JPS638757A - Image forming method - Google Patents
Image forming methodInfo
- Publication number
- JPS638757A JPS638757A JP15367186A JP15367186A JPS638757A JP S638757 A JPS638757 A JP S638757A JP 15367186 A JP15367186 A JP 15367186A JP 15367186 A JP15367186 A JP 15367186A JP S638757 A JPS638757 A JP S638757A
- Authority
- JP
- Japan
- Prior art keywords
- toner
- substrate
- polarity
- image forming
- forming method
- 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
Links
- 238000000034 method Methods 0.000 title claims description 24
- 239000000758 substrate Substances 0.000 claims abstract description 65
- 230000005684 electric field Effects 0.000 claims abstract description 23
- 238000011144 upstream manufacturing Methods 0.000 claims description 11
- 238000013459 approach Methods 0.000 claims description 2
- 239000003989 dielectric material Substances 0.000 claims description 2
- 230000002238 attenuated effect Effects 0.000 abstract description 4
- 230000003111 delayed effect Effects 0.000 abstract description 3
- 230000000052 comparative effect Effects 0.000 description 4
- 238000002834 transmittance Methods 0.000 description 4
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 3
- 229910052782 aluminium Inorganic materials 0.000 description 3
- 238000010586 diagram Methods 0.000 description 3
- 239000011521 glass Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 1
- 230000008034 disappearance Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 238000003384 imaging method Methods 0.000 description 1
- 239000010410 layer Substances 0.000 description 1
- 239000002356 single layer Substances 0.000 description 1
Landscapes
- Electrophotography Using Other Than Carlson'S Method (AREA)
Abstract
Description
【発明の詳細な説明】
(産業上の利用分野)
本発明は光導電性トナーを用いた画像形成方法に関する
。DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to an image forming method using a photoconductive toner.
(従来の技術) 光導電性トナーは、光を吸収して導電性を増し。(Conventional technology) Photoconductive toner absorbs light and increases its conductivity.
電極との間で電荷授受を行う結果、その極性が反転する
という特徴を有している。このようなトナーを用いた画
像形成方法を第6図に示す。It has the characteristic that the polarity is reversed as a result of transferring charge between the electrode and the electrode. An image forming method using such toner is shown in FIG.
まず1円筒状をしたアルミニウムなどの導電性基板31
上に1例えば正極性に帯電されたトナーを均一に付着さ
せる。次いで、導電性基板31に対向してネサガラスの
ような透明電極32を配設し、導電性基板31と透明電
極32との間に電界を生じさせる。このような状態で、
透明電極32の上方がら原稿像をトナ一層に露光する。First, a cylindrical conductive substrate 31 made of aluminum or the like.
For example, positively charged toner is uniformly deposited thereon. Next, a transparent electrode 32 such as Nesa glass is placed opposite the conductive substrate 31, and an electric field is generated between the conductive substrate 31 and the transparent electrode 32. In this situation,
The original image is exposed to a single layer of toner from above the transparent electrode 32.
原稿像以外の露光されたトナーは導電性を得て、その正
電荷は導電性基板31を通じて消失し、さらに導電性基
板31と透明電極32との間の電界により負極性となる
。露光されないトナーは正極性を維持する。このように
して、導電性基板31上には、原稿像に対応した正極性
のトナー像が形成される。この正極性のトナー像が転写
紙上に転写されることにより、所定の複写画像が得られ
る。The exposed toner other than the original image becomes conductive, its positive charge disappears through the conductive substrate 31, and further becomes negative polarity due to the electric field between the conductive substrate 31 and the transparent electrode 32. Toner that is not exposed maintains positive polarity. In this way, a positive toner image corresponding to the original image is formed on the conductive substrate 31. A predetermined copy image is obtained by transferring this positive polarity toner image onto a transfer paper.
光導電性トナーを用いた従来の画像形成方法では、光導
電性トナーを電界内に位置させた状態でそのトナーに原
稿像を露光する。このため、露光されたトナーの極性は
反転され、露光されないトナーとは逆極性になり、転写
時には、いずれか一方の極性のトナーのみが確実に転写
される。従って、得られる複写画像はコントラストのは
っきりしたものとなる。In conventional imaging methods using photoconductive toner, a document image is exposed to the photoconductive toner while the toner is positioned within an electric field. Therefore, the polarity of the exposed toner is reversed and becomes the opposite polarity of the unexposed toner, and during transfer, only toner of one of the polarities is reliably transferred. Therefore, the obtained copy image has a clear contrast.
しかし、トナー露光と同時に、該露光トナーを帯電時の
極性とは反対の極性とすべく、帯電されたトナー全体を
電界内に位置させると、非露光トナーの表面電位も同時
に減衰される。この露光から転写までの間に、非露光ト
ナーの表面電位が激しく減衰され、得られる画像のコン
トラストは低下する。帯電されたトナーを電界内に位置
させて露光する場合には、透明電極やスリットを有する
電極を基板に接触あるいは近接させなければならず、ト
ナ一層を乱すおそれもある。However, when the entire charged toner is placed in an electric field so that the exposed toner has a polarity opposite to the polarity at the time of charging at the same time as the toner is exposed, the surface potential of the unexposed toner is also attenuated at the same time. Between this exposure and transfer, the surface potential of the unexposed toner is severely attenuated, and the contrast of the resulting image is reduced. When the charged toner is placed in an electric field and exposed to light, a transparent electrode or an electrode having a slit must be brought into contact with or close to the substrate, which may disturb the toner layer.
(発明が解決しようとする問題点)
本発明は上記従来の問題点を解決するものであり、その
目的は、高コントラストの複写画像が得られる画像形成
方法を提供することにある。(Problems to be Solved by the Invention) The present invention solves the above-mentioned conventional problems, and its purpose is to provide an image forming method that can obtain a high-contrast copy image.
(問題点を解決するための手段)
本発明は、帯電された光導電性トナーを露光しその電荷
を消失させると共に電界内に位置させて電荷を消失した
該トナーに帯電時のトナー極性とは逆極性の電荷を付与
し9次いで一方の極性のトナーを転写紙に静電的に転写
して画像を得る画像形成方法であり、帯電された光導電
性トナーを露光するタイミングと、電荷を消失したトナ
ーに帯電時のトナー極性とは逆極性の電荷を付与するタ
イミングとを異ならせてなり、そのことにより上記目的
が達成される。(Means for Solving the Problems) The present invention exposes a charged photoconductive toner to light to eliminate its charge, and the toner is placed in an electric field to eliminate its charge. This is an image forming method in which an image is obtained by applying a charge of opposite polarity and then electrostatically transferring toner of one polarity to transfer paper, and the timing of exposing the charged photoconductive toner to light and the disappearance of the charge are determined The above-mentioned object is achieved by changing the timing at which a charge having a polarity opposite to the toner polarity at the time of charging is applied to the charged toner.
(実施例) 以下に本発明を、実施例について説明する。(Example) The present invention will be described below with reference to Examples.
本発明方法には1例えば、第1図に示すように。The method of the present invention includes one method, for example, as shown in FIG.
矢印A方向に回転可能な円筒状の導電性基板11が用い
られる。該導電性基板11としては1例えば。A cylindrical conductive substrate 11 rotatable in the direction of arrow A is used. For example, the conductive substrate 11 may be one.
アルミニウム基板が用いられる。該導電性基板11の表
面には1例えば、正極性に帯電された光導電性トナー1
4が均一に付着される。導電性基板11上に付着された
光導電性トナー14は1例えば基板11の頂部にて原稿
像が露光される。露光された光導電性トナー14は、導
電性を得、基板11を通じて正極性の電荷を消失する。An aluminum substrate is used. For example, positively charged photoconductive toner 1 is deposited on the surface of the conductive substrate 11.
4 is uniformly deposited. The photoconductive toner 14 deposited on the conductive substrate 11 is exposed, for example, to the top of the substrate 11 so that the original image is exposed. The exposed photoconductive toner 14 becomes conductive and loses positive charge through the substrate 11.
導電性基板11の、この露光位置より回転方向下流側に
は、該導電性基板11表面に対向して導電性電極12が
配設されている。該導電性電極12は、基板11表面と
は100〜500μm程度の間隙を有している。導電性
電極12と導電性基vi11との間には。On the downstream side of the conductive substrate 11 from this exposure position in the rotational direction, a conductive electrode 12 is disposed facing the surface of the conductive substrate 11 . The conductive electrode 12 has a gap of about 100 to 500 μm from the surface of the substrate 11. between the conductive electrode 12 and the conductive group vi11.
電源13にて印加される電圧により所定の電界が形成さ
れる。導電性基板11上の露光により電荷が消失したト
ナーは、基板11より負電荷を注入され。A predetermined electric field is formed by the voltage applied by the power source 13. The toner whose charge has disappeared due to exposure on the conductive substrate 11 is injected with negative charge from the substrate 11.
負極性となる。基板11上の一方の極性のトナーは。It becomes negative polarity. Toner of one polarity on the substrate 11.
所定の転写装置により転写紙へ静電的に転写される。こ
のとき2例えば、露光されて負極性となったトナーを転
写する場合には、転写紙の背面からプラスコロナ放電が
行われる。これにより、負極性のトナーのみが転写紙上
へ静電的に転写されることになり、基板1工上の正極性
のトナーは転写されるおそれがない。トナーを露光した
後にそのトナーを電界内に位置せしめるようにしている
ため。The image is electrostatically transferred onto a transfer paper by a predetermined transfer device. At this time, for example, when toner that has been exposed to negative polarity is to be transferred, positive corona discharge is performed from the back side of the transfer paper. As a result, only the toner of negative polarity is electrostatically transferred onto the transfer paper, and there is no possibility that the toner of positive polarity on the substrate 1 is transferred. This is because after the toner is exposed to light, the toner is placed within an electric field.
露光されないトナーの電荷が減衰されるタイミングが遅
れ、転写時におけるそのトナーは高帯電量を維持し、露
光されたトナーとの電位差が大きく。The timing at which the charge of the unexposed toner is attenuated is delayed, and the toner maintains a high charge amount during transfer, resulting in a large potential difference with the exposed toner.
従って、得られる画像は高コントラストとなる。Therefore, the resulting image has high contrast.
なお、逆極性の電荷を付与するタイミングは。Furthermore, the timing of applying charges of opposite polarity is as follows.
光導電性トナーの露光が完全に終了しない時点で行うこ
とが望ましい。It is desirable to carry out this process before the exposure of the photoconductive toner is completely completed.
第2図〜第4図は、それぞれ本発明方法の他の実施例を
示す。これらの実施例では、露光されたトナーに、帯電
時の極性とは逆極性の電荷を付与するための電界を、透
明電極により形成する。そして、この透明電極を介して
原稿像を露光する。FIGS. 2 to 4 each show other embodiments of the method of the present invention. In these embodiments, an electric field is formed using a transparent electrode to impart a charge having a polarity opposite to the polarity at the time of charging to the exposed toner. Then, the original image is exposed through this transparent electrode.
第2図に示す実施例では、透明電極15aの導電性基板
11の回転方向上流側部分の透光性がその下流側部分よ
りも高くなっている。簡単には、該透明電極15aの下
流側部分を遮光すればよい。該透明電極15aは基板1
1と100〜500μm程度の間隙をあけて対向して配
設されている。該透明電極15aと基板11との間には
、電源13にて印加される電圧により電界が形成される
。In the embodiment shown in FIG. 2, the upstream portion of the transparent electrode 15a in the rotational direction of the conductive substrate 11 has higher translucency than the downstream portion thereof. Simply, the downstream portion of the transparent electrode 15a may be shielded from light. The transparent electrode 15a is connected to the substrate 1
1 and are disposed facing each other with a gap of about 100 to 500 μm. An electric field is formed between the transparent electrode 15a and the substrate 11 by the voltage applied by the power source 13.
導電性基板11上の正極性に帯電された光導電性トナー
は、透明電極15aの基板11回転方向上流側部分にて
露光されてその電荷を消失し、その下流側部分にて負極
性に帯電される。The positively charged photoconductive toner on the conductive substrate 11 is exposed to light at the upstream portion of the transparent electrode 15a in the rotational direction of the substrate 11 to lose its charge, and is negatively charged at the downstream portion thereof. be done.
゛ 第3図に示す実施例で、一様な透光性を有する透明
電極15bを、導電性基板11の回転方向下流側端部が
、該基板11に接近するように傾斜させたものである。゛ In the embodiment shown in FIG. 3, a transparent electrode 15b having uniform translucency is tilted so that the downstream end in the rotational direction of the conductive substrate 11 approaches the substrate 11. .
該透明電極15bには電源13により電圧が印加され、
基板IIとの間に電界を形成するが。A voltage is applied to the transparent electrode 15b by the power source 13,
An electric field is formed between the substrate II and the substrate II.
上述の如く傾斜しているため、基板11の回転方向下流
側部分の電界強度が大きくなる。従って、基板11上の
正極性のトナーは、透明電極15bの上流側部分にて露
光され、その正極性の電荷を消失された後に、高強度の
電界部分にて負極性とされる。Because of the inclination as described above, the electric field strength at the downstream portion of the substrate 11 in the rotational direction is increased. Therefore, the positive polarity toner on the substrate 11 is exposed to light at the upstream portion of the transparent electrode 15b, and after its positive polarity charge is eliminated, it is made negative polarity in the high intensity electric field portion.
第4図に示す実施例では、第3図に示す透明電極15b
と同様に、一様の透光性を有する透明電極15cを基板
11に対して傾斜させることなく基板11に対向させて
配設し、該透明電極15cの基板11と対向する面に、
基板11の回転方向上流側部分が厚くなった誘電体16
を配設している。該誘電体16は。In the embodiment shown in FIG. 4, the transparent electrode 15b shown in FIG.
Similarly, a transparent electrode 15c having uniform light transmittance is arranged facing the substrate 11 without being inclined with respect to the substrate 11, and on the surface of the transparent electrode 15c facing the substrate 11,
Dielectric material 16 that is thicker on the upstream side in the rotational direction of substrate 11
has been set up. The dielectric 16 is.
厚みが増加するほど誘電率が上昇し、従って、透明電極
15cと基板11との間の電界は、基板11の回転方向
下流側部分がその上流側部分よりも高強度になる。基板
11上の正極性のトナーは、透明電極15cの上流側部
分にて露光され、その電荷が消失された後に、高強度の
電界部分にて負極性とされる。As the thickness increases, the dielectric constant increases, and therefore, the electric field between the transparent electrode 15c and the substrate 11 has a higher intensity on the downstream side in the rotational direction of the substrate 11 than on the upstream side. The positive polarity toner on the substrate 11 is exposed to light at the upstream side of the transparent electrode 15c, and after its charge is eliminated, it is made negative in the high intensity electric field.
ス11」1
第2図に示すようにして複写画像を得た。透明電極15
aは、その透光率が基板11回転方向上流側部分が95
%であり、その下流側部分にかけて順次減少し、該下流
側部分にて0%となっている。該透明電極15bは基板
11の頂部とは、その中心が500μm離れて、基Fi
11の接線方向に延びている。基十反11としてはアル
ミニウム基板を用いた。透明電極15aに2kVの電圧
を印加し、同時に基板11表面で3001uxとなるよ
うに画像露光を行った。この場合、第5図に示すように
、露光強度が最大となる時間T、と電界の強度が最大と
なる時間T2との時間のずれT (=T2 T+ )
は50m5ec、露光終了時間(T4)と電圧印加開始
時間(T□)との時間のずれ仁 (=T4−T:l )
は100m5ecであった。Step 11''1 A copy image was obtained as shown in FIG. Transparent electrode 15
a has a light transmittance of 95 on the upstream side in the rotational direction of the substrate 11.
%, and gradually decreases toward the downstream portion, reaching 0% at the downstream portion. The center of the transparent electrode 15b is 500 μm apart from the top of the substrate 11, and the base Fi
11 in the tangential direction. As the base 11, an aluminum substrate was used. A voltage of 2 kV was applied to the transparent electrode 15a, and at the same time, image exposure was performed on the surface of the substrate 11 at 3001 ux. In this case, as shown in FIG. 5, there is a time difference T (=T2 T+) between the time T when the exposure intensity is maximum and the time T2 when the electric field intensity is maximum.
is 50m5ec, the time difference between the exposure end time (T4) and the voltage application start time (T□) (=T4-T:l)
was 100m5ec.
電圧印加後の基板11上のトナーは1通常の転写装置に
より転写紙に転写して複写画像を得た。該複写画像のコ
ントラスト比(非露光部濃度に対する露光部濃度の割合
を百分率で表したもの)は。After the voltage was applied, the toner on the substrate 11 was transferred onto a transfer paper using an ordinary transfer device to obtain a copy image. The contrast ratio (the ratio of the exposed area density to the unexposed area density expressed as a percentage) of the copied image is:
約16.6であった。It was about 16.6.
去放開又
第3図に示すようにして複写画像を得た。透明電極15
cは、透光率が95%の均一なネサガラスを用い、基板
11の回転方向上流側部分で28%、その下流側部分で
0.5■鳳の間隔となるように傾斜させた。この場合、
露光強度が最大となる時間T1と電界強度が最大となる
時間T2との時間のずれTは150m5ec、露光終了
時間T4と電圧印加開始時間T、との時間のずれtは1
00m5ecであった。その他の条件は実験例1と同様
にして、複写画像を得た。得られた複写画像のコントラ
スト比は27.3であった。A copy image was obtained as shown in FIG. Transparent electrode 15
For c, uniform Nesa glass with a light transmittance of 95% was used, and the substrate 11 was tilted at an interval of 28% on the upstream side in the rotational direction and 0.5 cm on the downstream side. in this case,
The time difference T between the time T1 when the exposure intensity is maximum and the time T2 when the electric field strength is maximum is 150 m5 ec, and the time difference t between the exposure end time T4 and the voltage application start time T is 1.
It was 00m5ec. Copy images were obtained under the same conditions as in Experimental Example 1. The contrast ratio of the obtained copied image was 27.3.
此4石汁上
透光率が95%である均一なネサガラスを用いた透明電
極を、第6図に示すように、基板の頂部から500μm
離隔させて配設し1画像を露光すると同時に電圧を印加
した。露光強度が最大となる時間T1と電界強度が最大
となる時間T2とのずれがなく(T=O)、露光終了時
間T4と電圧印加開始時間T、との時間のずれ仁は10
0m5ecであった。その他の条件は実験例1と同様に
した。得られた複写画像のコントラスト比は4.8であ
った。As shown in Figure 6, a transparent electrode made of uniform Nesa glass with a light transmittance of 95% was placed 500 μm from the top of the substrate.
They were placed at a distance and a voltage was applied at the same time as one image was exposed. There is no difference between the time T1 when the exposure intensity is maximum and the time T2 when the electric field strength is maximum (T=O), and the time difference between the exposure end time T4 and the voltage application start time T is 10
It was 0m5ec. Other conditions were the same as in Experimental Example 1. The contrast ratio of the obtained copied image was 4.8.
止較尉叢
比較例1と同様に透明電極を配設し、露光が終了した時
点で電圧を印加した(1=0)。その他の条件は比較例
1と同様にした。得られた複写画像のコントラスト比は
1以下であった。Transparent electrodes were provided in the same manner as in Comparative Example 1, and a voltage was applied (1=0) when exposure was completed. Other conditions were the same as in Comparative Example 1. The contrast ratio of the obtained copied image was 1 or less.
実験例1および2と、比較例1および比較例2とを表1
に示す。Table 1 shows Experimental Examples 1 and 2, Comparative Example 1, and Comparative Example 2.
Shown below.
表1
(発明の効果)
本発明の画像形成方法は、このように、帯電された光導
電性トナーを露光してその電荷を消失させるタイミング
と、電荷を消失したトナーに帯電時の極性とは逆極性の
電荷を付与するタイミングとを異ならせ、後者のタイミ
ングを前者のタイミングよりも遅らせているため、露光
されないトナーの表面電位の減衰を抑制することができ
、それゆえ、高コントラストな画像が得られる。Table 1 (Effects of the Invention) In the image forming method of the present invention, as described above, the timing at which the charged photoconductive toner is exposed to light to eliminate its charge and the polarity when charging the toner that has lost its charge are determined. Since the timing of applying charges of opposite polarity is different and the latter timing is delayed than the former timing, it is possible to suppress the attenuation of the surface potential of the unexposed toner, and therefore, a high-contrast image can be obtained. can get.
4、 ヌ の パ な量゛ ■
第1図は本発明の画像形成方法の一例を示す模式図、第
2図〜第4図は、それぞれ本発明方法の別の実施例を示
す模式図、第5図は1本発明方法の説明のためのグラフ
、第6図は従来の画像形成方法の一例を示す模式図であ
る。4. Figure 1 is a schematic diagram showing an example of the image forming method of the present invention, and Figures 2 to 4 are schematic diagrams showing another embodiment of the method of the present invention, respectively. FIG. 5 is a graph for explaining the method of the present invention, and FIG. 6 is a schematic diagram showing an example of a conventional image forming method.
11・・・導電性基板、12・・・導電性電極、13・
・・電源。11... Conductive substrate, 12... Conductive electrode, 13.
··power supply.
14・・・光導電性トナー、15a、15b、15c・
・・透明電極。14... Photoconductive toner, 15a, 15b, 15c.
...Transparent electrode.
以上that's all
Claims (1)
させると共に電界内に位置させて電荷を消失した該トナ
ーに帯電時のトナー極性とは逆極性の電荷を付与し、次
いで一方の極性のトナーを転写紙に静電的に転写して画
像を得る画像形成方法であり、 帯電された光導電性トナーを露光するタイミングと、電
荷を消失したトナーに帯電時のトナー極性とは逆極性の
電荷を付与するタイミングとを異ならせた画像形成方法
。 2、前記逆極性の電荷を付与するタイミングは、前記光
導電性トナーの露光が完全に終了しない時点で開始され
る特許請求の範囲第1項に記載の画像形成方法。 3、前記光導電性トナーは移動可能な導電性の基板上に
付着され、その基板の移動に伴って該トナーが露光され
る特許請求の範囲第1項に記載の画像形成方法。 4、前記電界は前記基板と対向して配設された導電性電
極により形成され、該導電性電極は前記基板の露光位置
よりもその移動方向下流側に位置する特許請求の範囲第
3項に記載の画像形成方法。 5、前記電界は前記基板と対向して配設された透明電極
にて形成され、該透明電極を介して該基板上の前記光導
電性トナーが露光される特許請求の範囲第3項に記載の
画像形成方法。 6、前記透明電極の透光性が、前記基板の移動方向下流
側部分よりもその上流側部分の方が高くなっている特許
請求の範囲第5項に記載の画像形成方法。 7、前記透明電極の電界強度が、前記基板の移動方向下
流側部分がその上流側部分よりも大である特許請求の範
囲第5項に記載の画像形成方法。 8、前記透明電極は、前記基板の移動方向下流側端部が
該基板に接近するように傾斜している特許請求の範囲第
7項に記載の画像形成方法。 9、前記透明電極の前記基板と対向する面に、該基板の
移動方向上流側部分の誘電率を上昇させる誘電体が配設
されている特許請求の範囲第7項に記載の画像形成方法
。[Scope of Claims] 1. Charged photoconductive toner is exposed to light to eliminate its charge, and the toner is placed in an electric field to eliminate its charge, and a charge with a polarity opposite to the toner polarity at the time of charging is imparted to the toner. This is an image forming method in which the toner of one polarity is then electrostatically transferred to a transfer paper to form an image. An image forming method that differs in the timing of applying charges of opposite polarity to the toner polarity. 2. The image forming method according to claim 1, wherein the timing of applying the charges of opposite polarity is started at a time point when exposure of the photoconductive toner is not completely completed. 3. The image forming method according to claim 1, wherein the photoconductive toner is deposited on a movable conductive substrate, and the toner is exposed to light as the substrate moves. 4. The electric field is formed by a conductive electrode disposed opposite to the substrate, and the conductive electrode is located downstream of the exposure position of the substrate in the direction of movement thereof. The image forming method described. 5. According to claim 3, the electric field is formed by a transparent electrode disposed opposite to the substrate, and the photoconductive toner on the substrate is exposed through the transparent electrode. image forming method. 6. The image forming method according to claim 5, wherein the transparency of the transparent electrode is higher in an upstream portion of the substrate than in a downstream portion in the moving direction of the substrate. 7. The image forming method according to claim 5, wherein the electric field strength of the transparent electrode is greater in a downstream portion in the moving direction of the substrate than in an upstream portion. 8. The image forming method according to claim 7, wherein the transparent electrode is inclined such that the downstream end in the moving direction of the substrate approaches the substrate. 9. The image forming method according to claim 7, wherein a dielectric material that increases the dielectric constant of an upstream portion of the substrate in the moving direction is provided on a surface of the transparent electrode facing the substrate.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15367186A JPH0664378B2 (en) | 1986-06-30 | 1986-06-30 | Image forming method |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP15367186A JPH0664378B2 (en) | 1986-06-30 | 1986-06-30 | Image forming method |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS638757A true JPS638757A (en) | 1988-01-14 |
JPH0664378B2 JPH0664378B2 (en) | 1994-08-22 |
Family
ID=15567627
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP15367186A Expired - Lifetime JPH0664378B2 (en) | 1986-06-30 | 1986-06-30 | Image forming method |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0664378B2 (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012058321A (en) * | 2010-09-06 | 2012-03-22 | Fuji Xerox Co Ltd | Image forming apparatus |
-
1986
- 1986-06-30 JP JP15367186A patent/JPH0664378B2/en not_active Expired - Lifetime
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2012058321A (en) * | 2010-09-06 | 2012-03-22 | Fuji Xerox Co Ltd | Image forming apparatus |
Also Published As
Publication number | Publication date |
---|---|
JPH0664378B2 (en) | 1994-08-22 |
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