Liquid electro-photographic (LEP) printing uses a special kind of ink to form images on paper and other print substrates. LEP inks include toner particles dispersed in a carrier liquid. Accordingly, LEP ink is sometimes called liquid toner. In LEP printing processes, an electrostatic pattern of the desired printed image is formed on a photoconductor. This latent image is developed into a visible image by applying a thin layer of LEP ink to the patterned photoconductor. Charged toner particles in the ink adhere to the electrostatic pattern on the photoconductor. The liquid ink image is transferred from the photoconductor to an intermediate transfer member (ITM) that is heated to transform the liquid ink to a molten toner layer that is then pressed on to the print substrate.
The same part numbers designate the same or similar parts throughout the figures.
HP Indigo® commercial and industrial digital printing presses utilize Electrolnk® and other LEP inks developed by Hewlett-Packard Company in a thermal offset transfer process to print high quality images on a wide range of printing substrates. In one example LEP printing process, the ink image transferred from the photoconductor to the intermediate member (ITM) is about 5 μm thick with 20% toner, while the ink image transferred from the ITM to the print substrate is about 1 μm thick and nearly 100% toner. This change in thickness and concentration is achieved by heating the ITM to raise the temperature of the ink until the toner particles change phase and the carrier evaporates, transforming the liquid ink into a tacky layer of toner. In this transformed state, the toner layer adheres to the print substrate immediately on contact.
Infrared lamps are commonly used to heat the ITM from both the inside and the outside to maintain the ITM at the desired transformation temperature. Currently, the ink transformation process on the ITM takes hundreds of milliseconds and its environment sinks large amounts of heat, impeding faster printing and causing significant thermal losses.
It has been discovered that transferring the liquid ink image to an unheated ITM at ambient temperature and then rapidly raising the temperature of the ITM along a narrow band transforms the ink as desired and allows the ink transformation to occur very fast and with much smaller heat losses compared to current transfer processes. Accordingly, new ITM transfer systems and processes have been developed for fast and focused heating of the ITM. In one example, an array of lasers is arranged to direct laser beams across the surface of the ITM carrying the liquid ink image with enough power to almost instantly transform the liquid ink from a suspension of separate toner particles to a thin molten toner layer by eliminating most of the liquid carrier and melting the toner. For example, it is expected that laser beams each having an energy density at least 5 mJ/mm2 will be sufficient for many LEP printing applications to make the transformation in less than 20 ms, compared to 300 ms or more in current transfer processes.
In one example of a new LEP printing process, the inked image developed on the photoconductor is transferred to an unheated part of the ITM. The ITM carrying the inked image is heated rapidly from an ambient temperature, usually 20° C. to 30° C., to a peak temperature, typically 180° C. to 220° C., in less than 10 ms to transform the inked image to a thin molten toner layer which contains mostly toner (almost without liquid carrier). The layer is then released to the print substrate. “Unheated” in this context means not actively heated. The ITM may retain heat and, thus, the ambient temperature of unheated parts of ITM may be warmer than the surrounding operating environment.
A processor readable medium with instructions for fast and focused heating of the ITM may be implemented, for example, in the controller of the LEP printer.
The examples shown in the figures and described herein illustrate but do not limit the scope of the patent, which is defined in the Claims following this Description.
As used in this document, a “laser” means a device that produces a beam of coherent light; “light” means electromagnetic radiation of any wavelength; and “LEP ink” means a liquid that includes toner particles in a carrier liquid suitable for electro-photographic printing.
In the example shown, memory 18 includes a processor readable medium 20 with instructions 22 to control ITM heating. A processor readable medium 20 is any non-transitory tangible medium that can embody, contain, store, or maintain instructions for use by a processor 16. Processor readable media include, for example, electronic, magnetic, optical, electromagnetic, or semiconductor media. More specific examples of suitable processor readable media include a hard drive, a random access memory (RAM), a read-only memory (ROM), memory cards and sticks and other portable storage devices. Heating instructions 22 may be embodied, for example, in software, firmware, and/or hardware.
Although print engine 12 and controller 14 are shown in different blocks in
In one example printing process for an LEP printer such as that shown in
The liquid ink image is transferred from photoconductor 24 to an intermediate transfer member (ITM) 32 and then from ITM 32 to sheets or a web of paper or other print substrate 34 as it passes between ITM 32 and a pressure roller 36. A lamp or other suitable discharging device 37 removes residual charge from photoconductor 24 and ink residue is removed at a cleaning station 38 in preparation for developing the next ink image.
Print engine 12 also includes a heater 40 to heat ITM 32. As described in more detail below, ITM heater 40 is configured to rapidly heat a small part of ITM 32 to a temperature needed to transform the liquid ink image into a tacky layer of toner for transfer to print substrate 34. Heater 40 may be housed in an enclosure 42 to contain and evacuate vapors produced during heating.
It was discovered that transferring the liquid ink image to an unheated ITM blanket and rapidly raising the temperature of the surface of the blanket along a narrow band transforms the ink as desired and allows the ink transformation to occur very fast and with much smaller heat losses compared to the current transfer processes. Heat transfer calculations show, and testing confirms, that the time to transform the ink image from a thicker, liquid layer 54 received from the photoconductor to a thinner, tacky layer 58 transferred to the print substrate can be shortened by an order of magnitude—from hundreds of milliseconds in the current transfer process to tens of milliseconds (or less) in the new transfer process. The ink is heated by conduction from the outer part of ITM blanket 44, which has a high absorption coefficient at the laser wavelengths. The bulk of ITM 32 stays relatively cool so the energy used to maintain the transformation drops substantially compared to the current process and energy losses to the environment are small. As a result, significant energy savings can be realized even with the relatively low efficiency of existing laser diodes.
In one specific example, ITM heater 40 is configured as a single row of VCSELs 48 (Vertical Cavity Surface-Emitting Lasers) emitting light beams 52 at a wavelength of 980 nm. The VCSEL module has a maximum output power of 6.4 W/mm of printing width with a power density up to 160 W/mm2. nAn ITM blanket 44 currently used in LEP printers absorbs light across a wide band of wavelengths and, thus, may be used with a VCSEL type heater 40 in this example. The ITM was exposed to beams 52 for 40 μs with the post-heating time varied between 20 ms-30 ms (the time between exposure to beams 52 and contact with print substrate 34 at nip 59). Other suitable configurations are possible. For one example, other types of lasers or even non-laser, focused heat sources may be used for heater 40. The power of each laser 48 and/or the size of the array may be varied to achieve the desired heating characteristics. Also, the wavelength of light beams 52 emitted by lasers 48 and the absorption characteristics of ITM blanket 44 may be tuned to one another to help improve both the effectiveness and the efficiency of heater 40.
While the characteristics of heater 40 will vary depending on the particular printing application, it is expected that a heater 40 delivering a heat energy greater than 3 mJ/mm2 will be adequate for the desired ink transformation. Printing tests indicate that 5 mJ/mm2 (or more) per square meter of ITM blanket should be sufficient in many LEP ITM heating implementations for effective ink transformation to maintain good print quality. For example, it is expected that focused heating at an energy density greater than 3 mJ/mm2 of printing area will be sufficient in many LEP printing processes to raise the temperature of the exterior surface of an ITM blanket 150° C. or more in less than 10 ms (much less under some operating conditions—40 μms in the example noted above). Shorter post-heating times reduce the power used for effective ink transformation. Post-heating times may be reduced by shortening the distance between heater 40 and nip 59 or speeding up the ITM. Additional energy savings may be realized by turning off heater 40 when there is no ink on blanket 44 at band 56, for example at the seam area of the blanket.
“A” and “an” as used in the Claims means one or more.
As noted at the beginning of this Description, the examples shown in the figures and described above illustrate but do not limit the scope of the patent. Other examples are possible. Therefore, the foregoing description should not be construed to limit the scope of the patent, which is defined in the following Claims.
This is a continuation of U.S. patent application Ser. No. 15/545,913 filed Jul. 24, 2017 which is itself a Section 371 national stage of international patent application no. PCT/EP2015/054761 filed Mar. 6, 2015.
Number | Date | Country | |
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Parent | 15545913 | Jul 2017 | US |
Child | 16193377 | US |