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JPS58115455A - Imaging device - Google Patents

Imaging device

Info

Publication number
JPS58115455A
JPS58115455A JP21325181A JP21325181A JPS58115455A JP S58115455 A JPS58115455 A JP S58115455A JP 21325181 A JP21325181 A JP 21325181A JP 21325181 A JP21325181 A JP 21325181A JP S58115455 A JPS58115455 A JP S58115455A
Authority
JP
Japan
Prior art keywords
luminance
temperature
fluorescent
light
magnetic field
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP21325181A
Other languages
Japanese (ja)
Inventor
Sadatsugu Miura
三浦 禎次
Yoshiyuki Gomi
五味 芳行
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.)
Seiko Epson Corp
Suwa Seikosha KK
Original Assignee
Seiko Epson Corp
Suwa Seikosha KK
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 Seiko Epson Corp, Suwa Seikosha KK filed Critical Seiko Epson Corp
Priority to JP21325181A priority Critical patent/JPS58115455A/en
Publication of JPS58115455A publication Critical patent/JPS58115455A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G15/00Apparatus for electrographic processes using a charge pattern
    • G03G15/04Apparatus for electrographic processes using a charge pattern for exposing, i.e. imagewise exposure by optically projecting the original image on a photoconductive recording material
    • G03G15/04036Details of illuminating systems, e.g. lamps, reflectors

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Light Sources And Details Of Projection-Printing Devices (AREA)

Abstract

PURPOSE:To correct a drop of light quantity in the end part, and to get rid of an uneven light intensity distribution, by using a gas discharge tube of high luminance and low power, holding it at a constant temperature, and increasing the intensity of a light source by a magnetic field. CONSTITUTION:A titled device is provided with a temperature detecting element 45 for controlling a fluorescent lamp at a constant temperature, a fluorescent lamp heating device 44 and a temperature controlling circuit 45. When a temperature in a fluorescent lamp housing 46 has been set to 40-50 deg.C by this temperature controller, the highest luminance having a distribution of a balanced time can be obtained. In order to eliminate a luminance distribution in this balanced time, a samarium cobalt magnet 41 is installed to a luminance drop part 47, and a magnetic field of 600 gauss falling at right angles with length of a fluorescent tube is applied. As a result, a uniform luminance distribution curve whose uneven luminance is <=5% can be obtained. As for the magnet, a ferrite magnet, etc. are available, and in an optional fluorescent body other than an aluminate fluorescent material, and an optional discharge tube (a mercury lamp and a sodium lamp) are effective as well.

Description

【発明の詳細な説明】 本発明は、ゼログラフィ技術応用の印写装置、より詳し
くは、複写機或いは光プリンターの光源に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a printing device applying xerographic technology, and more particularly to a light source for a copying machine or an optical printer.

本発明の目的は、^速、高品質の印写を行なうために1
崗辺光量ムラのない高輝度、平面光源を得るととkある
The purpose of the present invention is to:
It is possible to obtain a high-brightness, flat light source with no unevenness in the amount of light.

複写機において、ハロゲンランプは高い出力の光源とし
て広く用いられている。しかしノ10ゲンランブは消費
電力が大きく、コストも高いため、廉価で高い光出力の
得られるアパーチャ型壁光灯に置き換えられようとして
いる。第一図には高輝縦壁光灯の例として、アパーチャ
型壁光灯を示すこの螢光灯は、螢光管1.1内に、反射
層15と螢光体層14とを有し、透明アパーチャ窓によ
り、指向のある高い光エネルギーを得ることが出来、感
光ドラムの分光感f%性4cll和した発光スペクトル
を有する螢光体を使用する事により、優れた光源となっ
ている。しかし、この螢光灯は、螢光灯の長さ方向に%
第2図の如き光量分布を有し、例えば、長さ5番−のも
のでは、中心から10am離れたところで、中心に比し
て2G−50%の輝度低下を生ずる。光学的なスリット
勢による光量分布の均一化をはかることは一般的に行な
われているが、これではiir*形成のための光エネル
ギーが減少し、プロセス速度が遅くなる欠点を有してい
る。このため、中心部の光量に対して、周辺部の光量を
増すことが望まれる。
In copying machines, halogen lamps are widely used as high output light sources. However, 10-gen lamps consume a lot of power and are expensive, so they are being replaced by aperture-type wall lamps that are inexpensive and provide high light output. FIG. 1 shows an aperture-type wall light as an example of a high-brightness vertical wall light. This fluorescent light has a reflective layer 15 and a phosphor layer 14 in a fluorescent tube 1.1. The transparent aperture window makes it possible to obtain high, directional light energy, and the use of a phosphor having an emission spectrum that is equal to the spectral sensitivity of the photosensitive drum (f%) makes it an excellent light source. However, this fluorescent lamp has % in the length direction of the fluorescent lamp.
For example, if the light intensity distribution is as shown in FIG. 2, and the length is 5, the luminance decreases by 2G-50% at a distance of 10 am from the center compared to the center. Although it is common practice to use optical slits to make the light intensity distribution uniform, this method has the disadvantage that the light energy for forming iir* is reduced and the process speed is slowed down. For this reason, it is desirable to increase the amount of light at the periphery relative to the amount of light at the center.

本発明は、このような要請に応えるものであり、本発明
による、光源の動作原理を第111に示す。
The present invention responds to such demands, and the operating principle of the light source according to the present invention is shown in the 111th section.

透明窓12を有するアパーチャ蓋壁光灯11のフィラメ
ント電極AIK交流電圧を印加して点灯動作している処
に1磁場s4を加える。螢光管内の荷電粒子52は、磁
場がない時には、交流電界によって加速され、平均自由
性ILL走行後に中性の粒子或いは逆極性の荷電粒子5
6と衝突し、紫外線及び可紫光線を発生する。螢色螢光
灯に於ては、−E紀紫外線或いは可視光線が^い効率に
て螢光体を励起し、高輝腹壁色光を発生する。
One magnetic field s4 is applied to the filament electrode of the aperture cover wall light 11 having the transparent window 12 where the AIK AC voltage is applied and the lighting operation is performed. When there is no magnetic field, the charged particles 52 in the fluorescent tube are accelerated by an alternating current electric field, and after the mean-freedom ILL travel, they become neutral particles or charged particles 5 of opposite polarity.
6 and generates ultraviolet and violet rays. In a fluorescent lamp, -E ultraviolet or visible light excites the phosphor with high efficiency, producing high-brightness abdominal wall color light.

これに対し、磁場を印加したときには、交流電界による
力に加えて、ai場54による新たなる力を受ける。(
第5図B)交流電界に直交する向きに磁場を印加すると
き、図示する様な軌跡を運動する。この運動は磁場がな
いときの単位時間当りの運動距離と較べて、磁場が有る
時の運動距離が増えるので、結果的に単位時間当りの衝
突確立が増えるととに和尚する。この結果、発光する紫
、外線の増加に伴なう輝度の向上が得られる。
On the other hand, when a magnetic field is applied, in addition to the force due to the alternating current electric field, a new force due to the AI field 54 is applied. (
Figure 5B) When a magnetic field is applied in a direction perpendicular to the alternating current electric field, it moves along a trajectory as shown. Compared to the distance traveled per unit time when there is no magnetic field, this motion increases the distance traveled when a magnetic field is present, and as a result, the probability of collision per unit time increases. As a result, brightness can be improved as the amount of violet and external rays emitted increases.

以下、本発明による祥細な実施例を述べる。Detailed embodiments according to the present invention will be described below.

実m例1 本発明による^輝度均−強度分布螢光灯の構成を第4図
に示す、第5図には、ここに用いる管長65−、アパー
チャ幅4騙によるアルイン酸塩螢光体を有する警光灯の
輝度分布特性の一町を示す。
Practical Example 1 Figure 4 shows the configuration of the uniform-luminance-intensity-distributed fluorescent lamp according to the present invention. Figure 5 shows an aluminate phosphor with a tube length of 65 mm and an aperture width of 4 mm used here. This figure shows one example of the brightness distribution characteristics of warning lights.

この結果、平衡時52においてもム4紙に必要な有効幅
に対して25%の光量ムラが生じていることがわかる。
As a result, it can be seen that even at the equilibrium state 52, there is a 25% unevenness in the amount of light with respect to the effective width required for the four sheets of paper.

また、環境の温度震動に起因する螢光管内水銀蒸気圧力
の変動による輝度分布の非平衡時51には、更に多くの
光量ムラを生じている。
Further, when the brightness distribution is not balanced 51 due to fluctuations in the mercury vapor pressure within the fluorescent tube due to environmental temperature fluctuations, even more unevenness in the amount of light occurs.

このため、環境条件の変動に対応する輝度分布の変動を
除去する事が必要となり、そのために警光灯を一定温度
に制御するための温度検出素子4sと警光灯加熱装置4
4と温度制御回路45と備える。かかる温度制御装置に
て、警光灯框体46内亀度を40〜50℃に設定したと
1、前記平衡時の分布を有する最高輝度を得ることが出
来る。この平衡時の輝度分布を無くすために1輝度低下
部47にサマリウムコバルト磁石41を設置し、螢光管
長に直交する600ガウスの磁界を印加する。
For this reason, it is necessary to eliminate fluctuations in the brightness distribution corresponding to fluctuations in environmental conditions, and for this purpose, a temperature detection element 4s and a warning light heating device 4 are used to control the warning light to a constant temperature.
4 and a temperature control circuit 45. In such a temperature control device, if the internal temperature of the warning light frame 46 is set to 40 to 50° C., the maximum brightness having the above-mentioned equilibrium distribution can be obtained. In order to eliminate this brightness distribution at the time of equilibrium, a samarium cobalt magnet 41 is installed in the one brightness reduction section 47, and a magnetic field of 600 Gauss perpendicular to the length of the fluorescent tube is applied.

この結果、輝度ムラS−以下の均一輝度分布曲線55を
得ることが出来る0本発明では上記ナマリウムーコバル
ト磁石の例を説明したが、フェライト磁石などその他の
磁石でも適用でき、更に警光灯としてアルイン酸塩螢光
体以外の任意の螢光体、警光灯以外の任意の放電管(水
銀灯−ナトリウムランプ等)でも有効である。
As a result, a uniform brightness distribution curve 55 with a brightness unevenness of S- or less can be obtained. In the present invention, the above-mentioned Namarium-Cobalt magnet has been described as an example, but other magnets such as ferrite magnets can also be applied, and furthermore, it can be used as a warning light. Any phosphor other than the aluminate phosphor and any discharge tube other than the warning light (mercury lamp-sodium lamp, etc.) are also effective.

実施例2 本発明による上記螢光灯源61、高速応答液晶マイクロ
シャッターアレー62、収束性光フアイバーレンズアレ
ー6易、感光体64、現倫装置65、定着装置66から
なる光プリンターを第4図に示す、温度制御装置と輝度
補正用磁石68とを有する管長550゛−管径25■φ
、アルずン酸塩螢光体による発光波長550■アパ一チ
ヤ幅4■の警光灯を18アンペアの高鳩波電流にて点灯
し、警光灯から101離れた位置に、100ハロの電気
的スイッチング可能なマイクロアパーデャを1G個/■
の密度にて20m+書入巾を有する^速液晶シャッター
アレー62と開口角20度明るさF1相当の収束性光フ
アイバーレンズアレー63とからなり、警光灯から出発
した入射角20度の光は、液晶シャッターの制御信号に
対応して、上記収束性光フアイバーレンズアレーの働き
により、上記液昂マイクロアパーチャ像を感光体64上
に静電潜像として形成する。この静電潜像を、磁性トナ
ーを用いた現俸器66によりlAg1シ、^正コロナに
よる転写器67を用いてA4寸法の曹通紙1に転写し、
熱又は圧力寓着することKより所望のプリシトが得られ
る。輝度補正用磁場のない光11においては5枚/分の
書入み速度に於て、周辺部でのプリント濃度ムラが顕著
なのに対して、輝度補正用磁石を用いる周辺部でのプリ
ント濃度ムラがなくなり、印写スピードも2割向上する
ことが出来た。
Embodiment 2 FIG. 4 shows an optical printer according to the present invention, which comprises the above-mentioned fluorescent light source 61, high-speed response liquid crystal micro-shutter array 62, convergent optical fiber lens array 6, photoreceptor 64, optical device 65, and fixing device 66. A tube length of 550゛ and a tube diameter of 25■φ has a temperature control device and a brightness correction magnet 68 as shown in FIG.
A warning light with an emission wavelength of 550 cm and an aperture width of 4 cm, which is made of an arusunate phosphor, is lit with a high dove wave current of 18 amperes, and a light of 100 ha is placed at a distance of 10 cm from the warning light. 1G electrically switchable micro apertures/■
It consists of a high-speed liquid crystal shutter array 62 with a writing width of 20 m + writing width at a density of , the liquid micro-aperture image is formed as an electrostatic latent image on the photoreceptor 64 by the action of the convergent optical fiber lens array in response to a control signal of the liquid crystal shutter. This electrostatic latent image is transferred onto A4 size paper 1 using a transfer device 67 using a magnetic toner and a transfer device 67 using a positive corona.
By applying heat or pressure, the desired precipitate can be obtained. With light 11 without a brightness correction magnetic field, print density unevenness in the peripheral area is noticeable at a writing speed of 5 sheets per minute, whereas print density unevenness in the peripheral area using a brightness correction magnet is noticeable. The printing speed was improved by 20%.

以上、本発明は印写装置用光源として、高輝度低電力の
ガス放電管を用いるもので、発光部端部における光量の
低下を補正するために磁場による光源強度の増大をはか
り、かつ外界環境の変動に起因する光強度分布ムラをな
くすために光源を画定i1度に保つものである。この結
果、高出力均−元エネルギー分布の光源を実現すること
kより、従来の印写装置の卵重濃度ムラをなくシ、為速
応答を可能にするものである。
As described above, the present invention uses a high-intensity, low-power gas discharge tube as a light source for a printing device, and uses a magnetic field to increase the light source intensity in order to compensate for a decrease in the amount of light at the end of the light emitting part. In order to eliminate unevenness in the light intensity distribution caused by fluctuations in the light intensity, the light source is kept at a defined i1 degree. As a result, by realizing a light source with a high output and uniform energy distribution, it is possible to eliminate the uneven egg weight density of the conventional printing apparatus and to achieve a fast response.

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

第1図は本発明に用いる警光灯の外観と断面構造を示す
。 11・−・・・・螢光管 12・・・・・・アパーチャ透明窓 15・・・・−反射層 14−・・・・・螢光体層 第2図は、上記警光灯の管長方向に対する光強度分布を
示す。 第5図は、本発明の動作原理を示す。 ムは磁場なしKおける動作原理を示し、Bは磁場ありに
おける動作原理を示す。 5゛1−・・・フィラメント 52・−一運動荷電粒子 55−・・・中性又は逆極性粒子 54・・・・−磁場 第4図は、本発明による螢光灯光源の構成を示す。 41・・・−磁石 42・・・・・・高鳩波電極 45−・−・Ii&検出素子 44−−−−加熱装置 45・−一温度制御回路 46・−自覚源框体 47・・・・・・輝度低下部 第5図は警光灯の輝度分布特性を示す。 51 ・・・−・非平衡時の不安定非対称輝度分布52
・・・−・平衡時の輝度分布 5ト・・一本発明による輝度補正後の輝置分布第6図は
、本発@における光プリンターの構成を示す。 61・−一・警光灯 62・・−・・・液晶マイクロシャッターアレー65・
・・・・・収速性光ファイノ(−レンズアレー64・・
・・・・感光ドラム 65・・・・・・IA倫器 66・・・・一定着器 67・・・・・・転写器 6B・・・・・・磁石。 以上 出願人 株式会社 霧訪精工舎 代理人弁理士 最 上  務 A         /a′。 第1図 第2図 ) β   ノ≦ 第3図 第4図 2 第6図
FIG. 1 shows the appearance and cross-sectional structure of a warning light used in the present invention. 11...Fluorescent tube 12...Aperture transparent window 15...-Reflection layer 14-...Fluorescent layer Figure 2 shows the tube length of the above warning light. Shows the light intensity distribution with respect to direction. FIG. 5 shows the principle of operation of the invention. Symbol K indicates the operating principle in the absence of a magnetic field, and B indicates the operating principle in the presence of a magnetic field. 5.1 - Filament 52 - Monokinetic charged particles 55 - Neutral or opposite polarity particles 54 - Magnetic field FIG. 4 shows the construction of a fluorescent light source according to the invention. 41...-Magnet 42...High pigeon wave electrode 45--Ii & detection element 44--Heating device 45--Temperature control circuit 46--Sensitive source frame 47... . . . Luminance Reduction Section FIG. 5 shows the luminance distribution characteristics of the warning light. 51 ...--Unstable asymmetric brightness distribution in non-equilibrium 52
. . . Brightness distribution at equilibrium (5) Brightness distribution after brightness correction according to the present invention FIG. 6 shows the configuration of the optical printer according to the present invention. 61・-1・Warning light 62・・・LCD micro shutter array 65・
...Accurate optical fin (-lens array 64...
... Photosensitive drum 65 ... IA connection device 66 ... Fixed attachment device 67 ... Transfer device 6B ... Magnet. The above applicant is Kiriwa Seikosha Co., Ltd. Representative Patent Attorney Tsumugi Mogami A/a'. Figure 1 Figure 2) β ≦ Figure 3 Figure 4 2 Figure 6

Claims (1)

【特許請求の範囲】 1)ゼログラフィプロセスを有する印写装置に於て、腋
ゼログラフィプロセスのための照明光源を有し、腋照明
光源は、ガス放電管と磁場尭生装置とからなり、該磁場
尭生装置は骸ガス放電管の発光部の端部に設置したこと
を特徴とする印、i*置 2)上記照明光源は、アパーチャ■螢光灯と磁場発生装
置と皺照明光源を一定温度に保つ定温装置とから成るこ
とを特徴とする特許−求範囲第一項記載の印写装置 S)液晶マイクiシャッターと収束性光フアイバーレン
ズアレーと感光体とを有することを特徴とする特許請求
範囲第2項記載の印写袈置
[Scope of Claims] 1) A printing apparatus having a xerography process, comprising an illumination light source for the armpit xerography process, the armpit illumination light source comprising a gas discharge tube and a magnetic field generating device, 2) The above-mentioned illumination light source has an aperture, a fluorescent lamp, a magnetic field generator, and a wrinkle illumination light source. A printing apparatus according to item 1 of the patent-requested scope characterized in that it comprises a constant temperature device that maintains the temperature at a constant temperature S) A printing apparatus characterized in that it has a liquid crystal microphone i-shutter, a converging optical fiber lens array, and a photoreceptor. Imprint holder set forth in claim 2
JP21325181A 1981-12-28 1981-12-28 Imaging device Pending JPS58115455A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP21325181A JPS58115455A (en) 1981-12-28 1981-12-28 Imaging device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP21325181A JPS58115455A (en) 1981-12-28 1981-12-28 Imaging device

Publications (1)

Publication Number Publication Date
JPS58115455A true JPS58115455A (en) 1983-07-09

Family

ID=16636004

Family Applications (1)

Application Number Title Priority Date Filing Date
JP21325181A Pending JPS58115455A (en) 1981-12-28 1981-12-28 Imaging device

Country Status (1)

Country Link
JP (1) JPS58115455A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4891664A (en) * 1987-06-15 1990-01-02 Minolta Camera Kabushiki Kaisha Illumination device for copying apparatus and the like

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5611847A (en) * 1979-07-09 1981-02-05 Matsushita Electric Works Ltd Flat-shaped electric discharge lamp
JPS5624372A (en) * 1979-08-02 1981-03-07 Ricoh Co Ltd Image recording method and its device
JPS5697962A (en) * 1979-12-29 1981-08-07 Matsushita Electric Works Ltd Lighting device for fluorescent lamp

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5611847A (en) * 1979-07-09 1981-02-05 Matsushita Electric Works Ltd Flat-shaped electric discharge lamp
JPS5624372A (en) * 1979-08-02 1981-03-07 Ricoh Co Ltd Image recording method and its device
JPS5697962A (en) * 1979-12-29 1981-08-07 Matsushita Electric Works Ltd Lighting device for fluorescent lamp

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4891664A (en) * 1987-06-15 1990-01-02 Minolta Camera Kabushiki Kaisha Illumination device for copying apparatus and the like

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