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JPS648806B2 - - Google Patents
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JPS648806B2 - - Google Patents

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Publication number
JPS648806B2
JPS648806B2 JP55048658A JP4865880A JPS648806B2 JP S648806 B2 JPS648806 B2 JP S648806B2 JP 55048658 A JP55048658 A JP 55048658A JP 4865880 A JP4865880 A JP 4865880A JP S648806 B2 JPS648806 B2 JP S648806B2
Authority
JP
Japan
Prior art keywords
lens
filter
disk
optical axis
optical path
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
Application number
JP55048658A
Other languages
Japanese (ja)
Other versions
JPS56153314A (en
Inventor
Toshuki Iguchi
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.)
Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP4865880A priority Critical patent/JPS56153314A/en
Publication of JPS56153314A publication Critical patent/JPS56153314A/en
Publication of JPS648806B2 publication Critical patent/JPS648806B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04NPICTORIAL COMMUNICATION, e.g. TELEVISION
    • H04N1/00Scanning, transmission or reproduction of documents or the like, e.g. facsimile transmission; Details thereof
    • H04N1/46Colour picture communication systems
    • H04N1/48Picture signal generators
    • H04N1/482Picture signal generators using the same detector device sequentially for different colour components

Landscapes

  • Engineering & Computer Science (AREA)
  • Multimedia (AREA)
  • Signal Processing (AREA)
  • Exposure Or Original Feeding In Electrophotography (AREA)
  • Optical Filters (AREA)
  • Facsimile Heads (AREA)
  • Facsimile Scanning Arrangements (AREA)
  • Mechanical Optical Scanning Systems (AREA)

Description

【発明の詳細な説明】 本発明は、原稿に描かれた画像を画素に分解し
て読み取ると同時に、各画素毎の色分解をする色
情報読取装置に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a color information reading device that separates and reads an image drawn on a document into pixels, and simultaneously performs color separation for each pixel.

従来、この種の装置は第1図に示したように構
成されている。第1図において、1は複数の色で
画像が描かれた原稿、2は、この原稿1の主走査
方向(矢印A方向)に配列された画素3(第2図
参照)の数と同数の読取素子(図示せず)を1列
に配設して、原稿1の主走査方向(矢印A方向)
に1列に配列された複数の画素3を同時に読み取
る撮像体、4は原稿1を副走査方向〔図面に対し
て垂直な方向(第2図参照)〕に一定の速度で搬
送するローラ、5は原稿1に描かれた画像を撮像
体2に結像させるレンズ、6は複数の色の平行平
面フイルタ、例えば、互いに補色の関係にある赤
色のフイルタ7と青緑(シアン)色のフイルタ8
とを交互に配設した円板〔第1図b参照〕で、こ
の円板6はフイルタ7及び8の平面が光軸に対し
て垂直になるようにして原稿1とレンズ5との間
の光路上に設置される。9は撮像体2の読取動作
に同期して円板6を回動させるモータである。
Conventionally, this type of apparatus has been constructed as shown in FIG. In Fig. 1, 1 is a document on which an image is drawn in multiple colors, and 2 is the same number of pixels 3 (see Fig. 2) arranged in the main scanning direction (direction of arrow A) of this document 1. Reading elements (not shown) are arranged in one row to scan the original 1 in the main scanning direction (direction of arrow A).
4 is an imaging body that simultaneously reads a plurality of pixels 3 arranged in a row; 4 is a roller that conveys the original 1 at a constant speed in the sub-scanning direction [direction perpendicular to the drawing (see FIG. 2)]; numeral 6 is a lens for forming an image drawn on the original document 1 on the imaging body 2; numeral 6 is a parallel plane filter of a plurality of colors; for example, a red filter 7 and a cyan filter 8, which are complementary colors to each other;
(See Figure 1b).This disk 6 is arranged between the document 1 and the lens 5 so that the planes of the filters 7 and 8 are perpendicular to the optical axis. Installed on the optical path. Reference numeral 9 denotes a motor that rotates the disk 6 in synchronization with the reading operation of the image pickup body 2.

このように構成された従来例では、原稿1をロ
ーラ4によつて副走査方向〔矢印B方向(第2図
参照)〕に搬送しながら、原稿1の主走査方向
(矢印A方向)に1列に配列された複数の画素3
を、回動する円板6のフイルタ7及び8によつて
1列毎に順次色分解した光が撮像体2の各読取素
子(図示せず)に入射すると、撮像体2の各読取
素子(図示せず)はフイルタ7を通過した各画素
3の光量に比例した電気信号とフイルタ8を透過
した各画素3の光量に比例した電気信号とを交互
に出力するので、論理回路(図示せず)において
これ等の電気信号を各画素3毎に比較することに
より、各画素3の有する色を識別することができ
る。ところで、各画素3の有する色を正確に色分
解するには、フイルタ7を通して撮像体2の各読
取素子(図示せず)が読み取つた範囲S1とフイル
タ8を通して撮像体2の各読取素子(図示せず)
が読取つた範囲S2とが第2図aに示したように各
画素3にそれぞれ一致していなければならない。
しかしながら、この従来例でローラ4によつて原
稿1を連続搬送しながら各画素3の読取りを行な
つているため、フイルタ7からフイルタ8或いは
フイルタ8からフイルタ7に変わる間に原稿1が
1/2画素(但し、円板6にm色のフイルタを順次
配列して1つの画素3をm通りに色分解する場合
には、1/m画素)分だけ副走査方向(矢印B方
向)に搬送され、フイルタ7を通して撮像体2の
各読取素子(図示せず)が読み取つた範囲S1(実
線で図示)とフイルタ8を通して撮像体2の各読
取素子(図示せず)が読み取つた範囲S2(点線で
図示)とが第2図bで示したように1/2画素分だ
けずれて、各画素3の有する色を正確に色分解で
きない欠点があつた。
In the conventional example configured in this way, while the document 1 is conveyed in the sub-scanning direction [in the direction of arrow B (see FIG. 2)] by the roller 4, the document 1 is conveyed in the main scanning direction (direction of arrow A). Multiple pixels arranged in columns 3
When the light that has been color-separated sequentially for each row by the filters 7 and 8 of the rotating disc 6 enters each reading element (not shown) of the image pickup body 2, each reading element (not shown) of the image pickup body 2 The logic circuit (not shown) alternately outputs an electric signal proportional to the amount of light from each pixel 3 that has passed through the filter 7 and an electric signal proportional to the amount of light from each pixel 3 that has passed through the filter 8. ), by comparing these electrical signals for each pixel 3, the color possessed by each pixel 3 can be identified. By the way, in order to accurately separate the colors of each pixel 3, it is necessary to separate the range S1 read by each reading element (not shown) of the image pickup body 2 through the filter 7 and the range S1 read by each reading element (not shown) of the image pickup body 2 through the filter 8. (not shown)
The read range S2 must correspond to each pixel 3 as shown in FIG. 2a.
However, in this conventional example, since each pixel 3 is read while the original 1 is continuously conveyed by the roller 4, the original 1 is 1/1 Conveyed in the sub-scanning direction (direction of arrow B) by 2 pixels (however, when one pixel 3 is color-separated into m ways by sequentially arranging filters of m colors on the disk 6, 1/m pixels). and a range S 1 (shown by a solid line) read by each reading element (not shown) of the image pickup body 2 through the filter 7 and a range S 2 read by each reading element (not shown) of the image pickup body 2 through the filter 8. (indicated by a dotted line) is shifted by 1/2 pixel as shown in FIG.

第3図は、他の従来例の構成を示したもので、
第1図と同一符号のものは同一部分を示してお
り、また、10及び11はそれぞれ原稿1と撮像
体2との間の光路長が変化しないように副走査方
向(矢印B方向)に移動する平面鏡である。
Figure 3 shows the configuration of another conventional example.
The same numbers as in FIG. 1 indicate the same parts, and 10 and 11 are moved in the sub-scanning direction (direction of arrow B) so that the optical path length between the original 1 and the image pickup body 2 does not change. It is a flat mirror.

このように構成された従来例では、第1図に示
した従来例のローラ4で原稿1を搬送させて副走
査をする代りに、平面鏡10及び11を移動させ
て副走査をするもので、この従来例にも第1図に
示した従来例と同様の欠点があつた。
In the conventional example configured as described above, instead of conveying the document 1 using the roller 4 shown in FIG. This conventional example also had the same drawbacks as the conventional example shown in FIG.

第4図は、前述した第1図及び第3図に示した
従来例の欠点を解消した従来例の構成を示したも
ので、第1図と同一符号のものは同一部分を示し
ており、色の異なる複数のフイルタ、例えば、フ
イルタ7及び8を個別に固定し、フイルタ7及び
8毎にそれぞれ撮像体2及びレンズ5を具備させ
て2つのレンズ系を設けたものである。
FIG. 4 shows the configuration of a conventional example that eliminates the drawbacks of the conventional examples shown in FIGS. 1 and 3, and the same reference numerals as in FIG. 1 indicate the same parts. A plurality of filters of different colors, for example, filters 7 and 8, are individually fixed, and each of the filters 7 and 8 is provided with an imaging body 2 and a lens 5, thereby providing two lens systems.

このように構成された従来例では、2つの撮像
体2の各読取素子(図示せず)によつて同一画素
3を同時に読み取ることができるため、各画素3
の有する色を正確に色分解することができる。し
かしながら、複数の撮像体2及び複数のレンズ5
が必要なため、色情報読取装置の価格が高くな
り、又、複数のレンズの光軸が一致するように調
整するのに手間が掛る欠点があり、更に、色分解
の数を増すと、これ等の欠点が急激に増加する欠
点があつた。
In the conventional example configured in this way, since the same pixel 3 can be read simultaneously by each reading element (not shown) of the two image pickup bodies 2, each pixel 3
It is possible to accurately separate the colors of However, a plurality of imaging bodies 2 and a plurality of lenses 5
This increases the price of the color information reading device, and it also takes time and effort to adjust the optical axes of multiple lenses to match.Furthermore, increasing the number of color separations There was a rapid increase in the number of shortcomings such as:

本発明は、上記従来例の欠点を解消するため
に、板厚、屈折率及び光線の入射角の内の少なく
とも1つの要素が異なる複数のフイルタまたは平
行平面ガラスを取り付けた円板をレンズの光軸に
向けて傾倒させて設置することにより、画素の読
取時機の違いによつて生じる画素の読取位置のず
れを防止した色情報読取装置を提供するものであ
る。以下、図面により本発明の実施例を詳細に説
明する。
In order to eliminate the drawbacks of the above-mentioned conventional examples, the present invention provides a lens with a circular plate attached with a plurality of filters or parallel plane glasses that differ in at least one element among plate thickness, refractive index, and incident angle of light rays. The present invention provides a color information reading device which prevents shifts in pixel reading positions caused by differences in pixel reading timing by installing the color information reading device tilted toward the axis. Embodiments of the present invention will be described in detail below with reference to the drawings.

第5図は、本発明の原理を示したもので、空気
中のみを通過する光線の光路をL0(実線で図示)、
板厚がt1、屈折率がn1(但し、1<n1)の平行平
面ガラス12(点線で図示)に角度θ1で入射する
光線の光路をL1(点線で図示)、板厚がt2(但し、
t1≦t2)、屈折率がn2(但し、1<n1≦n2)の平行
平面ガラス13(実線で図示)に角度θ2(但し、
θ1≦θ2)で入射する光線の光路をL2(1点鎖線で
図示)とし、入射光の光路L0,L1及びL2を互い
に平行にし、平行平面ガラス12及び13で屈折
した透過光の光路L1及びL2を空気中のみを通過
した光線の光路L0に一致させると、光路L0と光
路L1との間の距離ΔX1は、一般に、 ΔX1=t1・θ1(1−1/n1) ……(1) 光路L0の長さと光路L1の長さの差ΔY1は、一
般に、 ΔY1=t1(1−1/n1) ……(2) で示され、又、光路L0と光路L2との間の距離
ΔX2は、一般に、 ΔX2=t2・θ2(1−1/n2) ……(3) 光路L0の長さと光路L2の長さの差ΔY2は、一
般に、 ΔY2=t2(1−1/n2) ……(4) で示されるので、光路L1と光路L2との間の距離
ΔXは、(1)及び(3)式より、 ΔX=ΔX2−ΔX1=〔t2・θ2(1−1/n2)〕 −〔t1・θ2(1−1/n1)〕 ……(5) 光路L1の長さと光路L2の長さの差ΔYは、(2)及
び(4)式より、 ΔY=ΔY2−ΔY1=〔t2(1−1/n2)〕 −〔t1(1−1/n1)〕 ……(6) で現わされるが、光路長の差ΔYは、通常、平行
平面ガラス12及び13がレンズの前方に配置さ
れているならば、原稿1側の焦点深度が撮像体2
側の焦点深度に比べて深いので、無視することが
できる。従つて、原稿1をレンズ5の光軸に対し
て垂直方向に搬送して原稿1から発した入射光線
の光路をレンズ5の光軸に平行にし、且つ、(5)式
より、傾倒して設置した円板6にガラスの板厚及
び屈折率と入射光線の入射角の内少なくとも1つ
の要素の値を適宜変化させて取り付けたフイルタ
または平行平面ガラスによつて屈折させて、透過
光線の光路を一致させれば、異なる光路で光線が
フイルタ又は平行平面ガラスに入射しても、1つ
の透過光線の光路を通つて撮像体2の読取素子
(図示せず)に入射させることができるので、画
素3が副走査方向に移動しても、画素3の読取時
機の違いによる画素3の読取位置のずれを防止す
ることができる。
FIG. 5 shows the principle of the present invention, and shows the optical path of a ray that passes only through the air as L 0 (shown by a solid line),
The optical path of a light beam incident at an angle θ 1 on parallel plane glass 12 (indicated by a dotted line) with a plate thickness of t 1 and a refractive index of n 1 (1<n 1 ) is L 1 (indicated by a dotted line), and the plate thickness is t 2 (however,
t 1 ≦ t 2 ) and a refractive index of n 2 (however, 1<n 1 ≦n 2 ), an angle θ 2 (however,
The optical path of the incident light ray (θ 1 ≦ θ 2 ) is defined as L 2 (indicated by a dashed line), and the optical paths L 0 , L 1 and L 2 of the incident light are made parallel to each other and refracted by the parallel plane glasses 12 and 13. When the optical paths L 1 and L 2 of the transmitted light are made to coincide with the optical path L 0 of the light ray that has passed only through the air, the distance ΔX 1 between the optical path L 0 and the optical path L 1 is generally ΔX 1 = t 1 · θ 1 (1-1/n 1 ) ...(1) The difference ΔY 1 between the length of optical path L 0 and the length of optical path L 1 is generally expressed as ΔY 1 =t 1 (1-1/n 1 ) ... (2), and the distance ΔX 2 between the optical path L 0 and the optical path L 2 is generally expressed as ΔX 2 = t 2 · θ 2 (1-1/n 2 )... (3) Optical path L The difference ΔY 2 between the length of the optical path L 1 and the length of the optical path L 2 is generally expressed as ΔY 2 = t 2 (1-1/n 2 )...(4), so the difference between the optical path L 1 and the optical path L 2 is From equations ( 1 ) and ( 3 ) , the distance ΔX between /n 1 )] ...(5) The difference ΔY between the length of optical path L 1 and the length of optical path L 2 is calculated from equations (2) and (4) as follows: ΔY = ΔY 2 −ΔY 1 = [t 2 (1 -1/n 2 )] -[t 1 (1-1/n 1 )] ...(6) The difference in optical path length ΔY is usually the difference between the parallel plane glasses 12 and 13 of the lens. If it is placed in front, the depth of focus on the document 1 side will be the same as that of the image pickup body 2.
Since it is deep compared to the depth of focus on the side, it can be ignored. Therefore, by conveying the original 1 in a direction perpendicular to the optical axis of the lens 5 so that the optical path of the incident light beam emitted from the original 1 is parallel to the optical axis of the lens 5, and according to equation (5), by tilting The optical path of the transmitted light is refracted by a filter or parallel plane glass attached to the installed circular plate 6 by appropriately changing the value of at least one element among the thickness and refractive index of the glass and the angle of incidence of the incident light. By matching the rays, even if the rays enter the filter or parallel plane glass through different optical paths, the transmitted rays can be made to enter the reading element (not shown) of the image pickup body 2 through one optical path. Even if the pixel 3 moves in the sub-scanning direction, it is possible to prevent the reading position of the pixel 3 from shifting due to a difference in the reading timing of the pixel 3.

次に、この原理に基づいた本発明の実施例を詳
細に説明する。尚、第6図乃至第9図において、
本発明の実施例の理解を容易にするため、フイル
タまたは平行平面ガラスにおける光線の屈折状態
は、光学理論を無視して図示してあるが、実際に
は、光線がその光学理論に従つて屈折するもので
あることにいうまでもない。
Next, embodiments of the present invention based on this principle will be described in detail. In addition, in FIGS. 6 to 9,
In order to facilitate understanding of the embodiments of the present invention, the refraction state of light rays in a filter or plane-parallel glass is illustrated ignoring optical theory; Needless to say, it is something that can be done.

第6図は、本発明の一実施例を示したもので、
第1図及び第5図と同一符号のものは同一部分を
示しており、原稿1はレンズ5の光軸に対して垂
直な副走査方向(矢印B方向)に搬送され、又、
レンズ5の光軸に向けて傾倒させて設置した円板
6には、板厚が異なり、屈折率が等しいフイルタ
7及び8がそれぞれ同一の取付角、すなわち、入
射光線が同一の入射角で入射するように取り付け
られており、フイルタ7の板厚t2はフイルタ8の
板厚t1よりも大きくなつている。
FIG. 6 shows an embodiment of the present invention.
The same reference numerals as in FIGS. 1 and 5 indicate the same parts, and the original 1 is conveyed in the sub-scanning direction (direction of arrow B) perpendicular to the optical axis of the lens 5.
Filters 7 and 8 having different plate thicknesses and the same refractive index are placed on a disc 6 tilted toward the optical axis of the lens 5, so that the incident light rays are incident at the same angle of incidence. The plate thickness t 2 of the filter 7 is larger than the plate thickness t 1 of the filter 8.

このように構成された本実施例では、板厚の厚
いフイルタ7がレンズ5の光軸上に入つていると
きには、フイルタ7及び8がないときに撮像体2
の読取素子(図示せず)に入射する光線の光路
L0(実線で図示)の原稿1側の焦点Oから反副走
査方向((矢印B方向と反対方向)に遠いP点か
ら発した画素3の光線が入射光路L2(1点鎖線で
図示)を通つてフイルタ7に入射し、且つ、この
フイルタ7によつて屈折、色分解された透過光線
が光路L0と一致した透過光路L2(実線で図示)を
通つて撮像体2の読取素子(図示せず)に入射
し、又、板厚の薄いフイルタ8がレンズ5の光軸
上に入つているときには、フイルタ7及び8がな
いときに撮像体2の読取素子(図示せず)に入射
する光線の光路L0の原稿1側の焦点Oから反副
走査方向(矢印B方向と反対方向)に近いQ点、
すなわち、遠いP点から副走査方向(矢印B方
向)に1/2画素分ずれた位置から発した画素3の
光線が入射光路L1(点線で図示)を通つてフイル
タ8に入射し、且つ、このフイルタ8によつて屈
折、色分解された透過光線が光路L0と一致した
透過光路L1(実線で図示)を通つて撮像体2の読
取素子(図示せず)に入射するので、円板6を回
動させてフイルタ7及び8に交互にレンズ5の光
軸上に入れ換えれば、撮像体2の読取素子(図示
せず)は副走査方向(矢印B方向)に移動する各
画素3をP点及びP点から1/2画素分副走査方向
にずれたQ点で交互に読み取ることができる。
尚、P点とQ点との距離ΔXは、t1<t2,n1=n2
n,θ1=θ2=θ、1画素の副走査方向の寸法を
125μとすると、(5)式より、 ΔX=ΔX2−ΔX1=θ〔t2−t1)(1−1/n) =125/2=62.5(μ) となる。
In this embodiment configured as described above, when the thick filter 7 is placed on the optical axis of the lens 5, the imaging body 2 is
Optical path of the light beam incident on the reading element (not shown)
The light beam of pixel 3 emitted from point P , which is far from the focal point O on the document 1 side of L 0 (indicated by a solid line) in the anti-sub-scanning direction (in the direction opposite to arrow B), enters the incident optical path L 2 (indicated by a dashed line) ), and the transmitted light beam that is refracted and color-separated by this filter 7 passes through the transmitted optical path L 2 (shown by a solid line) that coincides with the optical path L 0 to read the image pickup body 2. When the thin filter 8 is placed on the optical axis of the lens 5, the light enters the reading element (not shown) of the image pickup body 2 when the filters 7 and 8 are not present. Point Q, which is close to the anti-sub-scanning direction (opposite direction of arrow B) from the focal point O on the document 1 side of the optical path L 0 of the light beam incident on the
That is, the light beam of pixel 3 emitted from a position shifted by 1/2 pixel in the sub-scanning direction (direction of arrow B) from the far point P enters the filter 8 through the incident optical path L 1 (shown by a dotted line), and , the transmitted light beam refracted and color-separated by this filter 8 enters the reading element (not shown) of the image pickup body 2 through the transmitted optical path L 1 ( shown by a solid line) that coincides with the optical path L 0 . By rotating the disk 6 and replacing the filters 7 and 8 alternately on the optical axis of the lens 5, the reading element (not shown) of the image pickup body 2 moves in the sub-scanning direction (arrow B direction). Pixel 3 can be read alternately at point P and at point Q, which is shifted by 1/2 pixel from point P in the sub-scanning direction.
Note that the distance ΔX between point P and point Q is t 1 < t 2 , n 1 = n 2 =
n, θ 1 = θ 2 = θ, the dimension of one pixel in the sub-scanning direction is
If it is 125μ, then from equation (5), ΔX=ΔX 2 −ΔX 1 =θ[t 2 −t 1 )(1−1/n) =125/2=62.5(μ).

第7図は、本発明の他の実施例を示したもの
で、第6図と同一符号のものは同一部分を示して
おり、レンズ5の光軸に向けて傾倒させて設置し
た円板6には、板厚が等しく、屈折率が異なるフ
イルタ7及び8がそれぞれ同一の取付角、すなわ
ち、入射光線が同一の入射角で入射するように取
り付けられており、フイルタ7の屈折率n2は、フ
イルタ8の屈折率n1よりも大きい。
FIG. 7 shows another embodiment of the present invention, in which the same reference numerals as in FIG. , filters 7 and 8 with the same plate thickness and different refractive indexes are installed at the same angle, that is, so that the incident light rays enter at the same angle of incidence, and the refractive index n 2 of the filter 7 is , is larger than the refractive index n 1 of the filter 8.

このように構成された本実施例では、第6図と
同様に、フイルタ7がレンズ5の光軸上に入つて
いるときには、P点にある画素3からの光線が光
路L2を通つて撮像体2の読取素子(図示せず)
に入射し、又、フイルタ8がレンズ5の光軸上に
あるときは、P点から1/2画素分副走査方向(矢
印B方向)にずれたQ点にある画素3からの光線
が光路L1を通つて撮像体2の読取素子(図示せ
ず)に入射するので、円板6を回動させてフイル
タ7及び8を交互にレンズ5の光軸上に入れ換え
れば、撮像体2の読取素子(図示せず)は副走査
方向(矢印B方向)に移動する各画素3をP点及
びQ点で交互に読み取ることができる。尚、P点
とQ点との距離ΔXは、t1=t2=t,n1<n2,θ1
θ2=θ,1画素の副走査方向の寸法を125μとする
と、(5)式より ΔX=θ・t(1/n1−1/n2)=62.5(μ) となる。
In this embodiment configured in this manner, when the filter 7 is placed on the optical axis of the lens 5, the light ray from the pixel 3 at point P passes through the optical path L2 and images are taken. Reading element on body 2 (not shown)
Also, when the filter 8 is on the optical axis of the lens 5, the light ray from the pixel 3 at the Q point, which is shifted from the P point by 1/2 pixel in the sub-scanning direction (in the direction of the arrow B), is on the optical path. Since the light enters the reading element (not shown) of the image pickup body 2 through L1 , if the disk 6 is rotated and the filters 7 and 8 are alternately placed on the optical axis of the lens 5, the image pickup body 2 A reading element (not shown) can read each pixel 3 moving in the sub-scanning direction (arrow B direction) alternately at points P and Q. Note that the distance ΔX between point P and point Q is t 1 = t 2 = t, n 1 < n 2 , θ 1 =
Assuming that θ 2 =θ and the dimension of one pixel in the sub-scanning direction is 125μ, ΔX=θ·t(1/n 1 −1/n 2 )=62.5(μ) from equation (5).

第8図は、本発明の更に他の実施例を示したも
ので、第6図と同一符号のものは同一部分を示し
ており、レンズ5の光軸に向けて傾倒させて設置
した円板6には、板厚及び屈折率が等しいフイル
タ7及び8がそれぞれ異なる取付角、すなわち、
入射光線が互いに異なる入射角で入射するように
取り付けられており、フイルタ7の円板6への取
付角はフイルタ8の円板6への取付角よりも大き
くしてあるので、フイルタ7への入射角はフイル
タ8への入射角よりも大きい。
FIG. 8 shows still another embodiment of the present invention, in which the same reference numerals as in FIG. 6 indicate the same parts. 6, filters 7 and 8 having the same plate thickness and refractive index are installed at different angles, that is,
The filter is attached so that the incident light rays are incident at different angles of incidence, and the angle at which the filter 7 is attached to the disk 6 is larger than the angle at which the filter 8 is attached to the disk 6. The angle of incidence is greater than the angle of incidence on the filter 8.

このように構成された本実施例では、第6図と
同様に、フイルタ7がレンズ5の光軸上に入つて
いるときには、P点にある画素3からの光線が光
路L2を通つて撮像体2の読取素子(図示せず)
に入射し、又、フイルタ8がレンズ5の光軸上に
あるときには、P点から1/2画素分副走査方向
(矢印B方向)にずれたQ点にある画素3からの
光線が光路L1を通つて撮像体2の読取素子(図
示せず)に入射するので、円板6を回動させてフ
イルタ7及び8を交互にレンズ5の光軸上に入れ
換えれば、撮像体2の読取素子(図示せず)は副
走査方向(矢印B方向)に移動する各画素3をP
点及びQ点で交互に読み取ることができる。尚、
P点とQ点との距離θXは、t1=t2=t,n1=n2
n,θ1<θ2,1画素の副走査方向の寸法を125μと
すると、(5)式より θX=t(θ2−θ1)(1−1/n) =62.5(μ) となる。
In this embodiment configured in this manner, when the filter 7 is placed on the optical axis of the lens 5, the light ray from the pixel 3 at point P passes through the optical path L2 and images are taken. Reading element on body 2 (not shown)
and when the filter 8 is on the optical axis of the lens 5, the light ray from the pixel 3 at point Q, which is shifted from point P by 1/2 pixel in the sub-scanning direction (direction of arrow B), follows the optical path L. 1 and enters the reading element (not shown) of the image pickup body 2. Therefore, by rotating the disc 6 and alternately replacing the filters 7 and 8 on the optical axis of the lens 5, the light of the image pickup body 2 can be read. A reading element (not shown) scans each pixel 3 moving in the sub-scanning direction (direction of arrow B) at P
It can be read alternately at point and Q point. still,
The distance θX between point P and point Q is t 1 = t 2 = t, n 1 = n 2 =
If n, θ 1 < θ 2 , and the dimension of one pixel in the sub-scanning direction is 125 μ, then from equation (5), θX = t (θ 2 − θ 1 ) (1-1/n) = 62.5 (μ) .

第9図は、本発明の更に他の実施例を示したも
ので、第1図と同一符号のものは同一部分を示し
ており、1はレンズ5の光軸に対して垂直な副走
査方向(矢印B方向)に搬送される原稿、12は
レンズ5の光軸に向けて傾倒させて設置した円板
で、この円板12に設けた開口13には平行平面
ガラス14が交互に取り付けられている〔第9図
b参照〕。15はモータ9と同期して回動するモ
ータで、このモータ15は、フイルタ7がレンズ
5の光軸上に入つているときに平行平面ガラス1
4がレンズ5の光軸上に入り、又、フイルタ8が
レンズ5の光軸上に入つているときに開口13が
レンズ5の光軸上に入るように円板12を回動す
る。
FIG. 9 shows still another embodiment of the present invention, in which the same reference numerals as in FIG. 1 indicate the same parts, and 1 indicates the sub-scanning direction perpendicular to the optical axis of the lens 5. The document 12 is tilted toward the optical axis of the lens 5 and is installed in the direction of the arrow B. Parallel plane glasses 14 are alternately attached to the openings 13 provided in the disk 12. [See Figure 9b]. 15 is a motor that rotates in synchronization with the motor 9, and this motor 15 rotates the parallel plane glass 1 when the filter 7 is placed on the optical axis of the lens 5.
4 is placed on the optical axis of the lens 5, and when the filter 8 is placed on the optical axis of the lens 5, the disc 12 is rotated so that the aperture 13 is placed on the optical axis of the lens 5.

このように構成された本実施例では、フイルタ
7及び平行平面ガラス14がレンズ5の光軸上に
入つているときには、平行平面ガラス14がない
ときに撮像体2の読取素子(図示せず)に入射す
る光線の光路L0(実線で図示)の原稿1側の焦点
Oから反副走査方向(矢印B方向と反対方向)に
1/2画素分ずれたP点から発した画素3の光線は、
入射光路L1(点線で図示)を通つて、先ず、フイ
ルタ7によつて色分解され、次に、平行平面ガラ
ス14によつて屈折された後、光路L0と一致し
た透過光路L1(実線で図示)を通つて撮像体2の
読取素子(図示せず)に入射し、又、フイルタ8
及び開口13がレンズ5の光軸上に入つていると
きには、O点から発した画素3の光線は、入射光
路L0(実線で図示)を通つてフイルタ8に入射
し、且つ、このフイルタ8によつて色分解された
透過光線が撮像体2の読取素子(図示せず)に入
射するので、円板6を回動させてフイルタ7及び
8と平行平面ガラス14及び開口13とを交互に
レンズ5の光軸上に入れ換えれば、撮像体2の読
取素子(図示せず)は副走査方向(矢印B方向)
に移動する各画素3をP点及O点で交互に読み取
ることができる。尚、O点とP点との距離ΔX
は、(1)式より、平行平面ガラス14の板厚をt、
平行平面ガラス14の屈折率をn、平行平面ガラ
ス14への光線L1の入射角をθとすると、(1)式
より、 ΔX=t・θ(1−1/n) となる。
In this embodiment configured as described above, when the filter 7 and the parallel plane glass 14 are placed on the optical axis of the lens 5, the reading element (not shown) of the image pickup body 2 The light beam of pixel 3 is emitted from point P, which is shifted by 1/2 pixel in the anti-sub-scanning direction (the direction opposite to arrow B) from the focal point O on the document 1 side of the optical path L 0 (shown by the solid line) of the light ray that enters the teeth,
Passing through the incident light path L 1 (shown by the dotted line), it is first color-separated by the filter 7 and then refracted by the plane-parallel glass 14, followed by the transmitted light path L 1 (which coincides with the light path L 0 ). It enters the reading element (not shown) of the image pickup body 2 through the filter 8 (shown with a solid line).
When the aperture 13 is on the optical axis of the lens 5, the light beam of the pixel 3 emitted from the point O enters the filter 8 through the incident optical path L0 (shown as a solid line), and The transmitted light beams separated by color are incident on the reading element (not shown) of the image pickup body 2, so by rotating the disc 6, the filters 7 and 8, the parallel plane glass 14, and the aperture 13 are alternately connected. If it is replaced on the optical axis of the lens 5, the reading element (not shown) of the image pickup body 2 will move in the sub-scanning direction (direction of arrow B).
Each pixel 3 that moves can be read alternately at point P and point O. In addition, the distance ΔX between point O and point P
From equation (1), the thickness of the parallel plane glass 14 is t,
If the refractive index of the plane-parallel glass 14 is n, and the angle of incidence of the light beam L1 on the plane-parallel glass 14 is θ, then from equation (1), ΔX=t·θ(1-1/n).

尚、本発明の実施例では、原稿1に描かれた画
像を2色に色分解する例で説明したが、画像をm
色に色分解するには、m色のフイルタを円板に配
列するか、又は(m−1)枚の平行平面ガラスを
円板のm個の開口に配列し、各読取位置の間隔を
125/m(μ)とすればよい。
In the embodiment of the present invention, the image drawn on the document 1 is separated into two colors.
To separate the colors into colors, either m-color filters are arranged on a disk, or (m-1) pieces of parallel flat glass are arranged in m apertures of the disk, and the intervals between each reading position are set as follows.
It may be 125/m (μ).

以上説明したように、本発明によれば、レンズ
の光軸に向けて傾倒した円板に、色が異なり、且
つ、板厚、屈折率及び光線の入射角の内の少なく
とも1つの要素が異なる複数のフイルタ又は板
厚、屈折率及び光線の入射角の内の少なくとも1
つの要素が異なる複数の平行平面ガラスを配列す
ることにより、色の異なるフイルタに入れ換わる
間に原稿が副走査方向に搬送されても、原稿側の
入射光路のみがずれて撮像体側の透過光路が一定
の状態で原稿を読み取ることができるので、各画
素を正確に色分解できる利点があり、又、撮像体
及びレンズが1個でよいため、色情報読取装置の
価格が安くなり、又、光学的な調整も簡単である
という利点がある。更に、第9図に示した実施例
によれば、本発明の装置を従来の色情報読取装置
に付加すれば、容易に従来の装置の欠点を解消す
ることができる利点がある。
As explained above, according to the present invention, the discs tilted toward the optical axis of the lens have different colors and differ in at least one element among the plate thickness, refractive index, and incident angle of light rays. At least one of a plurality of filters or plate thicknesses, refractive indexes, and incident angles of light rays.
By arranging multiple parallel plane glasses with different color elements, even if the document is conveyed in the sub-scanning direction while filters of different colors are being replaced, only the incident optical path on the document side will be shifted and the transmitted optical path on the image pickup side will be changed. Since the document can be read in a constant state, each pixel can be accurately separated into colors, which has the advantage of being able to accurately separate each pixel.Also, since only one image pickup body and lens are required, the price of the color information reading device is low, and optical It has the advantage of being easy to make adjustments. Furthermore, the embodiment shown in FIG. 9 has the advantage that by adding the device of the present invention to a conventional color information reading device, the drawbacks of the conventional device can be easily overcome.

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

第1図は従来の色情報読取装置の構成図、第2
図は原稿面の読取状態図、第3図及び第4図は従
来の色情報読取装置の構成図、第5図は本発明の
原理の説明図、第6図乃至第9図は本発明の実施
例の構成図ある。 1……原稿、2……撮像体、3……画素、4…
…ローラ、5……レンズ、6,12……円板、
7,8……フイルタ、9,15……モータ、1
0,11……平面鏡、13……開口、14……平
行平面ガラス。
Figure 1 is a configuration diagram of a conventional color information reading device;
3 and 4 are configuration diagrams of a conventional color information reading device. FIG. 5 is an explanatory diagram of the principle of the present invention. There is a configuration diagram of an embodiment. 1... Original, 2... Imaging body, 3... Pixel, 4...
...roller, 5...lens, 6, 12...disk,
7, 8... Filter, 9, 15... Motor, 1
0, 11...Plane mirror, 13...Aperture, 14...Parallel plane glass.

Claims (1)

【特許請求の範囲】 1 原稿の画像を撮像体の読取素子に結像させる
レンズと、このレンズの光軸に向けて傾倒した円
板と、この円板を回動する駆動装置と、前記円板
に配列する、板厚、屈折率及び前記円板への取付
角の内の少なくとも1つの要素が異なり且つ色が
異なる複数のフイルタとから成り、前記レンズの
光軸に平行な複数の光路を経て前記フイルタに入
射する光線を前記フイルタによつて色分解すると
同時に屈折させ、前記フイルタを透過した光線を
1つの光路に一致させることを特徴とする色情報
読取装置。 2 原稿の画像を撮像体の読取素子に結像させる
レンズと、この光軸に対して垂直に設けた第1の
円板と、この第1の円板を回動する第1の駆動装
置と、前記第1の円板に配列する、色の異なつた
複数のフイルタと、前記レンズの光軸に向けて傾
倒した第2の円板と、前記第1の駆動装置に同期
して前記第2の円板を回動する第2の駆動装置
と、前記第2の円板に配列する、板厚、屈折率及
び前記第2の円板への取付角の内の少なくとも1
つの要素が異なる複数の平行平面ガラスとから成
り、前記第1の円板及び前記第2の円板を同期さ
せて回動して、前記レンズの光軸に平行な複数の
光路を経て前記フイルタ及び前記平行平面ガラス
に入射する光線を、前記フイルタによつて色分解
し、且つ、前記平行平面ガラスによつて屈折さ
せ、前記平行平面ガラスを透過した光線を1つの
光路に一致させることを特徴とする色情報読取装
置。 3 前記第2の円板に前記平行平板ガラスを配列
しない開口を少なくとも1つ設けたことを特徴と
する特許請求の範囲第2項記載の色情報読取装
置。
[Scope of Claims] 1. A lens that forms an image of a document on a reading element of an image pickup body, a disk tilted toward the optical axis of the lens, a drive device that rotates the disk, and a drive device that rotates the disk. A plurality of filters are arranged on a plate and differ in at least one element among the plate thickness, refractive index, and attachment angle to the disc, and are different in color, and the filters are arranged on a plate to form a plurality of optical paths parallel to the optical axis of the lens. A color information reading device characterized in that the light rays incident on the filter are color-separated and refracted by the filter, and the light rays transmitted through the filter are made to coincide with one optical path. 2. A lens that forms an image of a document on a reading element of an image pickup body, a first disk provided perpendicular to the optical axis, and a first drive device that rotates the first disk. , a plurality of filters of different colors arranged on the first disk, a second disk tilted toward the optical axis of the lens, and a second drive device in synchronization with the first drive device. a second drive device for rotating a disc; and at least one of plate thickness, refractive index, and attachment angle to the second disc arranged on the second disc;
The first disk and the second disk are rotated in synchronization to pass the filter through a plurality of optical paths parallel to the optical axis of the lens. and the light rays incident on the parallel plane glass are color separated by the filter, and are refracted by the parallel plane glass, so that the light rays transmitted through the parallel plane glass are made to coincide with one optical path. Color information reading device. 3. The color information reading device according to claim 2, wherein the second circular plate is provided with at least one opening in which the parallel flat glass is not arranged.
JP4865880A 1980-04-15 1980-04-15 Color information reader Granted JPS56153314A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4865880A JPS56153314A (en) 1980-04-15 1980-04-15 Color information reader

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4865880A JPS56153314A (en) 1980-04-15 1980-04-15 Color information reader

Publications (2)

Publication Number Publication Date
JPS56153314A JPS56153314A (en) 1981-11-27
JPS648806B2 true JPS648806B2 (en) 1989-02-15

Family

ID=12809437

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4865880A Granted JPS56153314A (en) 1980-04-15 1980-04-15 Color information reader

Country Status (1)

Country Link
JP (1) JPS56153314A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
GB8421512D0 (en) * 1984-08-24 1984-09-26 Crosfield Electronics Ltd Image enhancement
JPS62200969A (en) * 1986-02-28 1987-09-04 Usac Electronics Ind Co Ltd Color information reader compensating color aberration
JPS62246033A (en) * 1986-04-19 1987-10-27 Konika Corp Color recording device with filter and diaphragm incorporated lens
JP2539203B2 (en) * 1986-12-18 1996-10-02 富士通株式会社 Color reading mechanism
DE3922512A1 (en) * 1989-07-08 1991-01-17 Kodak Ag DEVICE FOR CONVERTING LIGHT SIGNALS TO VIDEO SIGNALS
JP2007057848A (en) * 2005-08-24 2007-03-08 Sharp Corp Chromatic aberration correction method and projector

Also Published As

Publication number Publication date
JPS56153314A (en) 1981-11-27

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