Title:
Image forming method and apparatus
Document Type and Number:
Kind Code:
A1

Abstract:
In an image forming system, an image-bearing member having a photoconductor layer comprising an Si-based non-single crystal material is charged at a relatively low potential of 250 to 600 volts by a contact charging member in the presence of electroconductive fine powder. An electrostatic latent image formed on the image-bearing member is developed with a magnetic toner which includes magnetic toner particles comprising at least a binder resin and a magnetic iron oxide, and inorganic fine powder and electroconductive fine powder present at the surface of the magnetic toner particles. The magnetic toner has a weight-average particle size of 3-10 μm and an average circularity of 0.950 to 0.995, and contains 0.05 to 3.00 % of isolated iron-containing particles.
Inventors:
Komoto, Keiji (Numazu-shi, JP)
Takiguchi, Tsuyoshi (Suntoh-gun, JP)
Chiba, Tatsuhiko (Kamakura-shi, JP)
Magome, Michihisa (Shizuoka-ken, JP)
Hashimoto, Akira (Shizuoka-ken, JP)
Kaburagi, Takeshi (Susono-shi, JP)
      Plaque It!

Sponsored by:
Flash of Genius
Application Number:
09/987490
Publication Date:
08/22/2002
Filing Date:
11/15/2001
View Patent Images:
Images are available in PDF form when logged in. To view PDFs, Login  or  Create Account (Free!)
Primary Class:
Other Classes:
430/106.100, 430/108.600, 430/125.300, 430/110.300, 430/122.520
International Classes:
(IPC1-7): G03G013/14
Attorney, Agent or Firm:
FITZPATRICK CELLA HARPER & SCINTO (30 ROCKEFELLER PLAZA, NEW YORK, NY, 10112, US)
Claims:

What is claimed is:



1. An image forming method, comprising: a charging step of charging an image-bearing member by charging means comprising a charging member supplied with a voltage and abutted against the image-bearing member at a contact position; a latent-image forming step of forming an electrostatic latent image on the charged image-bearing member, a developing step of transferring a magnetic toner carried on a toner-carrying member onto the electrostatic latent image to develop the latent image, thereby forming a magnetic toner image on the image-bearing member, and a transfer step of electrostatically transferring the magnetic toner image on the image-baring member onto a transfer material via or without via an intermediate transfer member, wherein the image-bearing member comprises an electroconductive support and a photoconductor layer comprising a silicon-based non-single crystal material and disposed on the electroconductive support, and is charged to a potential of 250 to 600 volts in terms of an absolute value via the charging member abutted against it, the magnetic toner includes magnetic toner particles comprising at least a binder resin and a magnetic iron oxide, and inorganic fine powder and electroconductive fine powder present at the surface of the magnetic toner particles, the magnetic toner has a weight-average particle size of 3-10 μm, the magnetic toner has an average circularity of 0.950 to 0.995, and the magnetic toner contains 0.05 to 3.00% of isolated iron-containing particles.

2. The method according to claim 1, wherein in the charging step, electroconductive fine powder is present between the charging means and the image-bearing member.

3. The method according to claim 1, wherein in the charging step, the image-bearing member is charged to a potential of 250 to 550 volts in terms of an absolute value.

4. The method according to claim 1, wherein in the charging step, the image-bearing member is charged to a potential of 250 to 500 volts in terms of an absolute value.

5. The method according to claim 1, wherein the magnetic toner has a magnetization of 10-50 Am2/kg at a magnetic field of 79.6 kA/m.

6. The method according to claim 1, wherein the magnetic toner contains 0.05-2.00% of isolated iron-containing particles.

7. The method according to claim 1, wherein the magnetic toner contains 0.05-1.50% of isolated iron-containing particles.

8. The method according to claim 1, wherein the magnetic toner contains 0.05-0.80% of isolated iron-containing particles.

9. The method according to claim 1, wherein the magnetic toner has an average circularity of 0.970 to 0.995.

10. The method according to claim 1, wherein the magnetic toner has a mode circularity of at least 0.990.

11. The method according to claim 1, wherein the magnetic iron oxide in the magnetic toner has been surface-treated in an aqueous medium with a coupling agent hydrolyzed in the medium.

12. The method according to claim 1, wherein the inorganic fine powder blended with the magnetic toner particles in the magnetic toner has an average primary particle size of 4-80 nm.

13. The method according to claim 12, wherein the inorganic fine powder comprises at least one member selected from the group consisting of silica, titanium oxide alumina and double oxides of these.

14. The method according to claim 1, wherein the inorganic fine powder has been hydrophobized.

15. The method according to claim 14, wherein the inorganic fine powder has been treated with at least silicone oil.

16. The method according to claim 14, wherein the inorganic fine powder has been treated with at least a silane compound and silicone oil.

17. The method according to claim 1, wherein the electroconductive fine powder is non-magnetic.

18. The method according to claim 17, wherein the magnetic toner has a resistivity of at most 109 ohm.cm, and the electroconductive fine powder has a volume-average particle size smaller than that of the magnetic toner and is contained in a proportion of 0.2-10 wt. % of the magnetic toner.

19. The method according to claim 17, wherein the non-magnetic electroconductive fine powder has a resistivity of at most 106 ohm.cm.

20. The method according to claim 17, wherein at least a surface portion of the non-magnetic electroconductive fine powder comprises a metal oxide which contains a principal metal element and also an element different from the principal metal element in a proportion of 0.1-5 atom. % of the principal metal element, or a metal oxide in an oxygen-deficient state.

21. The method according to claim 1, wherein the magnetic toner contains a wax in a proportion of 0.1-20 wt. % of the magnetic toner.

22. The method according to claim 1, wherein the wax has a maximum heat-absorption peak temperature of 40-110° C. as measured by differential scanning calorimetry.

23. The method according to claim 1, wherein the wax has a maximum heat-absorption peak temperature of 45-90° C. as measured by differential scanning calorimetry.

24. The method according to claim 1, wherein the electroconductive support of the image-bearing member has a cylindrical shape, and the image-bearing member is free from a heater therefor inside the cylindrical support.

25. The method according to claim 1, wherein the image-bearing member has a laminate structure including an electroconductive support, a photoconductor layer comprising a silicon-based non-single crystal material and a surfacemost layer comprising a non-single crystal material different from that of the photoconductor layer.

26. The method according to claim 25, wherein the surfacemost layer comprises a non-single crystal carbon hydride film.

27. The method according to claim 1, wherein the developing step is operated to also function as a step of recovering a portion of the magnetic toner remaining on the image-bearing member after the transfer step of transferring the toner image onto the transfer material.

28. The method according to claim 1, wherein in the charging step, the image-baring member is charged by the charging member in the presence of electroconductive fine powder present in a density of at most 103 particles/mm2 at the contact position.

29. The method according to claim 1, wherein in the charging step, the image-bearing member is charged while moving the image-baring member and the charging member so as to provide a relative speed difference between surface moving speeds of these members at the contact position.

30. The method according to claim 29, wherein in the charging step, the image-bearing member and the charging member are moved in mutually opposite surface moving directions at the contact position.

31. The method according to claim 1, wherein in the charging step, the charging member is a roller member having an Asker C hardness of at most 50 deg.

32. The method according to claim 1, wherein in the charging step, the charging member is a roller member having a volume-resistivity of 103-108 ohm. cm.

33. The method according to claim 1, wherein in the charging step, the charging member is a roller member having a surface provided with minute cells providing an average spherical cell diameter of 5-300 μm and a void areal percentage at the surface of 15-90%.

34. The method according to claim 1, wherein in the charging step, the charging member is an electroconductive brush member.

35. The method according to claim 1, wherein in the charging step, the charging member is supplied with a DC voltage alone or in superposition with an AC voltage having a peak-to-peak voltage of below 2×Vth relative to a discharge initiation voltage Vth in DC voltage application.

36. The method according to claim 1, wherein in the charging step, the charging member is supplied with a DC voltage alone or in superposition with an AC voltage having a peak-to-peak voltage of below Vth relative to a discharge initiation voltage Vth in DC voltage application.

37. The method according to claim 1, wherein the charging member comprises magnetic particles.

38. The method according to claim 1, wherein in the charging step, the charging member comprises a magnetic brush formed of magnetically constrained magnetic particles and is supplied with a voltage while contacting the image-bearing member to charge the image-bearing member.

39. The method according to claim 38, wherein the magnetic particles have a volume-basis median diameter of 10-50 μm.

40. The method according to claim 38, wherein the magnetic particles have a volume resistivity of 1×104-1×109 ohm.cm.

41. The method according to claim 1, wherein the electrostatic latent image is a digital latent image.

42. The method according to claim 1, wherein in the developing step, the magnetic toner is carried in a layer at a density of 5-50 g/m2 on the toner-carrying member to develop the electrostatic latent image on the image-bearing member.

43. The method according to claim 1, wherein in the developing step, the magnetic toner is carried on the toner-carrying member in an amount regulated by a ferromagnetic metal blade disposed opposite to and with a small gap from the toner-carrying member.

44. The method according to claim 1, wherein in the developing step, the toner-carrying member is disposed opposite to and with a gap of 100-1000 μm from the image-bearing member.

45. The method according to claim 1, wherein in the developing step, the magnetic toner is disposed on the toner-carrying member in a layer thickness smaller than a gap between the toner-carrying member and the image-bearing member, and is transferred onto the image-bearing member to develop the electrostatic latent image thereon.

46. The method according to claim 1, wherein in the developing step, a developing bias voltage comprising at least an AC voltage is applied so as to form an alternating electric field between the toner-carrying member and the image-bearing member, wherein the alternating electric field has a peak-to-peak intensity of 3×106-1×107 V/m and a frequency of 100-5000 Hz.

47. The method according to claim 1, wherein in the transfer step, a transfer member is abutted against the image-bearing member via the transfer material to transfer the toner image from the image-baring member onto the transfer material.

48. An image forming apparatus, comprising: an image-bearing member, a charging means for charging the image-bearing member, an electrostatic latent-image forming means forming an electrostatic latent image on the charged image-bearing member, a developing means including a toner-carrying member for transferring a magnetic toner carried on the toner-carrying member onto the electrostatic latent image to form a toner image thereon, and a transfer means for electrostatically transferring the toner image on the image-bearing member onto a transfer material via or without via an intermediate transfer member, wherein the charging means comprises a charging member supplied with a voltage and abutted against the image-bearing member to form a contact nip with the image-bearing member, the image-bearing member comprises an electroconductive support and a photoconductor layer comprising a silicon-based non-single crystal material and disposed on the electroconductive support, and is charged to a potential of 250 to 600 volts in terms of an absolute value via the charging member abutted against it, the magnetic toner includes magnetic toner particles comprising at least a binder resin and a magnetic iron oxide, and inorganic fine powder and electroconductive fine powder present at the surface of the magnetic toner particles, the magnetic toner has a weight-average particle size of 3-10 μm, the magnetic toner has an average circularity of 0.950 to 0.995, and the magnetic toner contains 0.05 to 3.00% of isolated iron-containing particles.

49. The apparatus according to claim 48, wherein the developing means also functions as a means for recovering a portion of the magnetic toner remaining on the image-bearing member after transferring the toner image onto the transfer material.

50. The apparatus according to claim 48, wherein in the charging means, the image-bearing member is charged to a potential of 250 to 550 volts in terms of an absolute value.

51. The apparatus according to claim 48, wherein in the charging means, the image-bearing member is charged to a potential of 250 to 500 volts in terms of an absolute value.

52. The apparatus according to claim 48, wherein the image-bearing member is free from a means for warming it.

53. The apparatus according to claim 48, wherein the image-bearing member has a laminate structure including an electroconductive support, a photoconductor layer comprising a silicon-based non-single crystal material and a surfacemost layer comprising a non-single crystal material different from that of the photoconductor layer.

54. The apparatus according to claim 48, wherein the surfacemost layer comprises a non-single crystal carbon hydride film.

55. The apparatus according to claim 48, wherein the charging means is a means for charging the image-bearing member by abutting the charging member against the image-bearing member via electroconductive fine powder.

56. The apparatus according to claim 55, wherein the electroconductive fine powder is present at a density of at least 103 particles/mm2.

57. The apparatus according to claim 48, wherein the image-bearing member is charged while moving the image-baring member and the charging member so as to provide a relative speed difference between surface moving speeds of these members at the contact position.

58. The apparatus according to claim 57, wherein the image-bearing member and the charging member are moved in mutually opposite surface moving directions at the contact position.

59. The apparatus according to claim 48, wherein the charging member is a roller member having an Asker C hardness of at most 50 deg.

60. The apparatus according to claim 48, wherein the charging member is a roller member having a volume-resistivity of 103-108 ohm.cm.

61. The apparatus according to claim 48, wherein the charging member is a roller member having a surface provided with minute cells providing an average spherical cell diameter of 5-300 μm and a void real percentage at the surface of 15-90%.

62. The apparatus according to claim 48, wherein the charging member is an electroconductive brush member supplied with a voltage to charge the image-bearing member.

63. The apparatus according to claim 48, wherein the charging member is supplied with a DC voltage alone or in superposition with an AC voltage having a peak-to-peak voltage of below 2×Vth relative to a discharge initiation voltage Vth in DC voltage application.

64. The apparatus according to claim 48, wherein the charging member is supplied with a DC voltage alone or in superposition with an AC voltage having a peak-to-peak voltage of below Vth relative to a discharge initiation voltage Vth in DC voltage application.

65. The apparatus according to claim 48, wherein the charging member comprises a magnetic brush formed of magnetically constrained magnetic particles and is supplied with a voltage while contacting the image-bearing member to charge the image-bearing member.

66. The apparatus according to claim 65, wherein the magnetic particles have a volume-basis median diameter of 10-50 μm.

67. The apparatus according to claim 65, wherein the magnetic particles have a volume resistivity of 1×104-1×109 ohm.cm.

68. The apparatus according to claim 481, wherein in the developing means, the magnetic toner is carried in a layer at a density of 5-50 g/m2 on the toner-carrying member to develop the electrostatic latent image on the image-bearing member.

69. The apparatus according to claim 48, wherein in the developing means, the magnetic toner is carried on the toner-carrying member in an amount regulated by a ferromagnetic metal blade disposed opposite to and with a small gap from the toner-carrying member.

70. The apparatus according to claim 48, wherein in the developing means, the toner-carrying member is disposed opposite to and with a gap of 100-1000 μm from the image-bearing member.

71. The apparatus according to claim 48, wherein in the developing means, the magnetic toner is disposed on the toner-carrying member in a layer thickness smaller than a gap between the toner-carrying member and the image-bearing member, and is transferred onto the image-bearing member to develop the electrostatic latent image thereon.

72. The apparatus according to claim 48, wherein in the developing means, a developing bias voltage comprising at least an AC voltage is applied so as to form an alternating electric field between the toner-carrying member and the image-bearing member, wherein the alternating electric field has a peak-to-peak intensity of 3×10 6-1×107 V/m and a frequency of 100-5000 Hz.

73. The apparatus according to claim 48, wherein the transfer means includes a transfer member abutted against the image-bearing member via the transfer material to transfer the toner image from the image-baring member onto the transfer material.

Description:

FIELD OF THE INVENTION AND RELATED ART

[0001] The present invention relates to an image forming method and an image forming apparatus using a magnetic toner according to a recording method, such as electrophotography and electrostatic recording.

[0002] Hitherto, various proposals have been made regarding image forming methods using a magnetic toner.

[0003] U.S. Pat. No. 3,908,258 has proposed a developing method using an electroconductive magnetic toner, wherein an electroconductive magnetic toner is carried on an electroconductive sleeve containing a magnet therein and caused to contact an electrostatic image to effect the development. In this instance, in the developing region, an electroconductive path is formed of toner particles between an image-bearing member surface and the sleeve surface, and a charge is guided from the sleeve to the toner particles via the electroconductive path, whereby the resultant Coulomb force acting between the toner particles and the electrostatic images causes the toner particles to attach the electrostatic image to effect a development thereof. The developing method using an electroconductive magnetic toner is an excellent method capable of obviating problems involved in a conventional two-component developing method but, on the other hand, involves a difficulty in electrostatic transfer of the developed toner image from the image-bearing member to a recording material, such as plain paper because of the electroconductivity of the toner.

[0004] As a developing method using a high-resistivity magnetic toner which can be electrostatically transferred, there is a developing method utilizing dielectric polarization of toner particles. This method however involves an inherently slow developing speed and an insufficient developed image density.

[0005] As another developing method of using a high-resistivity magnetic toner, there is known a method wherein the magnetic toner particles are triboelectrically charged through friction between individual toner particles and between the toner particles and the developing sleeve and then caused to contact an electrostatic image on the image-bearing member to effect the development. This method involves a difficulty that insufficient triboelectric charge or charging failure is liable to occur due to a relatively low frequency of contact between the magnetic toner particles and the friction member and also due to exposure of the magnetic material at the magnetic toner particle surface.

[0006] JP-A 55−18656 has proposed a jumping developing method, wherein a thin layer of magnetic toner is applied and triboelectrically charged on a developing sleeve and is then brought to a proximity to an electrostatic image to develop the electrostatic image. This method is an excellent method in that it allows a sufficient triboelectrification by the application of a magnetic toner in a thin layer on a developing sleeve to increase the opportunity of contact between the developing sleeve and the toner.

[0007] However, such insulating magnetic toner particles are accompanied with a substantial amount of fine magnetic powder and also a portion of the magnetic powder exposed at the magnetic toner particle surface, which are liable to affect the flowability and triboelectric chargeability of the magnetic toner.

[0008] In the case of using a conventional magnetic toner containing magnetic powder, the magnetic powder exposed at the magnetic toner particle surface is considered to affect the toner performances. More specifically, due to the exposure at the magnetic toner particle surface of fine magnetic powder having a lower resistivity than a resin constituting the magnetic toner particles, the magnetic toner particles are liable to cause a lowering in chargeability, a lowering in flowability and separation of the magnetic powder due to friction or rubbing between individual magnetic toner particles and between the toner particles and a regulation member during a long term of uses, thus being liable to cause an image density lowering and image density irregularity called sleeve ghost.

[0009] A toner obtained through suspension polymerization (sometimes referred to as a “polymerization toner”) is advantageous for high-quality image formation because of easiness of smaller particle size toner production and an improved flowability due to a sphericity of resultant toner particle shape.

[0010] The flowability and chargeability of polymerization toner particles are however lowered due to inclusion therein of magnetic powder (generally comprising a magnetic iron oxide). This is because magnetic powder is generally hydrophillic to be predominantly present at the toner particle surface, so that a surface property modification of the magnetic powder becomes important for solving the problem.

[0011] As for surface treatment of magnetic powder for improved dispersion thereof in a polymerization toner, many proposals have been made. For example, JP-A 59−200254, JP-A 59−200256, JP-A 59−200257 and JP-A 59−224102 have proposed treatment of magnetic powder with various silane coupling agents, and JP-A 63-250660 and JP-A 10−239897 have disclosed treatment of silicon-containing magnetic powder with silane coupling agents.

[0012] These treatments provide a somewhat improved dispersibility in the toner but are accompanied with a problem that it is difficult to uniformly hydrophobize magnetic powder surfaces, so that it is difficult to obviate the coalescence of magnetic powder particles and the occurrence of untreated magnetic powder particles, thus leaving a room for further improvement in dispersibility of magnetic powder in the toner particles.

[0013] Further, as a result of such a surface treatment, the exposure of magnetic iron oxide powder from the magnetic toner particle surfaces can be suppressed to some extent, but it is difficult to uniformly hydrophobize the magnetic iron oxide powder surface, so that the occurrence of coalescent magnetic iron oxide powder particles and yet-unhydrophobized magnetic iron oxide powder particles is inevitable, and the suppression of the surface exposure of magnetic iron oxide powder becomes insufficient.

[0014] Further, JP-B 60−3181 has proposed a magnetic toner containing a magnetic iron oxide hydrophobized by treatment with an alkyltrialkoxysilane. The use of the thus-treated magnetic iron oxide powder has actually provided a toner having improved electrophotographic performances in various respects. However, the magnetic iron oxide powder inherently has a relatively low surface activity so that coalescence of magnetic powder particles and insufficient hydrophobization are inevitable, thus leaving the necessity of further improvement for use in an image forming method operated under a severe condition as by inclusion of a contact charging step discussed hereinafter. The use of a larger amount of hydrophobizing agent or a hydrophobizing agent having a higher viscosity provides a higher hydrophobicity of the treated magnetic powder but also results in increased coalescence of magnetic powder particles, thus resulting in a rather inferior dispersibility. As a result, a toner produced by using such a treated magnetic iron oxide powder is caused to have non-uniform triboelectric chargeability, leading to inferior fog prevention and transferability.

[0015] As described above, a conventional polymerization toner using such a surface-treated magnetic powder has not succeeded in a good combination of hydrophobicity and dispersibility, and it is difficult to stably obtain high-definition images if such a polymerization toner is used in an image forming method including a contact charging step as described hereinafter.

[0016] JP-A 5−66608 and JP-A 4−9860 have disclosed hydrophobized inorganic fine powder or inorganic fine powder hydrophobized and then treated with silicone oil. Further, JP-A 61−249059, JP-A 4−264453 and JP-A 5−346682 have disclosed to add hydrophobized inorganic fine powder and silicone oil-treated inorganic fine powder in combination.

[0017] Further, many proposals have been made regarding addition of electroconductive fine powder as an external additive. For example, carbon black as electroconductive fine powder is widely known as an external additive to be attached to or fixed on toner particles for the purpose of, e.g., imparting electroconductivity to the toner, or suppressing excessive charge of the toner to provide a uniform triboelectric charge distribution. Further, JP-A 57-151952, JP-A 59−168458 and JP-A 60−69660 have disclosed to externally add electroconductive fine powder of tin oxide, zinc oxide and titanium oxide, respectively, to high-resistivity toner particles. JP-A 56−142540 has proposed a toner provided with both developing performance and transferability by adding electroconductive magnetic particles, such as iron oxide, iron powder or ferrite, to high-resistivity magnetic toner particles so as to promote charge induction to the magnetic toner. Further, JP-A 61-275864, JP-A 62−258472, JP-A 61−141452 and JP-A 02-120865 have disclosed the addition of graphite, magnetite, polypyrrole electroconductive fine powder and polyaniline electroconductive fine powder to the respective toners. Further, the addition of various species of electroconductive fine powder to the toner is known.

[0018] In recent years, a contact charging device has been proposed and commercialized as a charging device for a member to be charged such as a latent image-bearing member because of advantages, such as low ozone-generating characteristic and a lower power consumption, than the corona charging device.

[0019] A contact charging device is a device comprising an electroconductive charging member (which may also be called a contact charging member or a contact charger) in the form of a roller (charging roller), a fur brush, a magnetic brush or a blade, disposed in contact with a member-to-be-charged, such as an image-bearing member, so that the contact charging member is supplied with a prescribed charging bias voltage to charge the member-to-be-charged to prescribed polarity and potential.

[0020] The charging mechanism (or principle) during the contact charging may include (1) discharge (charging) mechanism and (2) direct injection charging mechanism, and may be classified depending on which of these mechanism is predominant.

[0021] (1) Discharge Charging Mechanism

[0022] This is a mechanism wherein a member is charged by a discharge phenomenon occurring at a minute gap between the member and a contact charging member. As a certain discharge threshold is present, it is necessary to apply to the contact charging member a voltage which is larger than a prescribed potential to be provided to the member-to-be-charged. Some discharge product occurs wile the amount thereof is remarkably less than in a corona charger, and active ions, such as ozone, occur though the amount thereof is small.

[0023] (2) Direct Injection Charging Mechanism

[0024] This is a mechanism wherein a member surface is charged with a charge which is directly injected into the member from a contact charging member. This mechanism may also be called direct charging, injection charging or charge-injection charging. More specifically, a charging member of a medium resistivity is caused to contact a member-to-be-charged to directly inject charges to the member-to-be-charged basically without relying on a discharge phenomenon. Accordingly, a member can be charged to a potential corresponding to an applied voltage to the charging member even if the applied voltage is below a discharge threshold. This mechanism is not accompanied with occurrence of active ions, such as ozone, so that difficulties caused by discharge products can be obviated. However, based on the direct injection charging mechanism, the charging performance is affected by the contactivity of the contact charging member onto the member-to-be-charged. Accordingly, it is preferred that the charging member is provided with a more frequent contact and more dense points of contact with the member-to-be-charged.

[0025] As a contact charging device, a roller charging scheme using an electroconductive roller as a contact charging member is preferred because of the stability of charging performance and is widely used. During the contact charging according to the conventional roller charging scheme, the above-mentioned discharge charging mechanism (1) is predominant. A charging roller has been formed of a conductive or medium-resistivity rubber or foam material optionally disposed in lamination to provide desired characteristics.

[0026] Such a charging roller is provided with elasticity so as to ensure a certain contact with a member-to-be-charged, thus causing a large frictional resistance. The charging roller is moved following the movement of the member-to-be-charged or with a small speed difference with the latter. Accordingly, even if the direct injection charging is intended, the lowering in charging performance, and charging irregularities due to insufficient contact, contact irregularity due to the roller shape and attachment onto the member-to-be-charged, are liable to be caused.

[0027] FIG. 1 is a graph illustrating examples of charging efficiencies for charging photosensitive members by several contact charging members. The abscissa represents a bias voltage applied to the contact charging member, and the ordinate represents a resultant charged potential provided to the photosensitive member. The charging performance in the case of roller charging is represented by a line A. Thus, the surface potential of the photosensitive member starts to increase at an applied voltage exceeding a discharge threshold of ca. −500 volts. Accordingly, in order to charge the photosensitive member to a charged potential of −500 volts, for example, it is a general practice to apply a DC voltage of −1000 volts, or a DC voltage of −500 volts in superposition of an AC voltage at a peak-to-peak voltage of, e.g., 1200 volts, so as to keep a potential difference exceeding the discharge threshold, thereby causing the charged photosensitive member potential to be converged to a prescribed charged potential.

[0028] To describe based on a specific example, in a case where a charging roller is abutted against an OPC photosensitive member having a 25 μm-thick photosensitive layer, the surface potential of the photosensitive member starts to increase in response to an applied voltage of ca. 640 volts or higher and thereafter increases linearly at a slope of 1. The threshold voltage may be defined as a discharge inclination voltage Vth.

[0029] Thus, in order to obtain a photosensitive member surface potential Vd required for electrophotography, it is necessary to apply a DC voltage of Vd+Vth exceeding the required potential to the charging roller. Such a charging scheme of applying only a DC voltage to a contact charging member may be termed a “DC charging scheme”.

[0030] In the DC charging scheme, however, it has been difficult to charge the photosensitive member to a desired potential, since the resistivity of the contact charging member is liable to change in response to a change in environmental condition, and because of a change in Vth due to a surface layer thickness change caused by abrasion of the photosensitive member.

[0031] For this reason, in order to achieve a more uniform charging, it has been proposed to adopt an “AC charging scheme” wherein a voltage formed by superposing a DC voltage corresponding to a desired Vd with an AC voltage having a peak-to-peak voltage in excess of 2×Vth is applied to a contact charging member as described in JP-A 63−149669. According to this scheme, the charged potential of the photosensitive member is converged to Vd which is a central value of the superposed AC voltage due to the potential smoothing effect of the AC voltage, whereby the charged potential is not affected by the environmental change.

[0032] In the above-described contact charging scheme, the charging mechanism essentially relies on discharge from the contact charging member to the photosensitive member, so that a voltage exceeding a desired photosensitive member surface potential has to be applied to the contact charging member and a small amount of ozone is generated.

[0033] Further, in the AC-charging scheme for uniform charging, ozone generation is liable to be promoted, a vibration noise (AC charging noise) between the contact charging member and the photosensitive member due to AC voltage electric field is liable to caused, and the photosensitive member surface is liable to be deteriorated due to the discharge, thus posing a new problem.

[0034] Fur brush charging is a charging scheme, wherein a member (fur brush charger) comprising a brush of electroconductive fiber is used as a contact charging member, and the conductive fiber brush in contact with the photosensitive member is supplied with a prescribed charging bias voltage to charge the photosensitive member surface to prescribed polarity and potential. In the fur brush charging scheme, the above-mentioned discharge charging mechanism (1) may be predominant.

[0035] As the fur brush chargers, a fixed-type charger and a roller-type charger have been commercialized. The fixed-type charger is formed by bonding a pile of medium-resistivity fiber planted to or woven together with a substrate to an electrode. The roller-type charger is formed by winding such a pile about a core metal. A fiber density of ca. 100/mm 2 can be relatively easily obtained, but even at such a high fiber density, the contact characteristic is insufficient for realizing sufficiently uniform charging according to the direct injection charging. In order to effect a sufficiently uniform charging according to the direct injection charging, it is necessary to provide a large speed difference between the fur brush charger and the photosensitive member.

[0036] An example of the charging performance according to the fur brush charging scheme under DC voltage application is represented by a line B in FIG. 1 . Accordingly, in the cases of fur brush charging using any of the fixed-type charger and the roller-type charger, a high charging bias voltage is applied to cause a discharge phenomenon to effect the charging.

[0037] In contrast to the above-mentioned charging schemes, in a magnetic brush scheme, a charging member (magnet brush charger) obtained by constraining electroconductive magnetic particles in the form of a magnetic brush under a magnetic field exerted by a magnet roll is used as a contact charging member, and the magnetic brush in contact with a photosensitive member is supplied with a prescribed charging bias voltage to charge the photosensitive member surface to prescribed polarity and potential. In the magnetic brush charging scheme, the above-mentioned direct injection charging scheme (2) is predominant.

[0038] Uniform direct injection charging becomes possible, e.g., by using magnetic particles of 5−50 μm in particle size and providing a sufficient speed difference with the photosensitive member. An example of the charging performance according to the magnetic brush scheme under DC voltage application is represented by a line C in FIG. 1 , thus allowing a charged potential almost proportional to the applied bias voltage.

[0039] The magnetic brush charging scheme is however accompanied with difficulties that the device structure is liable to be complicated, and the magnetic particles constituting the magnetic brush are liable to be liberated from the magnetic brush to be attached to the photosensitive member.

[0040] Now, the application of such a contact charging scheme to a development and simultaneous cleaning method or a cleanerless image forming method, is considered.

[0041] The development and simultaneous cleaning method or the cleanerless image forming method does not use a cleaning member, so that the transfer residual toner particles remaining on the photosensitive member are caused to contact the contact charging system wherein the discharge charging mechanism is predominant. If an insulating toner is attached to or mixed into the contact charging member, the charging performance of the charging member is liable to be lowered.

[0042] In the charging scheme wherein the discharge charging mechanism is predominant, the lowering in charging performance is caused remarkably from a time when the toner layer attached to the contact charging member surface provides a level of resistance obstructing a discharge voltage. On the other hand, in the charging scheme wherein the direct injection charging mechanism is predominant, the lowering in charging performance is caused as a lowering in chargeability of the member-to-be-charged due to a lowering in opportunity of contact between the contact charging member surface and the member-to-be-charged due to the attachment or mixing of the transfer residual toner particles into the contact charging member.

[0043] The lowering in uniform chargeability of the photosensitive member (member-to-be-charged) results in a lowering in contrast and uniformity of latent image after imagewise exposure, and a lowering in image density and increased fog in the resultant images. Further, in the development and simultaneous cleaning method or the cleanerless image forming method, it is important to control the charging polarity and charge of the transfer residual toner particles on the photosensitive member and stably recover the transfer residual toner particles in the developing step, thereby preventing the recovered toner from obstructing the developing performance. For this purpose, the control of the charging polarity and the charge of the transfer residual toner particles are effected by the charging member.

[0044] This is more specifically described with respect to an ordinary laser beam printer as an example. In the case of a reversal development system using a charging member supplied with a negative voltage, a photosensitive member having a negative chargeability and a negatively charged toner, the toner image is transferred onto a recording medium in the transfer step by means of a transfer member applying a positive voltage. In this case, the transfer residual toner particles are caused to have various charges ranging from a positive polarity to a negative polarity depending on the properties (thickness, resistivity, dielectric constant, etc.) of the recording medium and the image area thereon.

[0045] However, even if the transfer residual toner is caused to have a positive charge in the transfer step, the charge thereof can be uniformized to a negative polarity by the negatively charged charging member for negatively charging the photosensitive member. As a result, in the case of a reversal development scheme, the negatively charged residual toner particles are allowed to remain on the light-part potential where the toner is to be attached, and some irregularly charged toner attached to the dark-part potential is attracted to the toner carrying member due to a developing electric field relationship during the reversal development so that the transfer residual toner at the dark-part potential is not allowed to remain thereat but can be recovered. Thus, by controlling the charging polarity of the transfer residual toner simultaneously with charging of the photosensitive member by means of the charging member, the development and simultaneous cleaning or cleanerless image forming method can be realized.

[0046] However, if the transfer residual toner particles are attached to or mixed to the contact charging member in an amount exceeding the toner charge polarity-controlling capacity of the contact charging member, the charging polarity of the transfer residual toner particles cannot be uniformized so that it becomes difficult to recover the toner particles in the developing step. Further, even if the transfer residual toner particles are recovered by a mechanical force of rubbing, they adversely affect the triboelectric chargeability of the toner on the toner-carrying member if the charge of the recovered transfer residual toner particles has not been uniformized.

[0047] Thus, in the development and simultaneous cleaning or cleanerless image forming method, the continuous image-forming performance and resultant image quality are closely associated with the charge-controllability and attachment-mixing characteristic of the transfer residual toner particles at the time of passing by the charging member.

[0048] Further, JP-B 7−99442 discloses to apply powder on a surface of a contact charging member contacting the member-to-be-charged so as to prevent charging irregularity and stabilize the uniform charging performance. This system however adopts an organization of moving a contact charging member (charging roller) following the movement of the member-to-be-charged (photosensitive member) wherein the charging principle generally relies on the discharge charging mechanism simultaneously as in the above-mentioned cases of using a charging roller while the amount of ozone adduct has been remarkably reduced than in the case of using a corona charger, such as scorotron. Particularly, as an AC-superposed DC voltage is used for accomplishing a stable charging uniformity, the amount of ozone adducts is increased thereby. As a result, in the case of a continuous use of the apparatus for a long period, the defect of image flow due to the ozone products is liable to occur. Further, in case where the above organization is adopted in the cleanerless image forming apparatus, the attachment of the powder onto the charging member is obstructed by mixing with transfer-residual toner particles, thus reducing the uniform charging effect.

[0049] Further, JP-A 5−150539 has disclosed an image forming method using a contact charging scheme wherein a developer comprising at least toner particles and electroconductive particles having an average particle size smaller than that of the toner particles is used, in order to prevent the charging obstruction due to accumulation and attachment onto the charging member surface of toner particles and silica fine particles which have not been fully removed by the action of a cleaning blade on continuation of image formation for a long period. The contact charging or proximity charging scheme used in the proposal is one relying on the discharge charging mechanism and not based on the direct injection charging mechanism so that the above problem accompanying the discharge mechanism accrues.

[0050] Further, in case where the above organization is applied to a cleanerless image forming apparatus, larger amounts of electroconductive particles and toner particles are caused to pass through the charging step and have to be recovered in the developing step. No consideration on these matters or influence of such particles when such particles are recovered on the developing performance of the developer has been paid in the proposal. Further, in a case where a contact charging scheme relying on the direct injection charging scheme is adopted, the electroconductive fine particles are not supplied in a sufficient quantity to the contact charging member, so that the charging failure is liable to occur due to the influence of the transfer residual toner particles.

[0051] Further, in the proximity charging scheme, it is difficult to uniformly charge the photosensitive member in the presence of large amounts of electroconductive fine particles and transfer residual toner particles, thus failing to achieve the effect of removing the pattern of transfer residual toner particles. As a result, the transfer residual toner particles interrupt the imagewise exposure pattern light to cause a toner particle pattern ghost. Further, in the case of instantaneous power failure or paper clogging during image formation, the interior of the image forming apparatus can be remarkably soiled by the developer.

[0052] In order to improve the charge control performance when the transfer residual toner particles are passed by the charging member in the development and simultaneous cleaning method, JP-A 11−15206 has proposed to use a toner comprising toner particles containing specific carbon black and a specific azo iron compound in mixture with inorganic fine powder. Further, it has been also proposed to use a toner having a specified shape factor and an improved transferability to reduce the amount of transfer residual toner particles, thereby improving the performance of the development and simultaneous cleaning image forming method. This image forming method however relies on a contact charging scheme based on the discharge charging scheme and not on the direct injection charging scheme, so that the system is not free from the above-mentioned problems involved in the discharge charging mechanism. Further, these proposals may be effective for suppressing the charging performance of the contact charging member due to transfer residual toner particles but cannot be expected to positively enhance the charging performance.

[0053] Further, among commercially available electrophotographic printers, there is a type of development and simultaneous cleaning image forming apparatus including a roller member abutted against the photosensitive member at a position between the transfer step and the charging step so as to supplement or control the performance of recovering transfer residual toner particles in the development step. Such an image forming apparatus may exhibit a good development and simultaneous cleaning performance and remarkably reduce the waste toner amount, but liable to result in an increased production cost and a difficulty against the size reduction.

[0054] JP-A 10−307456 has disclosed an image forming apparatus adapted to a development and simultaneous cleaning image forming method based on a direct injection charging mechanism and using a developer comprising toner particles and electroconductive charging promoter particles having particle sizes smaller than ½ of the toner particle size. According to this proposal, it becomes possible to provide a development and simultaneous cleaning image forming apparatus which is free from generation of discharge product, can remarkably reduce the amount of waste toner and is advantageous for producing inexpensively a small size apparatus. By using the apparatus, it is possible to provide good images free from defects accompanying charging failure, and interruption or scattering of imagewise exposure light. However, a further improvement is desired.

[0055] Further, JP-A 10−307421 has disclosed an image forming apparatus adapted to a development and simultaneous cleaning method, based on the direct injection charging mechanism and using a developer containing electroconductive particles having sizes in a range of {fraction (1/50)}-½ of the toner particle size so as to improve the transfer performance.

[0056] JP-A 10−307455 discloses the use of electroconductive fine particles having a particle size of 10 nm-50 μm so as to reduce the particle size to below one pixel size and obtain a better charging uniformity.

[0057] JP-A 10−307457 describes the use of electroconductive particles of at most about 5 μm, preferably 20 nm −5 μm, so as to bring a part of charging failure to a visually less recognizable state in view of visual characteristic of human eyes.

[0058] JP-A 10−307458 describes the use of electro-conductive fine powder having a particle size smaller than the toner particle size so as to prevent the obstruction of toner development and the leakage of the developing bias voltage via the electroconductive fine powder, thereby removing image defects. It is also disclosed that by setting the particle size of the electroconductive fine powder to be larger than 0.1 μm, the interruption of exposure light by the electroconductive fine powder embedded at the surface of the image-bearing member is prevented to realize excellent image formation by a development and simultaneous cleaning method based on the direct injection charging scheme.

[0059] JP-A 10−307456 has disclosed a development and simultaneous cleaning image forming apparatus capable of forming good images without causing charging failure or interruption of imagewise exposure light, wherein electroconductive fine powder is externally added to a toner so that the electroconductive powder is attached to the image-bearing member during the developing step and allowed to remain on the image-bearing member even after the transfer step to be present at a part of contact between a flexible contact charging member and the image-bearing member.

[0060] These proposals however have left a room for further improvement regarding the stability of performance during repetitive use for a long period and performance in the case of using smaller size magnetic toner particles in order to provide an enhanced resolution.

[0061] Further, as such members-to-be-charged, electrophotographic photosensitive members comprising an OPC (organic photoconductor) or an amorphous silicon (sometimes referred to as “a-Si”) are known.

[0062] An OPC photosensitive member has a serious difficulty in wear resistance and durability, and a countermeasure thereto is urgently desired. Including the OPC photosensitive member, currently commercially available photosensitive members for use in image forming apparatus are not necessarily satisfactory in all respects of sensitivity, durability, image quality and anti-pollution characteristic, and the weak points of respective photosensitive members have been compensated by toner designing or process designing to provide commercially acceptable image forming apparatus on the market.

[0063] An a-Si photosensitive member has a high sensitivity over an entire visible wavelength region and is therefor compatible with a semiconductor laser and color image formation. Further, it has a high surface hardness as represented by a Vickers hardness of 1500-2000 kg-f/mm 2 and allows a long life as represented by 5×10 5 to 10 6 or an even larger member of sheets. An a-Si Photosensitive member also has a heat resistance sufficient in practical use of image forming apparatus.

[0064] It is generally said that an a-Si photoconductor layer has a dark-part surface potential corresponding to its layer thickness. Currently commercialized photosensitive members include CdS-photosensitive members showing a dark-part surface potential of at least 500 volts, and Se-photosensitive member and OPC-photosensitive member showing dark-part surface potentials of at least 600−800 volts. In order to realize such a level of surface potential with an a-Si photoconductor layer, the layer thickness has to be increased.

[0065] In contrast thereto, in order to provide satisfactory productivity and production costs of a-Si photosensitive member and also satisfactory performances thereof, it has been proposed to form a photosensitive member having a smaller thickness of a-Si photoconductor layer, which however necessitates the selective use of a toner allowing a low developing potential. This is because a lower thickness of a-Si layer results in a lower surface potential then an OPC photosensitive member while it favors production cost and capacity and photosensitivity.

[0066] Accordingly, in order to use an a-Si photosensitive member commercially satisfactorily, it is necessary to use a toner having a high developing performance. It is also necessary to control the surface property of such a small-thickness a-Si layer for providing high image quality and high durability. a-Si photosensitive members comprising a non-single crystal deposition film principally comprising silicon as represented by a-Si and containing, e.g., hydrogen and/or a halogen, such as fluorine or chlorine, for compensating for hydrogen or dangling bond's have been proposed as a high-performance, high-durability and non-polluting photosensitive member, and several embodiments thereof have been commercialized. More specifically, U.S. Pat. No. 4,265,991 and JP-A 54−86341 have disclosed an electrophotographic photosensitive member including a photoconductor layer principally comprising a-Si. JP-A 60−12554 has disclosed a photosensitive member including a photoconductor layer comprising amorphous silicon and a surface layer containing carbon and halogen atoms. JP-A 2−111962 has disclosed a photosensitive member including a photosensitive layer of a-Si:H or a-C:H and a surface-protecting lubrication layer. These publications are all directed to provision of a photosensitive member with improved water-repellency and wear resistance and do not relate to improvements in magnetic toner and electrophotography process in combination with such a-Si photosensitive members.

SUMMARY OF THE INVENTION

[0067] An object of the present invention is to provide an image forming system (i.e., method and apparatus) which includes the use of a magnetic toner showing a stabling uniform chargeability regardless of environmental conditions and an amorphous or non-single crystal silicon photosensitive member and can provide fog-free images at high image density, good transferability and good image reproducibility for a long period of use.

[0068] Another object of the present invention is to provide an image forming system capable of stably providing good images without including an independent cleaning means.

[0069] A further object of the present invention is to provide an image forming system capable of preventing the generation of discharge products, remarkably reducing the amount of waste toner and providing good images free from charging failure even in a long period of repetitive image formation without including an independent cleaning means, thus providing an inexpensive and small-sized image forming system.

[0070] According to the present invention, there is provided an image forming method, comprising:

[0071] a charging step of charging an image-bearing member by charging means comprising a charging member supplied with a voltage and abutted against the image-bearing member at a contact position;

[0072] a latent-image forming step of forming an electrostatic latent image on the charged image-bearing member,

[0073] a developing step of transferring a magnetic toner carried on a toner-carrying member onto the electrostatic latent image to develop the latent image, thereby forming a magnetic toner image on the image-bearing member, and

[0074] a transfer step of electrostatically transferring the magnetic toner image on the image-baring member onto a transfer material via or without via an intermediate transfer member,

[0075] wherein the image-bearing member comprises an electroconductive support and a photoconductor layer comprising a silicon-based non-single crystal material and disposed on the electroconductive support, and is charged to a potential of 250 to 600 volts in terms of an absolute value via the charging member abutted against it,

[0076] the magnetic toner includes magnetic toner particles comprising at least a binder resin and a magnetic iron oxide, and inorganic fine powder and electroconductive fine powder present at the surface of the magnetic toner particles,

[0077] the magnetic toner has a weight-average particle size of 3-10 μm, the magnetic toner has an average circularity of 0.950 to 0.995, and the magnetic toner contains 0.05 to 3.00% of isolated iron-containing particles.

[0078] The present invention further provides an image forming apparatus, comprising: an image-bearing member, a charging means for charging the image-bearing member, an electrostatic latent-image forming means for forming an electrostatic latent image on the charged image-bearing member, a developing means including a toner-carrying member for transferring a magnetic toner carried on the toner-carrying member onto the electrostatic latent image to form a toner image thereon, and a transfer means for electrostatically transferring the toner image on the image-bearing member onto a transfer material, wherein the charging means comprises a charging member supplied with a voltage and abutted against the image-bearing member to form a contact nip with the image-bearing member, the image-bearing member comprises an electroconductive support and a photoconductor layer comprising a silicon-based non-single crystal material and disposed on the electroconductive support, and is charged to a potential of 250 to 600 volts in terms of an absolute value via the charging member abutted against it,

[0079] the magnetic toner includes magnetic toner particles comprising at least a binder resin and a magnetic iron oxide, and inorganic fine powder and electroconductive fine powder present at the surface of the magnetic toner particles,

[0080] the magnetic toner has a weight-average particle size of 3-10 μm,

[0081] the magnetic toner has an average circularity of 0.950 to 0.995, and

[0082] the magnetic toner contains 0.05 to 3.00% of isolated iron-containing particles.

[0083] These and other objects, features and advantages of the present invention will become more apparent upon a consideration of the following description of the preferred embodiments of the present invention taken in conjunction with the accompanying drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

[0084] FIG. 1 is a graph showing charging performances of several contact charging means.

[0085] FIGS. 2 and 3 respectively illustrate an embodiment of image forming system according to the invention.

[0086] FIG. 4 illustrates a developing device suitable for use in an image forming system of the invention.

[0087] FIGS. 5 and 6 are schematic sectional views for illustrating a sectional organization of an image-bearing member usable in an image forming system according to the invention.

[0088] FIG. 7 illustrates a contact transfer means suitably used in an image forming system of the invention.

[0089] FIG. 8 is a schematic sectional view for illustrating a sectional organization of a comparative photosensitive member (image-bearing member).

DETAILED DESCRIPTION OF THE INVENTION

[0090] For the purpose of uniformizing and stabilizing the chargeability of an image-bearing member for a long period in the image forming system of the present invention, it is important to satisfy a specific percentage of iron-containing isolated particles in the magnetic toner, and a specific relationship of material and charged potential of the image-bearing member.

[0091] The iron-containing isolated particles (comprising iron or an iron compound) in the magnetic toner used in the present invention are originated from magnetic iron oxide particles used as magnetic powder in the magnetic toner and play an important role for uniformizing and stabilizing the chargeability of the image-bearing member together with electroconductive fine powder externally added to the magnetic toner particles. Isolated magnetic iron oxide particles exhibit a low resistivity and a weak chargeability and also a property of abrading a member contacting the particles because of a high hardness thereof. On the other hand, the image-bearing member has a photoconductor layer formed of a silicon-based non-single crystal material, so that it exhibits a high surface free energy and has a tendency of showing a strong interaction with inorganic (fine) particles. The magnetic iron oxide particles thus attached to the image-bearing member surface function to enhance the injection charging performance in the charging step, and abrade the image-bearing member at the contact nip between the charging member, thereby refreshing the image-bearing member surface to retain the charging uniformity for a long period.

[0092] If the image-bearing member is charged to a surface potential of 250 to 600 volts and the isolated magnetic iron oxide particles are contained in a percentage of 0.05 to 3.00% by number of the toner particles), the magnetic iron oxide particles and electroconductive fine powder are supplied at an appropriate rate from the magnetic toner to the surface of the photoconductor layer comprising a silicon(Si)-based non-single crystal material and removed at an appropriate rate from the photoconductor layer surface, so that the amounts of the magnetic iron oxide particles and electroconductive fine powder on the photoconductor layer surface are stabilized to further stabilize the injection charging performance in the charging step and suppress the abrasion irregularity on the image-bearing member surface leading to non-uniform chargeability.

[0093] Herein, the “non-single crystal material” constituting a surface or photoconductor layer of the image-bearing is principally in an amorphous state but can contain a minor proportion of microcrystalline or polycrystalline material unlike a single-crystal material as is understood from representative processes for production of such a photoconductor or surface layer described hereinafter. The term “silicon-based” means that the material comprises silicon as a principal element.

[0094] To describe more fully the composition of the magnetic toner used in the present invention, it is important that the magnetic toner includes magnetic toner particles comprising at least a binder resin and a magnetic iron oxide, and inorganic fine powder and electroconductive fine powder present at the surface of the magnetic toner particles; has an average circularity of 0.950 to 0.995; and contains 0.05 to 3.00% of isolated iron-containing particles.

[0095] If the magnetic toner has an average circularity of at least 0.950, the surface unevenness of the magnetic toner particles is alleviated to some extent so that inorganic fine powder and electroconductive fine powder as other components of the magnetic toner of the present invention can be uniformly attached to the magnetic toner particle surfaces, thus providing a level of flowability suitable for use in an electrophotographic process. Below 0.950, a sufficient flowability is liable to be failed in some cases.

[0096] In the image forming system of the present invention, in the case where the developing step (or means) is also used as a step (or means) for recovering residual toner on the image-bearing member, the electroconductive fine powder behaves separately from the toner particles and is supplied to the charging step to promote the charging of the image-bearing member. In this instance, if the toner has an average circularity below 0.950, the effective supply of the electroconductive fine powder from the toner to the charging step is liable to be hindered.

[0097] A higher circularity of toner tends to improve the image forming performances, and an average circularity of 0.970 or higher is preferred.

[0098] A toner comprising toner particles having an average circularity of 0.970 or higher exhibits a very excellent transferability. This is presumably because in such a magnetic toner having a high circularity, the magnetic toner particles are cause to have a small contact area with the photosensitive member, thus resulting in a small force of attachment force attributable to image force and van der Waals force onto the photosensitive member. As a result of a high transferability. The amount of transfer residual toner is reduced, and the amount of the magnetic toner present at the pressure nip between the charging member and the photosensitive member is reduced to prevent the occurrence of toner attachment onto the photosensitive member, thus remarkably reducing image defects.

[0099] Further, magnetic toner particles having an average circularity of at least 0.970 are almost free from surface edges to reduce the friction at the pressure nip between the charging member and the photosensitive member, to suppress the abrasion of the photosensitive member surface. These effects are particularly pronounced in an image forming method including a contact transfer step liable to cause a hollow transfer image dropout. It is particularly preferred that the magnetic toner has a mode circularity of at least 0.990 meaning that particles having a circularity of at least 0.990 are predominant since the effect can be insufficient in some cases if predominant particles have a low circularity even if the average circularity is high.

[0100] If the magnetic toner satisfies preferable features having an average circularity of at least 0.970 and a mode circularity of 0.990, toner ears formed on the toner-carrying member become fine and dense to provide a uniform charge, so that fog is remarkably reduced.

[0101] The average circularity and mode circularity are used as quantitative measures for evaluating particle shapes and based on values measured by using a flow-type particle image analyzer (“FPIA-1000”, mfd. by Toa Iyou Denshi K.K.). A circularity (Ci) of each individual particle (having a circle equivalent diameter (DCE) of at least 3.0 μm) is determined according to an equation (1) below, and the circularity values (Ci) are totaled and divided by the number of total particles (m) to determine an average circularity (Ca) as shown in an equation (2) below:

Circularity Ci=L 0 /L, (1)

[0102] wherein L denotes a circumferential length of a particle projection image, and L 0 denotes a circumferential length of a circle having an area identical to that of the particle projection image. 1 Average circularity ( Ca ) = i = 1 m Ci / m ( 2 ) embedded image

[0103] Further, the mode circularity (Cmod) is determined by allotting the measured circularity values of individual toner particles to 61 classes in the circularity range of 0.40-1.00, i.e., from 0.400-0.410, 0.410-0.420, . . . , 0.990-1.000 (for each range, the upper limit is not included) and 1.000, and taking the circularity of a class giving a highest frequency as a mode circularity (Cmod).

[0104] Incidentally, for actual calculation of an average circularity (Ca), the measured circularity values (Ci) of the individual particles were divided into 61 classes in the circularity range of 0.40-1.00, and a central value of circularity of each class was multiplied with the frequency of particles of the class to provide a product, which was then summed up to provide an average circularity. It has been confirmed that the thus-calculated average circularity (Ca) is substantially identical to an average circularity value obtained (according to Equation (2) above) as an arithmetic mean of circularity values directly measured for individual particles without the above-mentioned classification adopted for the convenience of data processing, e.g., for shortening the calculation time.

[0105] More specifically, the above-mentioned FPIA measurement is performed in the following manner. Into 10 ml of water containing ca. 0.1 mg of surfactant, ca. 5 mg of magnetic toner sample is dispersed and subjected to 5 min. of dispersion by application of ultrasonic wave (20 kHz, 50 W), to form a sample dispersion liquid containing 5,000−20,000 particles/μl. The sample dispersion liquid is subjected to the FPIA analysis for measurement of the average circularity (Ca) and mode circularity (Cm) with respect to particles having D CE ≧3.0 μm.

[0106] The average circularity (Ca) used herein is a measure of roundness, a circularity of 1.00 means that the magnetic toner particles have a shape of a perfect sphere, and a lower circularity represents a complex particle shape of the magnetic toner.

[0107] Herein, only particles having a circle-equivalent diameter (D CE =L/π) of at least 3 μm are taken for the circularity measurement because particles smaller than 3 μm include a substantial amount of external additives and the inclusion of such particles can distort the circularity characteristic of magnetic toner particles.

[0108] A magnetic toner having an average circularity (Ca) of at least 0.950, preferably at least 0.970 and a mode circularity (Cmod) of at least 0.990 exhibits a remarkably improved transferability even at a small particle size, which has provided a difficulty in providing an improved transferability, and also exhibits a remarkably improved developing performance for a low-potential latent image. It is particularly effective for development of digital minute spot latent images. This means that the magnetic toner exhibits a good matching with a non-single crystal (or roughly amorphous) silicon photosensitive member used in the image forming system of the present invention.

[0109] If the average circularity (Ca) is below 0.950, the magnetic toner not only exhibits a lower transferability but also can exhibit a lower developing performance. On the other hand, if the average circularity exceeds 0.995, the toner surface deterioration becomes noticeable, thus posing a problem in durability.

[0110] Next, the percentage of isolated iron-containing particles will be described. The isolated iron-containing particles are particles of iron or iron compound (typically magnetic iron oxide particles) isolated from magnetic toner particles. The isolation percentage can also be determined by observation through, e.g., a scanning electron microscope but may conveniently be determined by plasma-induced particle luminescence spectra. In the latter measurement method, the percentage of isolated iron-containing particles (Fe.iso (%)) is determined based on the frequency of atomic luminescence (abbreviated as “AL”) of Fe separate or simultaneous with C (carbon) atomic luminescence and calculated according to the following formula:

Fe.iso (%)=100×{number of AL of Fe alone}/{(number of AL of Fe simultaneous with AL of C)+(number of AL of Fe alone)}

[0111] In this instance, AL of Fe is regarded as simultaneous if it occurs within 2.6 m.sec from AL of C, and regarded as separate if it occurs thereafter.

[0112] In the case of a magnetic toner particle containing magnetic iron oxide particles, the simultaneous luminescences of carbon atom and iron atom means a luminescence from a toner particle containing magnetic iron oxide dispersed therein, and the luminescence of only iron atom means a luminescence from an isolated iron-containing particle.

[0113] In the plasma-induced luminescence measurement method, fine particles like toner particles are introduced into plasma, particle by particle, to determine an element and a particle size of a luminescent particle from its luminescence spectrum. For example, in the case where a magnetic toner particle is introduced into plasma, each toner particle causes one luminescence of carbon (constituting the binder resin) and one luminescence of iron (constituting the magnetic iron oxide) which can be respectively observed. As one toner particle causes one luminescence, the number of toner particles can be determined based on the number of observed luminescences (C with Fe). The measurement may be performed by using, e.g., a particle analyzer (“PT1000”, made by Yokogawa Denki K.K.) according to a principle described in Japan Hardcopy '97 Paper Collection, pp. 65-68.

[0114] More specifically, for the measurement, a sample toner left standing overnight in an environment of 23° C. and 60%RH is subjected to measurement together with 0.1% O 2 -containing helium gas in the above environment. For spectrum separation, Channel 1 detector is used for carbon atom (at wavelength of 247.86 nm, with a recommended value of K factor) and Channel 2 detector is used for iron atom (at wavelength of 239.56 nm, with K factor of 3.3764). Sampling is performed at a rate of one scan for covering 1000-1400 times of luminescence of carbon atom, and the sampling is repeated until the luminescences of carbon atom reaches at least 10,000 times. By integrating the luminescences, a particle size distribution curve is drawn with the number of luminescences taken on the ordinate and with the cube root of voltage representing a particle size on the abscissa, while effecting the sampling so that the particle size distribution curve exhibits a single peak and no valley. Based on the measured data while taking noise cut level during the measurement at 1.50 volts, Fe.iso (%) is calculated according to the above formula.

[0115] Incidentally, an azo-iron compound as a charge control agent may be contained in a toner in some cases, but the azo iron compound is an organometallic compound, so that it cannot result in a luminescence of only iron atom.

[0116] As a result of our study, there is found a close correlation between the percentage of isolated iron-containing particles (Fe.iso (%)) and the rate of exposure of magnetic iron oxide particles at the toner particle surfaces. More specifically, if Fe.iso (%) is at most 3.00%, the exposure at the toner particle surfaces of magnetic iron oxide particles is suppressed to provide a high chargeability. This is attributable to the uniformity of particle size distribution of the magnetic iron oxide particles and uniformity of surface treatment of the magnetic iron oxide particles. For example, in case where the surface treatment of the magnetic iron oxide particles is ununiform, magnetic iron oxide fine particles having a high hydrophillicity due to insufficient surface treatment are exposed to the toner particle surface, and a portion or all of them can be isolated from the toner particles.

[0117] Accordingly, a magnetic toner containing a lower percentage of isolated iron-containing particles tends to show a higher chargeability. On the other hand, if Fe.iso (%) is higher than 3.00%, the charge-leakage points are increased, thus being liable to result in a magnetic toner having an insufficient chargeability. This tendency becomes particularly remarkable in a high temperature/high humidity environment. A magnetic toner having a low chargeability is not desirable because it causes increased fog, causes a lower transferability and is liable to cause charging failure. Further, a magnetic toner satisfying both a high average circularity and a low percentage of isolated iron-containing particles can acquire a high chargeability and also a very high transferability as a result of synergy with the toner particle shape.

[0118] On the other hand, an Fe-iso (%) of below 0.05% means that substantially no magnetic iron oxide particles are isolated from the magnetic toner particles. Such a magnetic toner having a low Fe.iso (%) has a high chargeability but is liable to cause an excessive charge resulting in images having a low image density and accompanied with roughening, in image formation on a large number of sheets, particularly in a low temperature/low humidity environment. This is presumably because of the following mechanism.

[0119] A magnetic toner carried on a toner-carrying member is not wholly transferred for development onto the photosensitive member, but some magnetic toner remains on the toner-carrying member even immediately after the development. This tendency is particularly noticeable in the jumping developing mode using a magnetic toner. Further, magnetic toner particles having a high circularity form uniformly thin ears in the developing regions, and toner particles present at the tips of ears are used for development and toner particles present close to the toner-carrying member are not readily consumed for the development.

[0120] As a result, the magnetic toner particles close to the toner carrying member are liable to be excessively charged due to repetitive tribo-electrification with the charging members, and the transfer for development thereof becomes further difficult. In such a state, the charge uniformity of the magnetic toner is impaired, to result in rough images.

[0121] Now, if a magnetic toner having Fe.iso (%) >0.05% is used, the excessive charge of the magnetic toner is suppressed due to the isolated magnetic iron oxide particles and magnetic iron oxide particles present at the toner particle surfaces, and the charge uniformity of the magnetic toner is promoted to suppress the roughening of images.

[0122] As a result, even for a magnetic toner having a high circularity and a high chargeability, the excessive charge (charge-up phenomenon) in a long-term use can be alleviated if the exposed magnetic iron oxide particles are present, so that Fe.iso (%) of at least 0.05% is important.

[0123] For the above reason, Fe.iso (%) of 0.05% -3.00% is necessary. Fe.iso (%) is preferably 0.05-2.00%, more preferably 0.05−1.50%, further preferably 0.05−0.80%.

[0124] The magnetic toner used in the present invention may preferably comprise magnetic toner particles produced through the polymerization process. The magnetic toner particles can be produced through the pulverization process, but the magnetic toner particles produced through the pulverization process are generally indefinitely shaped and have to be mechanically or thermally treated in order to have an average circularity of at least 0.950 as an essential requirement, or a preferable circularity of at least 0.970 (and also a preferred mode circularity of at least 0.990).

[0125] Thus, in the present invention, the magnetic toner particles may preferably be produced through the polymerization process, examples of which may include: direct polymerization, suspension polymerization, emulsion polymerization, emulsion-association polymerization and seed polymerization. Among these, the suspension polymerization process is particularly preferred in order to easily provide a good balance of particle size and particle shape.

[0126] In the suspension polymerization process for producing a magnetic toner according to the present invention, a monomeric mixture is formed by uniformly dissolving or dispersing a monomer and magnetic powder (fine particles) (and, optionally, other additives, such as wax, a colorant, a crosslinking agent and charge control agent), followed by dispersing the monomeric mixture in an aqueous medium containing a dispersion stabilizer by means of an appropriate stirrer, and subjecting the dispersed monomeric mixture to suspension polymerization in the presence of a polymerization initiator to obtain toner particles of a desirable particle size.

[0127] The magnetic polymerization toner polymerized through the suspension polymerization process is caused to comprise individual toner particles having a uniformly spherical shape, so that it is easy to obtain a toner having a circularity of at least 0.970 as a preferred physical requirement of the present invention, and further such a magnetic toner has a relatively uniform chargeability distribution, thus exhibiting a high transferability.

[0128] However, by using a monomeric mixture containing ordinary magnetic powder at the time of suspension polymerization, it is difficult to suppress the exposure of the magnetic powder to the resultant toner particle surface, the resultant toner particles are liable to have remarkably lower flowability and chargeability, and also it is difficult to obtain a magnetic toner having a desirable circularity because of strong interaction between the magnetic powder and water. This is (1) because magnetic powder particles are generally hydrophillic, thus being liable to be localized at the toner particle surfaces, and (2) because at the time of suspension of the monomeric mixture in an aqueous medium or at the time of stirring the suspension liquid during the polymerization, the magnetic powder is moved at random within the suspended liquid droplets and the suspended liquid droplet surfaces comprising the monomer are pulled by the randomly moving magnetic powder, thereby distorting the liquid droplets from spheres. In order to solve such problems, it is important to modify the surface property of the magnetic iron oxide powder.

[0129] As for magnetic powder used in the magnetic toner of the present invention, it is extremely preferred that the magnetic iron oxide particles are surface-treated for hydrophobization by dispersing magnetic iron oxide particles in an aqueous medium into primary particles thereof, and while maintaining the primary particle dispersion state, hydrolyzing a coupling agent in the aqueous medium to surface-coat the magnetic iron oxide particles. According to this hydrophobization method in an aqueous medium, the magnetic iron oxide particles are less liable to coalesce with each other than in a dry surface-treatment in a gaseous system, and the magnetic iron oxide particles can be surface-treated while maintaining the primary particle dispersion state due to electrical repulsion between hydrophobized magnetic iron oxide particles.

[0130] The method of surface-treatment of magnetic iron oxide particles with a coupling agent while hydrolyzing the coupling agent in an aqueous medium does not require gas-generating coupling agents, such as chlorosilanes or silazanes, and allows the use of a high-viscosity coupling agent which has been difficult to use because of frequent coalescence of magnetic iron oxide particles in a conventional gaseous phase treatment, thus exhibiting a remarkable hydrophobization effect.

[0131] As a coupling agent usable for surface-treating the magnetic iron oxide particles used in the present invention, a silane coupling agent or a titanate coupling agent may be used. A silicone coupling agent is preferred, and examples thereof may be represented by the following formula (I):

R m SiY n (I),

[0132] wherein R denotes an alkoxy group, Y denotes a hydrocarbon group, such as alkyl, vinyl, glycidoxy or methacryl, and m and n are respectively integers of 1-3 satisfying m+n=4.

[0133] Examples of the silane coupling agents represented by the formula (I) may include: vinyltrimethoxysilane, vinyltriethoxysilane, gamma-methacryloxypropyltrimethoxysilane, vinyltriacetoxysilane, methyltrimethoxysilane, methyltriethoxysilane, isobutyltrimethoxysilane, dimethyldimethoxysilane, dimethyldiethoxysilane, trimethylmethoxysilane, hydroxypropyltrimethoxysilane, phenyltrimethoxysilane, n-hexadecyltrimethoxysilane, and n-octadecyltrimethoxysilane.

[0134] It is particularly preferred to use an alkyltrialkoxysilane coupling agent represented by the following formula (II) to treat the magnetic powder for hydrophobization in an aqueous medium:

C p H 2p+1 —Si—(OC q H 2q+1 ) 3 (II),

[0135] wherein p is an integer of 2-20 and q is an integer of 1-3.

[0136] In the above formula (II), if p is smaller than 2, the hydrophobization treatment may become easier, but it is difficult to impart a sufficient hydrophobicity, thus making it difficult to suppress the exposure of the magnetic powder to the toner particle surfaces. On the other hand, if p is larger than 20, the hydrophobization effect is sufficient, but the coalescence of the magnetic powder particles becomes frequent, so that it becomes difficult to sufficiently disperse the treated magnetic powder particles in the toner, thus being liable to result in a toner exhibiting lower fog-prevention effect and transferability.

[0137] If q is larger than 3, the reactivity of the silane coupling agent is lowered, so that it becomes difficult to effect sufficient hydrophobization.

[0138] It is particularly preferred to use an alkyltrialkoxysilane coupling agent represented by the formula (II) wherein p is an integer of 3-15, and q is an integer of 1 or 2.

[0139] The coupling agent may preferably be used in 0.05-20 wt. parts, more preferably 0.1-10 wt. parts, per 100 wt. parts of the magnetic powder.

[0140] Herein, the term “aqueous medium” means a medium principally comprising water. More specifically, the aqueous medium includes water alone, and water containing a small amount of surfactant, a pH adjusting agent or/and an organic solvent.

[0141] As the surfactant, it is preferred to use a nonionic surfactant, such as polyvinyl alcohol. The surfactant may preferably be added in 0.1-5 wt. parts per 100 wt. parts of water. The pH adjusting agent may include an inorganic acid, such as hydrochloric acid. The organic solvent may include methanol which may preferably be added in a proportion of 0-500 wt. % of water.

[0142] For the surface-treatment of magnetic iron oxide particles with a coupling agent in an aqueous medium, appropriate amounts of magnetic iron oxide particles and coupling agent may be stirred in an aqueous medium. It is preferred to effect the stirring by means of a mixer having stirring blades, e.g., a high-shearing force mixer (such as an attritor or a TK homomixer) so as to disperse the magnetic iron oxide particles into primary particles in the aqueous medium under sufficient stirring.

[0143] The thus-surface treated magnetic iron oxide is free from particle agglomerates and individual particles are uniformly surface-hydrophobized. Accordingly, the magnetic powder is uniformly dispersed in polymerization toner particles to provide almost spherical polymerization toner particles free from surface-exposure of the magnetic iron oxide. As a result, by using such magnetic iron oxide particles, it becomes possible to provide a magnetic toner having Ca≧0.970, Cmod≧0.990 and Fe.iso (%)≦1.50%.

[0144] If such a magnetic toner is used in the image forming method of the present invention, the abrasion of and toner melt-attachment onto the photosensitive member are further effectively suppressed, and it becomes possible to form high-quality images stably even in a low humidity environment.

[0145] Further, while the magnetic toner has a uniformly high chargeability due to presence of little or no surface-exposed magnetic iron oxide, the magnetic toner can provide good image during image formation on a large number of sheets in a low temperature/low humidity environment due to the presence of electroconductive fine powder at the magnetic toner particle surfaces.

[0146] It is preferred that the magnetic toner used in the present invention contains a wax as described below in a proportion of 0.1-20 wt. % thereof.

[0147] In the image forming method, a magnetic toner image transferred onto a transfer(-receiving) material, such as paper, is thereafter fixed onto the transfer material by application of energy, such as heat and/or pressure, to provide a semipermanently fixed image. In this instance, a heat-pressure fixing scheme, such as a hot roller-fixing scheme, is frequently adopted.

[0148] By using a weight-average particle size of at most 10 μm, it is possible to obtain a very high-definition image, but such a small-particle size magnetic toner particles are liable to be buried between fibers of paper as a typical transfer medium and fail to receive sufficient heat, thus being liable to cause low-temperature offset. However, by including an appropriate amount of a wax as a release agent, the magnetic toner used in the present invention can satisfy both a high resolution and anti-offset characteristic as well as prevention of abrasion of the photosensitive member.

[0149] Examples of waxes usable in the magnetic toner used in the present invention may include: petroleum waxes and derivatives thereof, such as paraffin wax, microcrystalline wax and petrolactum; montan wax and derivatives thereof; hydrocarbon wax by Fischer-Tiropsch process and derivative thereof; polyolefin waxes as represented by polyethylene wax and derivatives thereof; and natural waxes, such as carnauba wax and candelilla wax and derivatives thereof. The derivatives may include oxides, block copolymers with vinyl monomers, and graft-modified products. Further examples may include: higher aliphatic alcohols, fatty acids, such as stearic acid and palmitic acid, and compounds of these, acid amide wax, ester wax, ketones, hardened castor oil and derivatives thereof, vegetable waxes and animal waxes.

[0150] Among such waxes, it is preferred to use a wax showing a maximum heat-absorption peak in a temperature range of 40-110° C., more preferably 45-90° C., in the course of temperature increase on a DSC cure measured by using a differential scanning calorimeter. The inclusion of a wax having a maximum heat-absorption peak in the above-mentioned temperature range, contributes to improvements in low-temperature fixability and effective releasability. If the maximum heat-absorption peak temperature (Tabs.max) is below 40° C., the wax is liable to exhibit only a weak self-cohesion, thus lowering the anti-high-temperature offset characteristic. On the other hand, if Tabs.max exceeds 110° C., the fixation temperature is raised so that low-temperature offset is liable to occur. Further, in the case of production of magnetic toner particles by particle formation and polymerization in an aqueous medium, the wax is liable to precipitate during the particle formation.

[0151] The maximum heat-absorption peak temperature (Tabs.max) of a wax may be measured by using a differential scanning calorimeter (DSC) (e.g., “DSC-7”, available from Perkin-Elmer Corp.) according to ASTM D3418-8. Temperature correction of the detector may be effected based on melting points of indium and zinc, and calorie correction may be effected based on heat of fusion of indium. For the measurement, a sample is placed on an aluminum pan and subjected to heat at an increasing rate of 10° C./min in parallel with a blank aluminum pan as a control.

[0152] The magnetic toner used in the present invention may preferably contain such a wax in a proportion of 0.1-20 wt. % of the entire magnetic toner. Below 0.1 wt. %, the low-temperature offset-suppression effect is lowered, and above 20 wt. %, the long-term storability is lowered and the dispersibility of the other toner ingredients becomes lowered to result in lower flowability and image forming performances of the resultant magnetic toner.

[0153] The magnetic toner used in the present invention can further contain a charge control agent so as to stabilize the chargeability. Known charge control agents can be used. It is preferred to use a charge control agent providing a quick charging speed and stably providing a constant charge. In the case of polymerization toner production, it is particularly preferred to use a charge control agent showing low polymerization inhibition effect and substantially no solubility in aqueous dispersion medium.

[0154] Specific examples of negative charge control agents may include: metal compounds of aromatic carboxylic acids, such as salicylic acid, alkylsalicylic acids, dialkylsalicylic acids, naphthoic acid, and dicarboxylic acids; metal salts or metal complexes of azo-dyes and azo pigments; polymeric compounds having a sulfonic acid group or carboxylic acid group in side chains; boron compounds, urea compounds, silicon compounds, and calixarenes.

[0155] Positive charge control agents may include: quaternary ammonium salts, polymeric compounds having such quaternary ammonium salts in side chains, quinacridone compounds, nigrosine compounds and imidazole compounds.

[0156] The charge control agent may be included in the toner by internal addition or external addition to the toner particles. The amount of the charge control agent can vary depending on toner production process factors, such as binder resin species, other additives and dispersion methods, but may preferably be 0.1-10 wt. parts, more preferably 0.1-5 wt. parts, per 100 wt. parts of the binder resin.

[0157] In the case of providing a negatively chargeable magnetic toner, it is preferred to add a metal salt or a metal complex of an azo dye or an azo pigment.

[0158] However, it is not essential for the magnetic toner used in the present invention to contain a charge control agent, but the toner need not necessarily contain a charge control agent by positively utilizing the triboelectrification with a toner layer thickness-regulating member and a toner-carrying member.

[0159] Next, description will be made on the magnetic iron oxide and the binder resin contained in the magnetic toner particles.

[0160] The magnetic toner particles contain at least particles of a magnetic iron oxide, such as magnetite, maghemite, or ferrite.

[0161] The magnetic iron oxide particles may preferably have a BET specific surface area (SBET) of 2-30 m/g, more preferably 3-28 m/g, as measured according to nitrogen-adsorption, and a Mohs' hardness of 5-7.

[0162] For providing the magnetic toner used in the present invention, the magnetic iron oxide particles may preferably be used in 10-200 wt. parts, more preferably 20-180 wt. parts, per 100 wt. parts of the binder resin. Below 10 wt. parts, the coloring power of the resultant magnetic toner is liable to be insufficient, and the suppression of fog becomes difficult. Above 200 wt. parts, the resultant toner is held at an excessively large force onto the toner-carrying member, to show a lower developing performance. Moreover, the dispersion of magnetic iron oxide particles to individual toner particles becomes difficult, and the fixability is lowered.

[0163] The magnetic iron oxide particles used for constituting the magnetic toner used in the image forming method of the invention may be produced, e.g., in the following manner, in the case of magnetite-based magnetic iron oxide.

[0164] To a ferrous salt aqueous solution, an alkali, such as sodium hydroxide, in an amount equivalent to the iron in the ferrous salt or larger to prepare an aqueous solution containing ferrous hydroxide. While retaining the pH of the thus-prepared aqueous solution at pH 7, preferably pH 8-10 and warming the aqueous solution at a temperature of 70° C. or higher, air is blown into the aqueous solution to oxidize the ferrous hydroxide, thereby first forming seed crystals functioning as nuclei of magnetic iron oxide particles to be produced.

[0165] Then, to the slurry-form liquid containing the seed crystals, an aqueous solution containing ferrous salt in an amount of ca. 1 equivalent based on the amount of the previously added alkali, is added. While keeping the liquid at pH 6-10, air is blown thereinto to proceed with the reaction of the ferrous hydroxide, thereby growing magnetic iron oxide particles around the seed crystals as nuclei. Along with the progress of the oxidation reaction, the liquid pH is shifted toward an acidic side, but it is preferred not to allow the liquid pH go down to below 6. At a final stage of the oxidation, the liquid pH is adjusted, and the slurry liquid is sufficiently stirred so as to disperse the magnetic iron oxide in primary particles. In this state, a coupling agent for hydrophobization is added to the liquid to be sufficiently mixed under stirring. Thereafter, the slurry is filtered out and dried, and the dried product is lightly disintegrated to provide hydrophobic treated magnetic iron oxide particles.

[0166] Alternatively, the iron oxide particles after the oxidation reaction may be washed, filtered out and then, without being dried, re-dispersed in another aqueous medium. Then, the pH of the re-dispersion liquid is adjusted and subjected to hydrophobization by adding a coupling agent under sufficient stirring. Anyway, it is preferred that untreated iron oxide particles formed in the oxidation reaction system are subjected to hydrophobization in their wet slurry state and without being dried prior to the hydrophobization.

[0167] As the ferrous salt used in the above-mentioned production process, it is generally possible to use ferrous sulfate by-produced in the sulfuric acid process for titanium production or ferrous sulfate by-produced during surface washing of steel sheets. It is also possible to use ferrous chloride. In the above-mentioned process for producing magnetic iron oxide from a ferrous salt aqueous solution, a ferrous salt concentration of 0.5-2 mol/liter is generally used so as to obviate an excessive viscosity increase accompanying the reaction and in view of the solubility of a ferrous salt, particularly of ferrous sulfate. A lower ferrous salt concentration generally tends to provide finer magnetic iron oxide particles. Further, as for the reaction conditions, a higher rate of air supply, and a lower reaction temperature, tend to provide finer product particles.

[0168] By using a magnetic toner containing the thus-produced hydrophobic magnetic iron oxide particles, it becomes possible to realize an image forming method wherein the abrasion of and toner attachment onto the photosensitive member are effectively suppressed to stably provide high-quality images.

[0169] The magnetic iron oxide particles may have octahedral, hexahedral, spherical, acicular or flaky shape, but magnetic iron oxide particles having less anisotropic shapes, such as octahedral, hexahedral or spherical are preferred in order to provide a high image density. Such particle shapes may be confirmed by observation through a scanning electron microscope (SEM).

[0170] It is preferred that the magnetic iron oxide particles have a volume-average particle size of 0.1-0.3 μm and contain at most 40% by number of particles of 0.03-0.1 μm, based on measurement of particles having particle sizes of at least 0.03 μm, also in view of magnetic properties of the magnetic iron oxide particles. It is further preferred that the amount of particles of 0.3 μm or larger is suppressed to at most 10% by number.

[0171] Magnetic iron oxide particles having an average particle size of below 0.1 μm are not generally preferred because they are liable to provide a magnetic toner giving images which are somewhat tinted in red and insufficient in blackness with enhanced reddish tint in halftone images. Further, as the magnetic iron oxide particles are caused to have an increased surface area, the dispersibility thereof is lowered, and an inefficiently larger energy is consumed for the production. Further, the coloring power of the magnetic iron oxide particles can be lowered to result in insufficient image density in some cases.

[0172] On the other hand, if the magnetic iron oxide particles have an average particle size in excess of 0.3 μm, the weight per one particle is increased to increase the probability of exposure thereof to the toner particle surface due to a specific gravity difference with the binder during the production. Further, the wearing of the production apparatus can be promoted and the dispersion stability of a monomer composition containing the magnetic iron oxide particles is liable to become unstable.

[0173] Further, if particles of 0.1 μm or smaller exceed 40% by number of total particles (having particle sizes of 0.03 μm or larger), the magnetic iron oxide particles are liable to have a lower dispersibility because of an increased surface area, liable to form agglomerates in the toner to impair the toner chargeability, and are liable to have a lower coloring power. If the percentage is lowered to at most 30% by number, the difficulties are preferably alleviated.

[0174] Incidentally, magnetic iron oxide particles having particle sizes of below 0.03 μm receive little stress during the toner production so that the probability of exposure thereof to the toner particle surface is low. Further, even if such minute particles are exposed to the toner particle surface, they do not substantially function as leakage sites lowering the chargeability of the toner particles. Accordingly, the particles of 0.03-0.1 μm are noted herein, and the percentage by number thereof is suppressed to below a certain limit.

[0175] On the other hand, if particles of 0.3 μm or larger exceed 10% by number, the magnetic iron oxide particles are caused to have a lower coloring power, thus being liable to result in a lower image density. Further, as the number of magnetic iron oxide particles is decreased at an identical weight percentage, it becomes difficult statistically to have the magnetic iron oxide particles be present up to the proximity of the toner particle surface and distribute equal numbers of magnetic iron oxide particles to respective toner particles. This is undesirable. It is further preferred that the percentage be suppressed to at most 5% by number.

[0176] In the present invention, it is preferred that the magnetic iron oxide production conditions are adjusted so as to satisfy the above-mentioned conditions for the particle size distribution, or the produced magnetic iron oxide particles are used for the toner production after adjusting the particle size distribution as by pulverization and/or classification. The classification may suitably be performed by utilizing sedimentation as by a centrifuge or a thickener, or wet classification using, e.g., a cyclone.

[0177] The volume-average particle size and particle size distribution of iron oxide particles described herein are based on values measured in the following manner.

[0178] Sample particles in a sufficiently dispersed state are photographed at a magnification of 3×10 4 through a transmission electron microscope (TEM), and 100 particles each having a particle size of at least 0.03 μm selected at random in visual fields of the taken photographs are subjected to measurement of projection areas. The particle size (projection area-equivalent circle diameter (DCE)) of each particle is determined as a diameter of a circle having an area equal to the measured projection area of the particle. Based on the measured particle sizes of the 100 particles, a volume-average particle size (Dv=(Σ(nD CE 3 )/Σn) {fraction (1/30)} ), percentage by number of particles of 0.03 μm-0.1 μm and percentage by number of particles of 0.3 μm or larger are determined.

[0179] The volume-average particle size and particle size distribution of magnetic iron oxide particles dispersed within toner particles may be measured in the following manner.

[0180] Sample toner particles are sufficiently dispersed in a cold-setting epoxy resin, which is then hardened for 2 days at 40° C. The hardened product is sliced into thin flakes by a microtome. The thin flakes are observed through a TEM and photographic at magnification of 1×10 4 -4×10 4 . One hundred iron oxide particles of at least 0.03 μm in particle size selected at random in visual fields of the taken photographs are subjected to measurement of projection areas. From the projection areas of the 100 iron oxide particles, a volume-average particle size (projection area-equivalent circular diameter), percentage by number of particles of 0.03 μm-0.1 μm and percentage by number of particles of 0.3 μm or larger are determined similarly as the above.

[0181] The magnetic iron oxide particles may preferably have magnetic properties including a saturation magnetization of 10-200 Am 2 /kg as measured at a magnetic field of 795.8 kA/m, a residual magnetization of 1-100 Am 2 /kg, and a coercive force of 1-30 kA/m.

[0182] It is particularly preferred that the magnetic toner used in the present invention has a magnetization of 10-50 Am/kg at a magnetic field of 79.6 kA/m (1000 oersted).

[0183] The magnetization at a magnetic field of 79.6 mA/m is taken as a property of a magnetic toner in a magnetic field realized in an actual image forming apparatus, while the saturation magnetization is used as a parameter representing magnetic properties of magnetic iron oxide. The magnetic field acting on magnetic toners is most commercially available image fo