en
Publication of JPH0793670B2 publication Critical patent/JPH0793670B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は画像読取装置に関し、特に線状光源(蛍光灯や
ハロゲンランプ又は複数の発光素子を一次元方向に配列
したLEDアレイ光源等)と特定形状の集光レンズを用い
て原稿面を斜め方向から照明し、該原稿からの反射光束
又は透過光束を結像レンズ系を介して撮像素子面上に結
像させて該原稿面上の画像情報を順次高精度に読み取る
ようにした例えば複写機、ファクシミリ、イメージスキ
ャナー等に好適な画像読取装置に関するものである。
The present invention relates to an image reading device, and in particular to a linear light source (such as a fluorescent lamp, a halogen lamp, or an LED array light source in which a plurality of light emitting elements are arranged in a one-dimensional direction). An image on the surface of the original is formed by illuminating the surface of the original from a diagonal direction using a condenser lens of a specific shape, and forming an image of the reflected light beam or the transmitted light beam from the original document on the image pickup element surface via the imaging lens system. The present invention relates to an image reading apparatus suitable for, for example, a copying machine, a facsimile, an image scanner or the like, which sequentially reads information with high accuracy.

(従来の技術) 従来より画像読取装置においては原稿面を照明する照明
部として棒状の集光レンズ付のLEDアレイを用いて該原
稿面を斜め方向から照明しているものが知られている。
(Prior Art) It has been known that an image reading apparatus illuminates a document surface from an oblique direction by using an LED array with a rod-shaped condenser lens as an illumination unit for illuminating the document surface.

そして該原稿面からの光束を結像レンズ系を介してCCD
等の撮像素子面上に結像させて原稿面よりの画像情報を
読み取っている。
Then, the light flux from the document surface is passed through the imaging lens system to the CCD.
The image information is read from the original surface by forming an image on the surface of the image pickup device such as.

この様な画像読取装置においてCCD等の撮像素子を用い
て原稿面上の画像情報の読取りを行う場合には原稿面の
照度分布(光量分布)は、できるだけ均一であることが
読取精度を向上させるのに好ましい。
In such an image reading apparatus, when the image information on the document surface is read by using an image pickup device such as a CCD, the illuminance distribution (light amount distribution) on the document surface should be as uniform as possible to improve the reading accuracy. Is preferred.

第9図は従来のこの種の画像読取装置の要部概略図と原
稿面における照度分布を示した説明図である。
FIG. 9 is a schematic view of a main part of a conventional image reading apparatus of this type and an explanatory view showing an illuminance distribution on a document surface.

同図において90は集光レンズ付LEDアレイ(原稿照明
部)であり線状光源(LEDアレイ光源)91と棒状の集光
用の集光レンズ92より構成されており、原稿3を斜め下
方向から照明している。
In the figure, 90 is an LED array with a condensing lens (document illuminating section), which is composed of a linear light source (LED array light source) 91 and a rod-shaped condensing lens 92 for condensing the document 3 in an oblique downward direction. Lighting from.

3は原稿(例えば反射原稿又は透過原稿)であり後述す
る搬送ローラ7によって矢印Dの如く副走査方向に移動
している。
Reference numeral 3 is an original (for example, a reflective original or a transparent original), which is moved in the sub-scanning direction as indicated by an arrow D by a conveyance roller 7 described later.

6は反射ミラーであり、原稿3からの反射光束を後述す
る結像手段4側に反射させることにより光路を折り曲げ
ている。4は結像手段であり原稿3からの反射光束を撮
像素子(イメージセンサー)5面上に結像させている。
撮像素子5は一次元より成る例えばCCD等から成ってい
る。搬送ローラ7は原稿3を読み取り方向に応じて搬送
させている。
Reference numeral 6 denotes a reflecting mirror, which bends the optical path by reflecting the light flux reflected from the original 3 toward the image forming means 4 described later. An image forming unit 4 forms an image of the reflected light flux from the original 3 on the surface of an image sensor (image sensor) 5.
The image pickup device 5 is composed of a one-dimensional CCD, for example. The conveyance roller 7 conveys the document 3 according to the reading direction.

同図において線状光源91から発光した光束は棒状の集光
レンズ92で集光され、該集光レンズ92により原稿3の読
取位置Aを中心に所定領域を斜め下方より照明してい
る。
In the figure, the light flux emitted from the linear light source 91 is condensed by a rod-shaped condenser lens 92, and the condenser lens 92 illuminates a predetermined area from the reading position A of the original 3 obliquely from below.

そして照明された原稿3からの反射光束は反射ミラー6
を介して結像手段4により撮像素子5面上に結像され、
これにより原稿3面上の画像情報を読取っている。
The reflected light flux from the illuminated original 3 is reflected by the reflection mirror 6.
An image is formed on the surface of the image sensor 5 by the image forming means 4 via
As a result, the image information on the third surface of the document is read.

第10図はこのときの線状光源91から発する光束の空間へ
の発光エネルギー放出分布を示した説明図と後述する仮
想平面πの定義を説明する説明図である。
FIG. 10 is an explanatory view showing the emission energy emission distribution to the space of the luminous flux emitted from the linear light source 91 at this time and an explanatory view for explaining the definition of a virtual plane π described later.

同図に示した様に通常線状光源91から放出される光束の
発光エネルギーの強度の値がピーク(最大)になる方向
は線状光源91の基板91aに対して略垂直上方である。
As shown in the figure, the direction in which the intensity value of the luminous energy of the luminous flux emitted from the normal linear light source 91 reaches a peak (maximum) is substantially vertically above the substrate 91a of the linear light source 91.

この発光エネルギーの強度の値が最大値をとる方向Yと
線状光源の長手方向(例えばLEDアレイのチップ配列方
向)Xとの2方向によって形成される仮想平面を以下仮
想平面πと定義する。
An imaginary plane formed by two directions, that is, the direction Y in which the value of the intensity of the emission energy has the maximum value and the longitudinal direction of the linear light source (for example, the chip array direction of the LED array) X is defined as a virtual plane π.

尚、仮想平面πは線状光源91の基板91aに対し線状光源9
1を含む直交平面で与えられる。
The virtual plane π is the linear light source 9 with respect to the substrate 91a of the linear light source 91.
Given in an orthogonal plane containing 1.

ここで前記第9図で示した従来の原稿照明部90を構成す
る棒状の集光レンズ92の原稿面3と仮想平面πに直交す
る断面形状は一般にこの仮想平面πを境にして対称面と
する面対称となっている。
Here, the cross-sectional shape orthogonal to the original plane 3 and the virtual plane π of the rod-shaped condenser lens 92 constituting the conventional original illumination unit 90 shown in FIG. 9 is generally a plane of symmetry with the virtual plane π as a boundary. It is symmetrical to the plane.

(発明が解決しようとする問題点) しかしながらこの様な棒状の集光レンズを用いて原稿を
斜め下方向より照明すると下記のような問題点が生じて
くる。
(Problems to be Solved by the Invention) However, when a document is illuminated obliquely from below by using such a rod-shaped condenser lens, the following problems occur.

線状光源(発光点)91から集光レンズ92を通過して原
稿面上の読取位置Bに到達するまでの光路長は線状光源
91から集光レンズ92を通過して原稿3面上の読取位置C
に到達するまでの光路長よりも短いことから読取位置B
の方が読取位置Cよりも照度が高くなる。
The optical path length from the linear light source (light emitting point) 91 to the reading position B on the document surface after passing through the condenser lens 92 is the linear light source.
Scanning position C on the 3rd side of the original from 91 through the condenser lens 92
Since it is shorter than the optical path length to reach the reading position B
Has higher illuminance than the reading position C.

集光レンズ92の中心を通過した光束と周辺部を通過し
た光束の焦点を結ぶ結像位置がズレてしまい、特に周辺
部を通過した光束は強く曲げられ内側に周り込む現象、
所謂負の球面収差が生じてくる。
A phenomenon in which the image forming position where the focal point of the light flux passing through the center of the condenser lens 92 and the focal point of the light flux passing through the peripheral portion are displaced, and in particular the light flux passing through the peripheral portion is strongly bent and goes around inward,
So-called negative spherical aberration occurs.

この為第9図の原稿面における照度分布に示すように各
々の読取位置B、Cの原稿面照度にリップルが生じてく
る。
Therefore, as shown in the illuminance distribution on the document surface of FIG. 9, ripples occur in the illuminance of the document surface at each of the reading positions B and C.

この様な現象が現われる結果、装置のメカ精度による原
稿読取位置のズレ(読取位置B−C間)における照度の
バラツキΔEが大きなものとなり原稿面上での照度分布
の不均一さを生じさせてくる。
As a result of the appearance of such a phenomenon, the variation ΔE of the illuminance at the deviation of the document reading position (between the reading positions B and C) due to the mechanical precision of the apparatus becomes large and the unevenness of the illuminance distribution on the document surface is caused. come.

この為従来の画像読取装置では装置設計上において信号
出力のマージン設定が困難をきわめ、厳しいメカ精度の
要求や調整項目が増えること等により装置のコストアッ
プの要因となってくる。
For this reason, in the conventional image reading apparatus, it is difficult to set a margin for signal output in designing the apparatus, and strict mechanical precision requirements and adjustment items increase, which causes a cost increase of the apparatus.

本発明は前述した従来の画像読取装置の問題点を解決す
る為に仮想平面πに対して集光レンズの形状を適切に形
成し、若しくは集光レンズの位置を偏心させることによ
り、原稿の読取位置がずれた際に生じる原稿面上の照度
のバラツキを小さく抑えることができ、高精度な読取り
を図りつつメカ精度を緩和し、調整項目を増やさずに容
易に組立てることができる安価な構成の画像読取装置の
提供を目的とする。
In order to solve the above-mentioned problems of the conventional image reading apparatus, the present invention appropriately forms the shape of the condenser lens with respect to the virtual plane π or decenters the position of the condenser lens to read a document. The variation in illuminance on the document surface that occurs when the position is misaligned can be suppressed to a small value, the mechanical precision is relaxed while achieving high-accuracy reading, and the assembly can be easily assembled without increasing the adjustment items. An object is to provide an image reading device.

(問題点を解決する為の手段) 本発明の画像読取装置は、原稿面上の読取面を該読取面
に対し斜め方向から線状光源からの光束により照明し、
該読取面からの光束を結像手段により撮像素子面上に結
像させ、前記原稿面上の画像情報を読み取る画像読取装
置において、前記線状光源と前記原稿面との間に集光レ
ンズを設け、該集光レンズは、前記線状光源の発光エネ
ルギー強度が最大値をとる方向と前記線状光源の長手方
向との2方向より形成される平面πに対して非面対称な
形状の屈折面を有し、該平面πより該原稿面に近い方の
屈折面の曲率半径をRa、該平面πより該原稿面に遠い方
の屈折面の曲率半径をRbとしたとき、Ra>Rbとなるよう
にして該原稿面上の照度分布の均一化を図っていること
を特徴としている。
(Means for Solving Problems) An image reading apparatus of the present invention illuminates a reading surface on a document surface with a light beam from a linear light source obliquely with respect to the reading surface,
In an image reading device for reading the image information on the document surface by forming an image of the light flux from the reading surface on the image pickup element surface by an image forming means, a condenser lens is provided between the linear light source and the document surface. The condensing lens is provided with a refraction of a non-symmetrical shape with respect to a plane π formed by two directions of a direction in which the emission energy intensity of the linear light source has a maximum value and a longitudinal direction of the linear light source. Ra> Rb, where Ra is the radius of curvature of a refracting surface closer to the original surface than the plane π and Ra is Rb, and Rb is the radius of refraction surface farther away from the original surface than the plane π. In this way, the illuminance distribution on the document surface is made uniform.

(実施例) 第1図は本発明の一実施例の画像読取装置の要部概略図
である。
(Embodiment) FIG. 1 is a schematic view of a main part of an image reading apparatus according to an embodiment of the present invention.

同図において第9図に示した要素と同一要素には同符番
を付している。
In the figure, the same elements as those shown in FIG. 9 are designated by the same reference numerals.

1は線状光源であり例えば複数の発光素子を一次元方向
に配列したLEDアレイ光源、ハロゲンランプ、そして蛍
光灯等より成っており、原稿3に対して斜め方向に配置
している。
Reference numeral 1 denotes a linear light source, which includes, for example, an LED array light source in which a plurality of light emitting elements are arranged in a one-dimensional direction, a halogen lamp, a fluorescent lamp, and the like, and is arranged obliquely with respect to the original 3.

2は本発明に係る集光レンズであり原稿3の読取装置と
線状光源1との間に設けられている。集光レンズ2は前
述した仮想平面πに対して屈折面が非面対称であり、線
状光源1の長手方向、例えば複数の発光素子が並んでい
る方向に対して棒状の形状より形成されている。
Reference numeral 2 denotes a condenser lens according to the present invention, which is provided between the reading device for the original 3 and the linear light source 1. The condensing lens 2 has a refraction surface that is asymmetric with respect to the virtual plane π described above, and is formed in a rod shape in the longitudinal direction of the linear light source 1, for example, the direction in which a plurality of light emitting elements are arranged. There is.

本実施例では線状光源1と集光レンズ2の各要素で原稿
照明部10を構成しており、該原稿照明部10より原稿3を
斜め下方向から照明している。
In the present embodiment, each element of the linear light source 1 and the condenser lens 2 constitutes a document illuminating section 10, and the document illuminating section 10 illuminates the document 3 obliquely from below.

本実施例においては原稿照明部10で照明された原稿3を
搬送ローラ7により同図に示す矢印Dの如く副走査方向
に移動させながら該原稿3からの反射光束を反射ミラー
6を介して結像手段4により撮像素子5面上に結像させ
て順次原稿3面上の画像情報を読取っている。
In this embodiment, the original 3 illuminated by the original illuminating unit 10 is moved by the conveying roller 7 in the sub-scanning direction as indicated by arrow D in FIG. An image is formed on the surface of the image sensor 5 by the image means 4 and the image information on the surface of the original 3 is read sequentially.

次に本発明に係る集光レンズ2の形状及び光学的作用に
ついて第2図を用いて説明する。
Next, the shape and optical action of the condenser lens 2 according to the present invention will be described with reference to FIG.

第2図は第1図に示した線状光源1及び集光レンズ2の
一部分を拡大した断面説明図である。
FIG. 2 is an enlarged cross-sectional explanatory view of a part of the linear light source 1 and the condenser lens 2 shown in FIG.

同図において集光レンズ2は仮想平面πに対して左右非
対称(非面対称)な面形状より成っている。
In the figure, the condenser lens 2 has a surface shape that is asymmetrical (non-plane symmetric) with respect to the virtual plane π.

具体的には集光レンズ2の入射面と光軸との交点aから
基板1aとの間隔d0をd0=1と基準にしたとき、交点aか
ら集光レンズ2の射出面と光軸との交点bまでの間隔d1
をd1=11、入射面側のレンズ面2aの曲率半径R2をR2=
5、射出面側レンズ面2bのうち片側の面2b1の曲率半径R
1をR1=6、そして集光レンズ2の幅寸法DをD=8の
比率にして集光レンズ2の各部の寸法を設定している。
Specifically, when the distance d 0 from the intersection a between the incident surface of the condenser lens 2 and the optical axis to the substrate 1a is set as d 0 = 1, the exit surface of the condenser lens 2 and the optical axis from the intersection a. interval d 1 to an intersection b of the
Is d 1 = 11, the radius of curvature R2 of the lens surface 2a on the incident surface side is R2 =
5. Radius of curvature R of one surface 2b1 of the exit surface side lens surface 2b
1 is R1 = 6, and the width dimension D of the condenser lens 2 is set to a ratio of D = 8 to set the dimensions of each part of the condenser lens 2.

又非対称部分である集光レンズ2の射出面側の図面上左
側の部分の面2b2(第1図において原稿面3に近い部
分)、例えば曲率中心Oからみて仮想平面πより30゜を
越えた部分2b2にはパワー(屈折力)をつけていない。
即ちこのノンパワー部2b2を平面より形成して他の部分2
b1(パワー部)をシリンドリカル形状より形成してい
る。これにより仮想平面πに対し左右非対称な形成を成
している。
The surface 2b2 (the portion near the original surface 3 in FIG. 1) on the left side of the drawing on the exit surface side of the condenser lens 2 which is an asymmetric portion, for example, exceeds 30 ° from the virtual plane π when viewed from the center of curvature O. No power (refractive power) is attached to the portion 2b2.
That is, the non-power portion 2b2 is formed from a flat surface and the other portion 2
The b1 (power part) is formed in a cylindrical shape. This forms a left-right asymmetry with respect to the virtual plane π.

この様な形状の集光レンズ2のノンパワー部2b2を通過
した線状光源1からの光束は原稿3の読取位置には集光
しない。この為原稿3を照明する為の照度は低下するが
読取位置B付近では球面収差による光束の周り込み現象
は発生しない。
The light beam from the linear light source 1 that has passed through the non-power portion 2b2 of the condenser lens 2 having such a shape is not condensed at the reading position of the original 3. For this reason, the illuminance for illuminating the original 3 is reduced, but in the vicinity of the reading position B, the phenomenon of the light flux wrapping around due to spherical aberration does not occur.

本実施例ではこの光学的作用を利用して原稿面上の読取
位置B−A間の照度分布にリップルが生じないようにし
ている。
In this embodiment, this optical action is used to prevent ripples from occurring in the illuminance distribution between the reading positions B-A on the document surface.

一方、仮想平面πに対して射出面の図面上右側の部分2b
1の形状は前記第9図で示した従来の集光レンズ92の形
状(シリンドリカル形状)と同様であるので読取位置A
より読取位置Cの方向に向うにつれて照明照度は低下す
るが、球面収差による周り込み現象により再び照明照度
は上り結局読取位置Bから読取位置Cまでは第3図に示
すように照度のバラツキをΔEだけ小さく抑えたブロー
ド(幅広い)な原稿面照度分布を得ることができる。
On the other hand, the portion 2b on the right side in the drawing of the exit surface with respect to the virtual plane π
The shape of 1 is the same as the shape (cylindrical shape) of the conventional condenser lens 92 shown in FIG.
The illumination illuminance decreases more toward the reading position C, but the illumination illuminance rises again due to the rounding phenomenon due to spherical aberration, and eventually the illuminance variation ΔE from the reading position B to the reading position C as shown in FIG. It is possible to obtain a broad (wide) original surface illuminance distribution that is kept small.

特に第3図の点線で示した従来の原稿読取位置B−A間
の照度分布に比べて本実施例では同図の実線で示したよ
うに照度のバラツキがΔEとなり、極めて小さく抑えた
照度分布を得ている。これにより原稿読取位置B−C間
の照度の均一化を図っている。
In particular, compared with the conventional illuminance distribution between the document reading positions B-A shown by the dotted line in FIG. 3, the variation in illuminance becomes ΔE as shown by the solid line in FIG. Is getting Thereby, the illuminance between the document reading positions B and C is made uniform.

この様に本実施例では集光レンズ2の屈折面形状を前述
したように仮想平面πに対し非面対称となるように形成
し、線状光源1から発光される光束を集光レンズ2によ
り効率良く原稿面上を照射させ原稿面における照度分布
の均一化を図り精度の良い読取りを行っている。
As described above, in the present embodiment, the refracting surface shape of the condenser lens 2 is formed so as to be asymmetric with respect to the virtual plane π as described above, and the light flux emitted from the linear light source 1 is generated by the condenser lens 2. The original surface is efficiently irradiated to make the illuminance distribution on the original surface uniform, and accurate reading is performed.

尚、本実施例において集光レンズ2の原稿面と仮想平面
πに直交する断面形状をシリンドリカル形状と平面によ
って形成して原稿面における照度分布の均一化を図って
きたが仮想平面πを境にして非面対称な形成であればど
のような形状であっても良く、例えば非球面形状を用い
て該集光レンズ2の断面形状を形成しても本発明は前述
と同様に原稿面における照度分布の均一化を図ることが
できる。
In this embodiment, the cross-sectional shape of the condenser lens 2 orthogonal to the original surface and the virtual plane π is formed by the cylindrical shape and the flat surface to make the illuminance distribution uniform on the original surface. Any shape may be used as long as it is non-asymmetrical. For example, even if the cross-sectional shape of the condenser lens 2 is formed by using an aspherical shape, the present invention is similar to the above-mentioned illumination on the document surface. The distribution can be made uniform.

又第4図に示す様に2つの屈折面の曲率半径R1、R2を仮
想平面πを境にして図面上左右で異なる値としても良
く、例えばR1(左)>R2(右)となるようにして集光レ
ンズ2を形成しても前述の実施例と同様に原稿面上の照
度分布のバラツキΔEを小さく抑えることができる。
As shown in FIG. 4, the radii of curvature R1 and R2 of the two refracting surfaces may be different on the left and right in the drawing with the virtual plane π as a boundary, for example, R1 (left)> R2 (right). Even if the condensing lens 2 is formed by using the same, the variation ΔE in the illuminance distribution on the document surface can be suppressed to a small level as in the above-described embodiment.

第5図、第6図は各々本発明の他の一実施例の集光レン
ズの原稿面と仮想平面πに直交する断面方向に関する説
明図と原稿面における照度分布の説明図である。
FIG. 5 and FIG. 6 are explanatory views relating to a document surface of a condensing lens of another embodiment of the present invention and a sectional direction orthogonal to the virtual plane π, and an explanatory view of illuminance distribution on the document surface.

前述の実施例の集光レンズ2は、該集光レンズ2の形状
それ自体を仮想平面πに対して非面対称な形状になるよ
うに形成して線状光源1から発光された光束を集光レン
ズ2で集光し、該集光レンズ2により原稿3を斜め下方
向から照明する場合を示したが、第5図、第6図の各々
の実施例においては集光レンズ2の形状、それ自体は光
軸に対して左右対称な形状より構成し、該集光レンズ2
の対称面を仮想平面πに対して偏心させて原稿3を斜め
下方向から照明している。
The condenser lens 2 of the above-mentioned embodiment collects the luminous flux emitted from the linear light source 1 by forming the shape itself of the condenser lens 2 so as to have an asymmetric shape with respect to the virtual plane π. The case where the light is condensed by the optical lens 2 and the original 3 is illuminated from the obliquely downward direction by the condensing lens 2 is shown. In each of the embodiments shown in FIGS. 5 and 6, the shape of the condensing lens 2 is The condensing lens 2 itself has a shape symmetrical to the optical axis.
The symmetry plane of is eccentric with respect to the virtual plane π, and the original 3 is illuminated obliquely from below.

即ち仮想平面πに対して集光レンズ2の形状が非面対称
となるように集光レンズ2を偏心させていることを特徴
としている。
That is, the condensing lens 2 is decentered so that the shape of the condensing lens 2 is asymmetric with respect to the virtual plane π.

第5図、第6図の各々の実施例においての集光レンズ2
は光軸に対して左右対称なかまぼこ型の形状を有してい
る。
Condensing lens 2 in each of the embodiments shown in FIGS.
Has a semi-cylindrical shape which is symmetrical with respect to the optical axis.

第5図においては集光レンズ2を仮想平面πに対して並
行に距離lだけ並行偏心させて仮想平面πに対して非面
対称となるように構成している。
In FIG. 5, the condenser lens 2 is configured so as to be decentered parallel to the virtual plane π by a distance l so as to be asymmetric about the virtual plane π.

この時、偏心による左右非対称のコマ収差が発生し、同
図に示す様に原稿の読取位置A〜C間の領域にかけて
は、集光レンズ2の曲面に入射する角度が大きい為光束
の屈折する量が大きく強く曲げられて密になる傾向を示
している。
At this time, left-right asymmetrical coma aberration occurs due to decentering, and as shown in the figure, the light beam is refracted in the area between the reading positions A to C of the document because the angle of incidence on the curved surface of the condenser lens 2 is large. The amount is large and it is strongly bent and tends to become dense.

又読取位置A−B間の領域にかけては、逆に集光レンズ
2の曲面に入射する角度が小さい為光束の屈折する量が
小さく弱く曲げられ、疎になる傾向を示している。
On the other hand, in the area between the reading positions A and B, on the contrary, since the angle of incidence on the curved surface of the condenser lens 2 is small, the amount of refraction of the light beam is small and the light beam is weakly bent and tends to be sparse.

この結果、原稿面における照度のバラツキΔEは同図に
示した様に小さく抑えることができる。
As a result, the variation ΔE in illuminance on the document surface can be suppressed to a small level as shown in FIG.

この様に本実施例では集光レンズ2を仮想平面πに対し
て並行に偏心させたときに発生する偏心コマ収差を利用
して原稿を斜め下方向から照明する際に伴う読取位置B
(光路長の短い側)の照度が上がる現象を緩和させてい
る。これにより照度のバラツキΔEを小さく抑えて原稿
面の照度の均一化を図っている。
As described above, in the present embodiment, the reading position B that accompanies when the document is illuminated obliquely from below using the decentering coma aberration generated when the condenser lens 2 is decentered in parallel with the virtual plane π.
The phenomenon that the illuminance on the side (shorter optical path length) increases is mitigated. As a result, the variation ΔE of the illuminance is suppressed to be small, and the illuminance on the document surface is made uniform.

第6図においては集光レンズ2を基板1aに対し角度θだ
け傾き偏心させることにより仮想平面πに対して非面対
称となるように構成している。
In FIG. 6, the condenser lens 2 is tilted and decentered with respect to the substrate 1a by an angle θ so as to be asymmetric with respect to the virtual plane π.

この時集光レンズ2を偏心させたときに発生する偏心コ
マ収差を利用して第5図の実施例と同様に原稿を斜め下
方向から照明する際に伴う読取位置B(光路長の短い
側)の照度が上がる現象を緩和させて原稿面における照
度の均一化を図っている。
At this time, by using the decentering coma aberration generated when the condenser lens 2 is decentered, the reading position B (the side where the optical path length is short is accompanied by the illumination of the document from the obliquely downward direction as in the embodiment of FIG. ), The phenomenon that the illuminance rises is alleviated, and the illuminance on the document surface is made uniform.

この様に第5図、第6図の各実施例で示した集光レンズ
2は、かまぼこ型のレンズを利用して仮想平面πに対し
て非面対称となる様に偏心させて、この時発生するコマ
収差を利用して原稿面上における照度のバラツキΔEを
小さく抑えている。
In this way, the condenser lens 2 shown in each of the embodiments of FIGS. 5 and 6 is decentered so as to be asymmetric with respect to the virtual plane π by using a kamaboko type lens, and at this time, By utilizing the generated coma aberration, the variation ΔE of the illuminance on the document surface is suppressed to be small.

尚、このときの集光レンズ2の形状は両面を凸部で形成
しても最適な解は存在する。
It should be noted that there is an optimum solution for the shape of the condenser lens 2 at this time even if both surfaces are formed with convex portions.

又、前述した様に仮想平面πに対して左右非対称の形状
の集光レンズを更に仮想平面πに対して平行偏心や傾き
偏心させて配置しても良い。
Further, as described above, a condensing lens having a shape that is asymmetrical with respect to the virtual plane π may be further arranged in parallel decentering or tilt decentering with respect to the virtual plane π.

以上述べた各実施例は集光レンズの原稿面と仮想平面π
に直交する断面方向についてのみ示してきたが、例えば
線状光源の長手方向にパワーを有する第7図、第8図に
各々示した様に一部が強い凸状を有する集光レンズ2、
又は段階的に凸部を配列した形状等から成る集光レンズ
2でも、仮想平面πに対して非面対称な形状であれば前
述の実施例と同様の効果が得られる。
In each of the embodiments described above, the original surface of the condenser lens and the virtual plane π
Although it has been shown only in the cross-sectional direction orthogonal to, the condensing lens 2 having a partially strong convex shape as shown in FIGS. 7 and 8 having power in the longitudinal direction of the linear light source,
Alternatively, even in the condenser lens 2 having a shape in which convex portions are arranged stepwise, the same effect as that of the above-described embodiment can be obtained as long as the shape is asymmetric with respect to the virtual plane π.

又、各実施例において画像読取装置の原稿照明部は原稿
を斜め下方から照明して原稿の画像情報を読み取るよう
に構成したが、原稿に対して斜め上方より照明して透過
光束を用いても本発明は前述の実施例と同様の効果を得
ることができる。
Further, in each of the embodiments, the document illuminating unit of the image reading apparatus is configured to illuminate the document obliquely from below and read the image information of the document, but it is also possible to illuminate the document obliquely from above and use the transmitted light flux. The present invention can obtain the same effects as those of the above-mentioned embodiment.

又原稿走査として各実施例は原稿を搬送ローラを用いて
副走査方向に移動させ順次原稿の画像情報を読取ってい
るが、原稿を固定にして光学系を移動させて走査するミ
ラーレンズを用いたミラー走査方法を用いた装置や、結
像手段と撮像素子等の光学部材を一体化に構成して原稿
走査させる原稿の走査方法を用いた装置にも本発明は同
様に適用することができる。
Further, as the original scanning, in each embodiment, the original is moved in the sub-scanning direction by using the conveying roller to sequentially read the image information of the original, but the original is fixed and the optical system is moved to use the mirror lens for scanning. The present invention can be similarly applied to an apparatus using a mirror scanning method and an apparatus using an original scanning method in which an image forming unit and an optical member such as an image sensor are integrally formed to scan an original.

(発明の効果) 本発明によれば線状光源と原稿読取位置との間に所定形
状の集光レンズを前述した仮想平面πに対して非面対称
となるように設け、該集光レンズを介して原稿面上を照
明することにより、斜め方向から原稿面を照明しても原
稿読取位置がずれた際に生じる原稿面上の照度のバラツ
キを小さく抑えることができ、これにより装置に要求さ
れるメカ精度を緩和することができ、又組立工程を容易
にした読取精度の高い安価な画像読取装置を達成するこ
とができる。
(Effect of the Invention) According to the present invention, a condenser lens having a predetermined shape is provided between the linear light source and the document reading position so as not to be asymmetric with respect to the virtual plane π, and the condenser lens is provided. By illuminating the original surface via the light source, even if the original surface is illuminated from an oblique direction, it is possible to suppress the variation in the illuminance on the original surface caused by the deviation of the original reading position. It is possible to reduce the mechanical precision of the image reading apparatus and to achieve an inexpensive image reading apparatus with a high reading accuracy that facilitates the assembly process.

【図面の簡単な説明】[Brief description of drawings]

第1図は本発明の一実施例の画像読取装置の要部概略
図、第2図は第1図で示した線状光源と集光レンズの一
部分の拡大断面図、第3図は第1図における原稿面の照
度分布の説明図、第4図は左右の曲率が異なる形状を有
する集光レンズの断面図、第5図、第6図は各々本発明
の他の一実施例の集光レンズの断面と、その方向に関す
る原稿面の照度分布の説明図、第7図、第8図は各々本
発明の他の一実施例の集光レンズの斜視図、第9図は従
来の画像読取装置の要部概略図と原稿面の照度分布の説
明図、第10図は仮想平面πの定義を説明するための説明
図と発光エネルギー分布の説明図である。 図中、1、91は線状光源、2、92は集光レンズ、3は原
稿、4は結像手段、5は撮像素子、6は反射ミラー、7
は搬送ローラー、1aは基板、10、90は原稿照明部、πは
線状光源の発光強度が最大値をとる方向と線状光源の長
手方向の2つの方向より決定される仮想平面である。
FIG. 1 is a schematic view of a main part of an image reading apparatus according to an embodiment of the present invention, FIG. 2 is an enlarged sectional view of a part of the linear light source and the condenser lens shown in FIG. 1, and FIG. FIG. 4 is an explanatory view of the illuminance distribution on the document surface, FIG. 4 is a cross-sectional view of a condenser lens having a shape in which the left and right curvatures are different, and FIGS. 5 and 6 are the condensers of another embodiment of the present invention. FIG. 7 is a perspective view of a condenser lens of another embodiment of the present invention, and FIG. 9 is a conventional image reading method. FIG. 10 is a schematic view of a main part of the apparatus and an explanatory view of illuminance distribution on a document surface, and FIG. 10 is an explanatory view for explaining the definition of the virtual plane π and an explanatory view of emission energy distribution. In the figure, 1 and 91 are linear light sources, 2 and 92 are condenser lenses, 3 are originals, 4 is image forming means, 5 is an image pickup element, 6 is a reflection mirror, and 7
Is a transport roller, 1a is a substrate, 10 and 90 are original document illumination parts, and π is an imaginary plane determined by two directions, the direction in which the emission intensity of the linear light source has a maximum value and the longitudinal direction of the linear light source.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】原稿面上の読取面を該読取面に対し斜め方
向から線状光源からの光束により照明し、該読取面から
の光束を結像手段により撮像素子面上に結像させ、前記
原稿面上の画像情報を読み取る画像読取装置において、
前記線状光源と前記原稿面との間に集光レンズを設け、
該集光レンズは、前記線状光源の発光エネルギー強度が
最大値をとる方向と前記線状光源の長手方向との2方向
より形成される平面πに対して非面対称な形状の屈折面
を有し、該平面πより該原稿面に近い方の屈折面の曲率
半径をRa、該平面πより該原稿面に遠い方の屈折面の曲
率半径をRbとしたとき、Ra>Rbとなるようにして該原稿
面上の照度分布の均一化を図っていることを特徴とする
画像読取装置。
1. A reading surface on a document surface is illuminated with a light beam from a linear light source obliquely to the reading surface, and the light beam from the reading surface is imaged on an image pickup element surface by an image forming means. In an image reading device for reading image information on the document surface,
A condenser lens is provided between the linear light source and the document surface,
The condensing lens has a refracting surface that is asymmetric with respect to a plane π formed by two directions of a direction in which the emission energy intensity of the linear light source has a maximum value and a longitudinal direction of the linear light source. When the radius of curvature of the refracting surface closer to the original surface than the plane π is Ra and the radius of curvature of the refractive surface farther from the plane π to the original surface is Rb, Ra> Rb. The image reading apparatus is characterized in that the illuminance distribution on the surface of the original is made uniform.
JP1259483A 1989-10-04 1989-10-04 Image reader Expired - Fee Related JPH0793670B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1259483A JPH0793670B2 (en) 1989-10-04 1989-10-04 Image reader

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1259483A JPH0793670B2 (en) 1989-10-04 1989-10-04 Image reader

Publications (2)

Publication Number Publication Date
JPH03121653A JPH03121653A (en) 1991-05-23
JPH0793670B2 true JPH0793670B2 (en) 1995-10-09

Family

ID=17334710

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1259483A Expired - Fee Related JPH0793670B2 (en) 1989-10-04 1989-10-04 Image reader

Country Status (1)

Country Link
JP (1) JPH0793670B2 (en)

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2566185B2 (en) * 1992-08-06 1996-12-25 スタンレー電気株式会社 LED array
JP3275912B2 (en) 2000-08-08 2002-04-22 松下電器産業株式会社 Metal vapor discharge lamp
JP4170818B2 (en) 2003-04-11 2008-10-22 株式会社リコー Lighting device, document reading device, image forming device
JP2011038829A (en) * 2009-08-07 2011-02-24 Topcon Corp Interference microscope and measuring apparatus

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63173455A (en) * 1987-01-13 1988-07-18 Matsushita Graphic Commun Syst Inc Photoelectric converter

Also Published As

Publication number Publication date
JPH03121653A (en) 1991-05-23

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