JPH03121653A - Picture reader - Google Patents

Picture reader

Info

Publication number
JPH03121653A
JPH03121653A JP1259483A JP25948389A JPH03121653A JP H03121653 A JPH03121653 A JP H03121653A JP 1259483 A JP1259483 A JP 1259483A JP 25948389 A JP25948389 A JP 25948389A JP H03121653 A JPH03121653 A JP H03121653A
Authority
JP
Japan
Prior art keywords
original
light source
document
linear light
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.)
Granted
Application number
JP1259483A
Other languages
Japanese (ja)
Other versions
JPH0793670B2 (en
Inventor
Motomu Fukazawa
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

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Landscapes

  • Microscoopes, Condenser (AREA)
  • Optical Systems Of Projection Type Copiers (AREA)
  • Light Sources And Details Of Projection-Printing Devices (AREA)
  • Facsimile Heads (AREA)
  • Facsimile Scanning Arrangements (AREA)

Abstract

PURPOSE:To decrease the dispersion of illuminance on an original face caused when an original read position is deviated by providing a condenser lens of a prescribed shape between a linear light source and the original read position not in symmetry with respect to an imaginary plane and lighting the original face via the condenser lens. CONSTITUTION:A condenser lens 2 is provided between a linear light source 1 and a reader of an original 3. The refracting face of the condenser lens 2 is in asymmetry with respect to an imaginary plane pi and formed with array of bars in the lengthwise direction of the linear light source 1 such as in a direction where plural light emitting elements are arranged. Then an original light section 10 is formed by the linear light source 1 and the condenser 2 and the original light section 10 lights the original 3 from the oblique and lower direction. Since the shape of the condenser lens 2 is formed properly with respect to the imaginary plane pi in this way, the dispersion in the illuminance on the original face caused when the read position of the original 3 is deviated is decreased.

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
結像させて譲原槁面にの画像情報を順次高M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
キャナー簿に好適な画像読取装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Industrial Application Field) The present invention relates to an image reading device, and particularly 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 one dimension). A condensing lens with a specific shape is used to illuminate the document surface from an oblique direction, and the reflected or transmitted light beam from the document is imaged on the image pickup device surface via an imaging lens system to produce an image on the surface. The present invention relates to an image reading device that sequentially reads information at a high M degree and is suitable for, for example, copying machines, facsimile machines, and image scanners.

(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) Conventionally, an image reading apparatus is known in which an LED array with a bar-shaped condensing lens is used as an illumination unit for illuminating the document surface to illuminate the document surface from an oblique direction.

そして該原稿面からの光束を結像レンズ系を介してCO
D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 beam from the document surface is passed through an imaging lens system to a CO
Image information from the document surface is read by forming an image on the surface of an image sensor such as D.

この様な画像読取装置においてCOD笠の撮像素子を用
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m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。
When reading image information on the document surface using a COD shaded image sensor in such an image reading device, it is important to make the illuminance distribution (light m distribution) on the document surface as uniform as possible to improve reading accuracy. It is preferable to do so.

第9図は従来のこの神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 an explanatory diagram showing a schematic view of the main parts of the conventional image reading device and an illuminance distribution on the 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, reference numeral 90 denotes an LED array (original illumination unit) with a condensing lens, which is composed of a linear light source (LED array light source) 91 and a rod-shaped condensing lens 92 for condensing light.
is illuminated diagonally from below.

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によって矢印りの如く副走査方向に移動
している。
Reference numeral 3 denotes an original (for example, a reflective original or a transparent original), which is moved in the sub-scanning direction as indicated by the arrow by a conveyance roller 7, which will be 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−)5面上に結像させている。
Reference numeral 6 denotes a reflecting mirror, which bends the optical path by reflecting the reflected light beam from the original 3 toward an imaging means 4, which will be described later. Reference numeral 4 denotes an image forming means that forms an image of the reflected light beam from the original 3 on the surface of an image sensor (image sensor) 5.

撮@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。
The photographing element 5 is one-dimensional, for example, a CCD or the like. The conveyance roller 7 conveys the original 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, a light beam emitted from a linear light source 91 is condensed by a rod-shaped condensing lens 92, and the condensing lens 92 illuminates a predetermined area centered on the reading position A of the original 3 from diagonally 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l−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 a reflection mirror 6.
An image is formed on the surface l- of the image sensor 5 by the imaging means 4 via the image forming means 4, thereby reading the image information on the surface 3 of the document.

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 diagram showing the luminous energy emission distribution in space of the luminous flux emitted from the linear light source 91 at this time, and an explanatory diagram explaining the definition of the virtual plane π, which will be 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 of the luminous energy of the light beam emitted from the linear light source 91 peaks (maximum) is approximately perpendicularly 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
仮想乎面電と定義する。
The virtual plane formed by two directions, the direction Y in which the intensity value of the emitted light energy has the maximum value, and the longitudinal direction of the linear light source (for example, the direction in which chips are arranged in an LED array) X is hereinafter defined as a virtual surface plane. .

尚、仮想平面πは線状光源91の基板91aに対し線状
光源91を含む直交平面で与えられる。
Note that the virtual plane π is given by a plane orthogonal to the substrate 91a of the linear light source 91 and including the linear light source 91.

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 of the rod-shaped condensing lens 92 constituting the conventional document illumination section 90 shown in FIG. It has a plane of symmetry.

(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 using such a rod-shaped condensing lens, the following problems arise.

■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fffB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raC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 fffB on the document surface after passing through the condensing lens 92 is as follows: The illuminance at reading position B is higher than that at reading position C because the optical path length until reaching reading position raC is shorter.

■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してしよい、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。
■The imaging position that focuses the light beam that has passed through the center of the condenser lens 92 and the light beam that has passed through the periphery may be shifted.In particular, the light beam that has passed through the periphery is strongly bent and wraps around inward, a so-called phenomenon. 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谷
々の読取位i1!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 in FIG. 9, the reading position i1 of the valley! Ripples occur in the illuminance of the document surface of 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raB−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 this phenomenon, the variation ΔE in illuminance due to the deviation of the document reading position (between reading positions raB and C) due to the mechanical precision of the device becomes large, causing unevenness in the illuminance distribution on the document surface. 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簿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 conventional image reading devices, it is extremely difficult to set margins for signal output in the device design, and strict mechanical accuracy requirements and an increase in the number of adjustment items become a factor that increases the cost of the device.

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1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 problems of the conventional image reading device described above, the present invention is capable of reading a document by appropriately forming the shape of the condensing lens with respect to the virtual plane π, or by decentering the position of the condensing lens. An inexpensive configuration that can suppress variations in illuminance on the document surface that occur when the document is misaligned, reduce mechanical precision while achieving high-precision reading, and can be easily assembled without increasing the number of adjustment items. The purpose 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、該原稿面上の画像情報を読み取る画像読取装置
において、該線状光源と該原稿面との間に該線状光源の
発光エネルギー強度が最大値をとる方向と該線状光源の
長手方向との2方向より形成される平面πに対し非面対
称な形状の屈折面を有する集光レンズを設けたことを特
徴としている。
(Means for Solving the Problems) The image reading device of the present invention illuminates a reading surface on a document surface with a light beam from a linear light source from a diagonal direction with respect to the reading surface,
In an image reading device that forms an image of a light beam from the reading surface on an image sensor surface by an imaging means and reads image information on the document surface, the linear light source is provided between the linear light source and the document surface. characterized by providing a condenser lens having a refractive surface asymmetrical with respect to a plane π formed by two directions: the direction in which the luminous energy intensity of the linear light source reaches its maximum value, and the longitudinal direction of the linear light source. There is.

(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 diagram of main parts of an image reading device 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 this figure, the same elements as those shown in FIG. 9 are given 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、へロゲンランプ、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。
A linear light source 1 is composed of, for example, an LED array light source in which a plurality of light emitting elements are arranged in one dimension, a herogen lamp, a fluorescent lamp, etc., and is arranged diagonally with respect to the document 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l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 condensing lens according to the present invention, which is provided between the document reading device 3 and the linear light source 1. The condensing lens 2 has a refractive surface that is asymmetrical with respect to the virtual plane π described above, and is formed into a rod-like shape with respect to the longitudinal direction of the linear light source l, for example, the direction in which a plurality of light emitting elements are lined up. There is.

本実施例では線状光源l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 this embodiment, a linear light source 1 and a condensing lens 2 constitute a document illumination section 10, and the document 3 is illuminated from diagonally downward by the document illumination section 10.

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りの如く副走査方
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 illumination unit 10
While moving the document 3 in the sub-scanning direction as shown by the arrow shown in the figure by the conveyance roller 7, the reflected light beam from the document 3 is sequentially imaged on the surface of the image pickup device 5 by the imaging means 4 via the reflection mirror 6. Image information on three sides of the original is being read.

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 function of the condensing lens 2 according to the present invention will be explained using FIG. 2.

第2図は第1図に示した線状光源l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 view of a portion of the linear light source l and condenser lens 2 shown in FIG. 1.

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 symmetrical) 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すまでの
間隔d、をd、=t 1.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2blの曲率半径R1をR1=6、そして集光レ
ンズ2の幅寸法りを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 d0 between the intersection a of the entrance surface of the condenser lens 2 and the optical axis and the substrate 1a is set to d0=1, the distance between the exit surface of the condenser lens 2 and the optical axis from the intersection a is The distance d between the points of intersection is d,=t 1. The radius of curvature R2 of the lens surface 2a on the entrance surface side is R2=5, the radius of curvature R1 of the surface 2bl on one side of the lens surface 2b on the exit surface side is R1=6, and the width dimension of the condenser lens 2 is D=8. The dimensions of each part of the condenser lens 2 are set according to the ratio of .

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からみて仮想寮面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、即ちこのノンパワ一部2b2を平面より形成して他
の部分2bl(パワ一部)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
形状を成している。
Also, the surface 2b2 on the left side of the drawing on the exit surface side of the condensing lens 2, which is an asymmetrical part (the part close to the document surface 3 in FIG. 1), for example, is 30 degrees from the virtual surface π when viewed from the center of curvature O.
The portion 2b2 beyond 2b2 has no power (refracting power), that is, the non-power portion 2b2 is formed from a flat surface, and the other portion 2b1 (power portion) is formed from a cylindrical shape. As a result, the shape is asymmetrical with respect to the virtual plane π.

この様な形状の集光レンズ2のノンパワ一部2b2を通
過した線状光源l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 flux from the linear light source l that passes through the non-power portion 2b2 of the condensing lens 2 having such a shape is not focused on the reading position of the original 3, and therefore the illumination intensity for illuminating the original 3 is reduced. In the vicinity of the reading position B, the phenomenon of light flux convergence 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 effect is utilized to prevent ripples from occurring in the illuminance distribution between the reading positions B and 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2
bl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
iQAより読取位rftC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19Bから読取位rIIC
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()
ることができる。
On the other hand, the right part 2 of the exit surface in the drawing with respect to the virtual plane π
The shape of bl is the conventional condenser lens 92 shown in FIG.
(cylindrical shape), the illumination illuminance decreases as it moves from the reading position iQA toward the reading position rftC, but due to the wrap-around phenomenon caused by spherical aberration, the illumination illuminance rises again and eventually moves from the reading position 19B to the reading position rIIC.
Until now, as shown in Figure 3, we have created a broad document surface illuminance distribution with the illuminance variation reduced by ΔE ().
can be done.

特に第3図の点線で示した従来の原稿読取位置13− 
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(1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, the conventional document reading position 13- indicated by the dotted line in FIG.
Compared to the illuminance distribution between A and A, in this embodiment, the illuminance variation is ΔE as shown by the solid line in the figure, and the illuminance distribution is kept extremely small (1).
-C is aimed at making the illuminance 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。
In this way, in this embodiment, the shape of the refractive surface of the condenser lens 2 is formed to be asymmetric with respect to the virtual plane π as described above, and the light beam emitted from the linear light source 1 is directed by the condenser lens 2. The illuminance is efficiently irradiated onto the document surface, and the illuminance distribution on the document surface is made uniform to achieve highly accurate reading.

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 perpendicular to the document surface and the virtual plane π is formed by a cylindrical shape and a plane to make the illuminance distribution on the document surface uniform. For example, even if the cross-sectional shape of the condenser lens 2 is formed using an aspherical shape, the present invention can reduce the illuminance on the document surface as described above. It is possible to make the distribution uniform.

又第4図に示す様に2つの屈折面の曲率を径1i11.
R2を仮想平市電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。
Further, as shown in FIG. 4, the curvatures of the two refractive surfaces are set to diameters 1i11.
R2 may be set to a different value on the left and right sides of the drawing with the virtual flat streetcar as the border. For example, even if the condenser lens 2 is formed so that R1 (left)>R2 (right), the same result as in the above embodiment can be achieved. The variation ΔE in the illuminance distribution on the document surface can be kept small.

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。
FIGS. 5 and 6 are explanatory diagrams of a cross-sectional direction perpendicular to the document surface and the virtual plane π of a condensing lens according to another embodiment of the present invention, and an explanatory diagram of the illuminance distribution on the document surface, respectively.

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≠市電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lから発光された光束を集光レン
ズ2で集光し、註集光レンズ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 condensing lens 2 of the above-mentioned embodiment is formed so that the shape of the condensing lens 2 itself is asymmetrical with respect to the virtual tram, so that the light beam emitted from the linear light source l is condensed. Note: Although the case where the light is focused by the light lens 2 and the document 3 is illuminated from diagonally downward by the light condensing lens 2 is shown, in each of the embodiments shown in FIGS. 5 and 6, the shape of the light condensing lens 2, The condensing lens 2 has a shape that is symmetrical with respect to the optical axis.
The plane of symmetry of is eccentric to the virtual plane π, and the original 3 is illuminated obliquely from below.

即ち仮想γ而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, it is characterized in that the condenser lens 2 is decentered so that the shape of the condenser lens 2 is asymmetric with respect to the virtual γ and 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。
Condenser lens 2 in each embodiment of FIGS. 5 and 6
has a semicylindrical shape that 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に対して平
行に距@Itだけ平行偏心させて仮想乎市電に対して非
面対称となるように構成している。
In FIG. 5, the condensing lens 2 is parallel and decentered by a distance @It in parallel to the virtual plane π, so that it is asymmetrical with respect to the virtual tram.

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
屈折する看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, asymmetrical comatic aberration occurs due to eccentricity, and as shown in the figure, in the region between reading positions A and C of the document, the angle of incidence on the curved surface of the condenser lens 2 is large, so the light beam is refracted. It shows a tendency for the view to be greatly curved and become denser.

又読取位置Δ−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頃が
小さく弱く曲げられ、疎になる傾向を示している。
Moreover, in the area between the reading positions Δ and B, on the contrary, since the angle of incidence on the curved surface of the condenser lens 2 is small, the refraction of the light beam is small and weakly bent, and the light beams tend 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 kept small as shown in the figure.

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・ト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八Eを小さく抑えて原
稿面の照度の均一化を図っている。
In this way, in this embodiment, the reading position B that accompanies when illuminating the original from diagonally below is utilized by using the eccentric coma aberration that occurs when the condensing lens 2 is decentered in the direction of the virtual plane π. This alleviates the phenomenon of increased illuminance (on the short optical path length side). As a result, variations in illuminance 8E are suppressed to a small level, 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 placed at an angle θ with respect to the substrate 1a.
By making the inclination and eccentricity by 1, it is configured to be asymmetrical 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ra8(光路長の短い
1111)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, using decentering coma aberration that occurs when the condensing lens 2 is decentered, the reading position ra8 (1111 with a short optical path length) that accompanies when illuminating the original from diagonally downward as in the embodiment shown in FIG. ) to reduce the phenomenon in which the illuminance increases and to make the illuminance uniform on the document surface.

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 condensing lens 2 shown in each of the embodiments of FIGS. 5 and 6 uses a semicylindrical lens and is decentered so as to be asymmetric with respect to the virtual plane π. The generated coma aberration is used to suppress the variation ΔE in illuminance on the document surface.

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。
Note that an optimal solution exists even if the shape of the condenser lens 2 at this time is formed with convex portions on both sides.

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Nト行偏心や傾
き偏心させて配置しても良い。
Further, as described above, the condenser lens having a shape asymmetrical with respect to the virtual plane π may be further arranged with N-row eccentricity or tilt eccentricity with respect to the virtual plane π.

以上建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、仮想を面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。
Each of the embodiments constructed above is based on the original surface of the condensing lens and the virtual plane π.
Although only the cross-sectional direction perpendicular to the linear light source has been shown, for example, as shown in FIGS. 7 and 8, the condenser lens 2 has a strong convex shape, and has power in the longitudinal direction of the linear light source.
Alternatively, even if the condenser lens 2 has a shape in which convex portions are arranged in stages, the same effect as in the above embodiment can be obtained if the condenser lens 2 has a shape that is imaginary asymmetric with respect to the 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。
Furthermore, in each of the embodiments, the document illumination section of the image reading device is configured to illuminate the document from diagonally below to read the image information of the document, but it is also possible to illuminate the document from diagonally above and use transmitted light flux. The present invention can obtain the same effects as the above-described embodiments.

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
像手段と描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。
Furthermore, in each of the embodiments, the original is scanned in the sub-scanning direction using a conveyance roller, and the image information of the original is sequentially read. 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 optical member such as an image forming means and an imaging element are integrally configured 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。
(Effects of the Invention) According to the present invention, a condensing lens of a predetermined shape is provided between a linear light source and a document reading position so as to be asymmetrical with respect to the virtual plane π, and the condensing lens is By illuminating the document surface through the scanner, it is possible to suppress variations in illumination on the document surface that occur when the document reading position shifts, even if the document surface is illuminated from an oblique direction. In addition, it is possible to achieve an inexpensive image reading device with high reading accuracy and easy assembly process.

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

第1図は本発明の−χ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fY
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、l、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、la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 diagram of the main parts of an image reading device according to the -χ embodiment of the present invention, FIG. 2 is an enlarged sectional view of a portion of the linear light source and condensing lens shown in FIG. 1, and FIG. An explanatory diagram of the illuminance distribution on the document surface in Figure 1, and Figure 4 shows the shape with different left and right curvatures as fY.
FIGS. 5 and 6 are cross-sectional views of a condensing lens according to another embodiment of the present invention, and explanatory diagrams of the illuminance distribution on the document surface with respect to the direction thereof, FIGS. 7 and 6, respectively. 8 is a perspective view of a condensing lens according to another embodiment of the present invention, FIG. 9 is a schematic diagram of the main parts of a conventional image reading device and an explanatory diagram of the illuminance distribution on the document surface, and FIG. 10 is a virtual plane. FIG. 2 is an explanatory diagram for explaining the definition of π and an explanatory diagram of the emission energy distribution. In the figure, l, 91 is a linear light source, 2.92 is a condenser lens, 3
is the document, 4 is the image forming means, 5 is the image pickup device, 6 is the reflection mirror, 7 is the transport roller, la is the substrate, 10.90 is the document illumination section, π is the direction in which the emission intensity of the linear light source takes the maximum value This is a virtual plane determined from two directions: and the longitudinal direction of the linear light source.

Claims (1)

【特許請求の範囲】[Claims] (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、該原稿面上
の画像情報を読み取る画像読取装置において、該線状光
源と該原稿面との間に該線状光源の発光エネルギー強度
が最大値をとる方向と該線状光源の長手方向との2方向
より形成される平面πに対し非面対称な形状の屈折面を
有する集光レンズを設けたことを特徴とする画像読取装
置。
(1) A reading surface on the document surface is illuminated with a light beam from a linear light source from a diagonal direction with respect to the reading surface, and the light beam from the reading surface is imaged on the image sensor surface by an imaging means, In an image reading device that reads image information on a surface, there are two directions between the linear light source and the document surface: the direction in which the emitted energy intensity of the linear light source is at its maximum value, and the longitudinal direction of the linear light source. What is claimed is: 1. An image reading device comprising: a condenser lens having a refractive surface asymmetrical with respect to a plane π formed by the condenser lens.
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 true JPH03121653A (en) 1991-05-23
JPH0793670B2 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)

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0662185A (en) * 1992-08-06 1994-03-04 Stanley Electric Co Ltd Led array
US6774559B2 (en) 2000-08-08 2004-08-10 Matsushita Electric Industrial Co., Ltd. Metal vapor discharge lamp
US7548352B2 (en) 2003-04-11 2009-06-16 Ricoh Company, Limited Illumination device, document reading device, adjusting device, and image forming apparatus
JP2011038829A (en) * 2009-08-07 2011-02-24 Topcon Corp Interference microscope and measuring apparatus

Citations (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

Patent Citations (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

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0662185A (en) * 1992-08-06 1994-03-04 Stanley Electric Co Ltd Led array
US6774559B2 (en) 2000-08-08 2004-08-10 Matsushita Electric Industrial Co., Ltd. Metal vapor discharge lamp
US7548352B2 (en) 2003-04-11 2009-06-16 Ricoh Company, Limited Illumination device, document reading device, adjusting device, and image forming apparatus
JP2011038829A (en) * 2009-08-07 2011-02-24 Topcon Corp Interference microscope and measuring apparatus

Also Published As

Publication number Publication date
JPH0793670B2 (en) 1995-10-09

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