• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    The invention can be used in the reproduction of halftone and stroke originals and ensures the accuracy of the formation of a control signal for adjusting the intensity distribution and aperture of scanning light beams (SLR). The method consists in that two photoconverters (AF) receive the SLR and convert them into an elo signal. The first AF converts SSL to email. the signal in case of successive movement of villages sat across the diaphragm of a given width and by the size of the diaphragm size. The intensity of the FMR is measured by converting the electronic signals of both FCs into digital codes and storing them. Then, the CCL mismatch signal is generated by reading the stored digital codes, respectively. CCL located at the same distance from each other, and comparing the digital codes of both W. When compared, the SRI normalizes the intensity of the el, the signal of the first OP relative to the signal of the second AF, which corresponds to the village according to the formula The max and min distribution signals are extracted and the control signal for adjusting the intensity distribution of the FCL is generated therefrom. In the second embodiment of the method, the FCL aperture is measured and the control signal of its adjustment is generated. 2 sp, f .ty, 2 sp. (Y) 00 sd D
    公开号:SU1395149A3
    申请号:SU833660901
    申请日:1983-11-04
    公开日:1988-05-07
    发明作者:Шульц-Хенниг Йорг
    申请人:Др.-Инж.Рудольф Хелль Гмбх (Фирма)；
    IPC主号:
    专利说明:


    sn
    The invention relates to a technique of reproduction, in particular the recording of halftone and stroke originals.
    The purpose of the invention is to increase the accuracy of the formation of the control signal to adjust the intensity distribution and the aperture of the scanning light rays.
    Figo shows a structural electrical circuit of the device for implementing the proposed method in the first embodiment; Fig 2 - the same, according to the second variant
    A device for generating a control signal for adjusting a parameter of scanning light beams in the first embodiment (FIG.) Comprises a first diaphragm photoconverter 1, a first signal amplifier 2, a first analog-digital converter 3, a first register 4, a second photo converter 5, a second amplifier 6 signals, second analog-to-digital converter 7, second register 8, 9 clock sensor, first –key 10, first memory block 11, first dividing unit 12, first differentiator 13 first adder 14, third register 15 first comparator 16, n The first counter 7, the second counter 18, the fourth register 19, the five register 20, the second key 21, the third key 22, the second memory block 23, the second division block 24, the first multiplication unit 25, the third memory block 26, the fourth block 27 , memory sixth register 28, unit 29 of forming and adjusting the light rays about
    The device for generating a control signal for adjusting the parameter of scanning light beams according to the second variant (FIG2) further comprises a discriminator 30, a second differentiator 31, a seventh register 32, a second comparator 33, a third counter 34, an eighth register 35, a third comparator 36, delay line 37, fifth memory block 38, fourth comparator 39, fourth key 40, fourth counter 41, ninth register 42, tenth register 43, second adder 44, eleventh register 45, second multiplication unit 46, third block 47 divisions, twelfth register 48 , fifth key 49, subtraction unit 50, fourth division block 51, thirteenth register 52, fourth memory block 53, third block 54
    multiplying, fourteenth register 55 and fifteenth register 56, digital-to-digital converter 57, block 58 for adjusting the aperture of light rays
    The method of the first embodiment is carried out as follows.
    Scanning light beams are received by photoconverters C and 5), which convert the scanning light beams into an electrical signal, measure the intensity of the scanning light beams, generate an error signal of the scanning light beams by comparing the electrical signal of the reference light beam with the conversion of scanning light glitches into an electrical signal is accomplished by generating an electrical signal, corresponding to when it is sequentially moved across a diaphragm of a given width and by an amount equal to the size of the diaphragm of the first phototransducer, and the second photovoltage transforms the light into an electric signal by generating an electric signal corresponding to the signal of the scanning light beam2, the first and the second transducer into a digital code, remember the digital codes of the first and second transducers, read The stored digital codes corresponding to the scanning light beams located at the same distance from one another compare the digital codes of the first and second phototransducer. by normalizing the intensity and electric signal of the first phototransducer relative to the electric signal of the second phototransducer; light rays are determined by the formula 1. .
    F (x + 1 - - 2) "): is: -i52
    22 A eg
    Lh
    + F, Cx
    U x
    ).
    where F (x) is the distribution function
    intensity in the scanning light rays;
    X is the shift direction of the scanning light rays; S - width of the diaphragm of the first
    the photoconverter j dx is the distance between the centers of the apertures of the scanning light rays;
    F (k) - measured signals of the intensity of the scanning light rays
    followed by the formation of a control signal to adjust the intensity distribution of the scanning light rays by extracting the maximum and minimum signals of the scanning light rays
    The scanning light beams are projected onto the optical input of the first diaphragm photovoltage 1 (Fig. 1), converted into an electrical signal that is fed through the first signal amplifier 2 to the first analog-to-digital converter 3, from which the digital signal is fed to the first register 4o. The second phototransducer 5 electrical signal is supplied to one of the inputs of the first dividing unit 12 through the second amplifier 6 of the signal connected in series, the second analog-to-digital converter 7 and the second register 8o The signal from the 9-clock sensor controls the first key 10, from which the signal goes through the first memory block 11 to the corresponding input of the first dividing unit 12. The amplitude value of the signal is divided in the first dividing unit 12 by the integral signal from the second register 8, s the output of the first block 12 of the division signal enters the third register 15 through a serially connected first differentiator 13 and the first adder 14, in which the inverse convolution operation is performed - deconvolu- tion. In this case, the differential ratio of the signal pr This signal is added to the previously defined signal from the third register 15 and after adding in the first adder 14, the signal enters again into the third register 15. The measured signal from the third register 15 enters the first comparator 16, which compares them with the stored in the fourth and fifth registers. 19 and 20 maximum and minimum amplitudes and with a shortage or increase of load again
    0
    The fourth 19 and second 20 registers are filled with new signals. The first 17 and second 18 counters, receiving count increments from the sensor of 9 cycles, load alternately the fourth and 19 second and 20 registers of the maximum and minimum signals, respectively, through the second 21 and third 22 keys and the second memory block 23, the signal from which is supplied to the second block 24 of the Split. The obtained private ratios are multiplied in the first block 25 by multiplying by the ones read in the second
    5, the memory block 26, the control signals, the read signals are input into the sixth register 28, from which output the signal is fed to the block 29 of shaping and adjusting the intensity of the light rays
    The method according to the second embodiment is carried out as follows.
    Scanning light rays are received by photoconverters, convert scanning light beams into an electrical signal, measure apertures of scanning light beams, generate an error signal of scanning light beams by comparing the electrical signal of the aperture of the scanning light beams relative to the electrical signal of the reference light beam aperture, while converting the scanning light light rays into an electrical signal is accomplished by generating an electrical signal corresponding to scanning light rays, with sequential movement across
    The Q diaphragms of a given width and by an amount equal to the size of the diaphragm and the first photovoltage transducer, and the second photovoltage transform the scanning light beams into an electrical signal by forming
    the electrical signal corresponding to the signal of the entire scanning light beam converts the electrical signals of the first and second photovoltaic cells into a digital code, memorizes the digital codes of the first and second photovoltaic cells, reads the memorized digital codes corresponding to the scanning light beams located at equal distance from one another in the scanning the light beam, compare the digital codes of the first and second photoconverters by rationing the intensity
    0
    B
    0
    five
    513951
    the electrical signal of the first photoconverter with respect to the intensity of the electrical signal of the second, the transducer, and the signal — the intensity distribution of the scanning light rays — is determined by the formula
    F, (,. I. 42) „ll5l ... J).
    OH
    2
    J W / S LH V
    + F, (x -),
    where F (x) is the distribution function
    intensity in the light beam;
    X is the direction of shift; S - width of the diaphragm of the first
    photoconverter; & x is the distance between the centers of the apertures of the scanning light rays of the signals; F (x) - the measured signals of the intensity of the scanning light rays, followed by extracting the maximum signal of the intensity distribution of the scanning light rays, form from the selected maximum signal, scanning the light beams, the threshold signal corresponding to the 4fonts of the scanning light rays, form a signal corresponding to the increment of the scatter nor when moving the scanning light beams along the first photo-converter with the diaphragm, by multiplying the memorized maximum signal and the intensity of the scanning light beams on the signal corresponding to the distance between the centers of the apertures skaniruyupschh light rays generated by comparing a signal corresponding to the increment distance when moving the scanning light rays of the diaphragm lane I ..
    with the threshold signal, the signals obtained from the comparison are memorized, they form a signal corresponding to the difference between the signals of the two neighboring scanning light rays by subtracting the memorized signal corresponding to the distance traveled by another scanning light through the diaphragm of the first photoconverter, form a control signal the luminosity of the scanning light rays by comparing the shapes
    ,
    :
    , - 0
    five
    20
    25
    30 35
    55 40
    45
    50
    496
    signal corresponding to the difference of the increments of the signals of both neighboring scanning light beams with a threshold signal
    The scanning light beams are projected onto the optical input of the first diaphragm photovoltage 1 and converted into an electrical signal, which is amplified by the first amplifier 2 of the signal, the output of which sends the signal to the first analog-to-digital converter 3, from the output of which the digital code is entered into the first register A controlled The signal is supplied from a 16 clock sensor to the first memory block 11, the output of which sends a signal. To the first differentiator 13, a differentiated signal is added to a specific signal in the adder. 14, from the output of which the signal is input to the third register 15, from the output of which the signal is input to the adder 14 and the comparator 36, from the output of which the signal reads the main signal stored in the seventh register 32 and reloads it, leaving the amplitudes unchanged in block 5 The value of the slope of the amplitude obtained in the first differentiator 31 is read in the discriminator 30 when the sign of the signal changes, the third counter 34 increments in the score. The state of the third counter is compared in the third comparator 36 with the seventh register 35 with the first and last maximum signals; the signal from the output of the third comparator 36 controls the Fourth key 40; this signal also resets the seventh register 32 to zero. Through the delay line 37, the signal from the output of the fourth key 40 comes through the series-connected second adder 44 and the third block 47 dividing into the tenth register 43 o In the second adder 44 and the second block 24 dividing the amplitude of the first and last partial light beam, the boundary value of the signal is obtained, which corresponds to the overlap point of two seconds. Substituting constituent beams. The signal from the tenth register 43 enters the fourth comparator 39, where it is compared with the amplitude signal from the fifth memory block 38. The same signal enters the fourth counter 41, from the output of which the signal enters the second multiplication unit 46, which multiplies the signal of the ninth register 42 o. From the second multiplication unit 46, the signal enters the eleventh register 45. The signal from the fourth comparator 39 arrives at the control the input of the fifth key 49. The signal from the eleventh register 45 through the fifth key 49 enters the twelfth register 48, the signal from which enters the subtractor 50. The differential value of the signal, equal to the first and last values of the path of the light beam, enters the fourth division block 51, where it is divided into a signal from the thirteenth register 52, the signal from the fourth division block 51 arrives at the third multiplication unit 54, where it is multiplied with the signal from the fourteenth register 55 through the fourth block of memory 53, the signal in which is selected by parameters determining the actual state of the signal of the aperture of the light beam (for example, by means of variable optics) to the signal from the third block The multiplication 54 is fed through the serially connected fifth register 56 and a digital-to-analog converter. 57 to block 58
    权利要求:
    Claims (1)
    [1]
    1. A method of forming a control signal for adjusting a parameter of scanning light rays, including receiving photo scanning light by the photoelectric converters, converting the scanned light rays into an electrical signal, measuring the intensity of the scanned light beams, generating an error signal of the scanning light beams by comparing the electrical signal of the intensity of the scanning light. ofifjocri light rays of a thermal electric signal of a reference light beam, characterized in that, in order to increase the accuracy of forming the control signal of adjusting the intensity distribution of the scanning light rays; the conversion of the scanning light rays into an electrical signal is carried out by generating an electrical signal corresponding to the scanned light beam when it is sequentially moved across a diaphragm of a given width and
    by a value equal to the size of the diaphragm of the first photoconverter, and the second photovoltage converter converts the scanning light beam into an electrical signal by generating an electrical signal corresponding to the signal intensity of the entire scanning light beam, convert the electrical signals of the first and second photovoltaic cells into a digital code, memorize the digital codes of the first and second second photoconverters, read the stored digital codes corresponding to the scanning light beams located on one at a different distance from each other, the digital codes of the first and second photoconverters are compared by normalizing the intensity of the electrical signal of the first photoconverter relative to. the electrical signal of the second photo converter; the intensity distribution of the scanning light beams are determined by the formula
    F, (x | - | J,
    Zl: 2 I-ll2i.ILA.52
    THEIR
    F, (x
    S 2.
    their
    ).
    where F, (x) is the distribution function
    intensity of scanning light rays; X is the shift direction of the scanning light rays; S - width of the diaphragm of the first
    photoconverter; dx - distance between centers
    scanning apertures; F, (x) - measured signals of the intensity of the scanning light rays,
    with the subsequent formation of a control signal for adjusting the distribution of the intensity of the scanning light rays by separating the maximum and minimum signals of the distribution of the intensity of the scanning light and light rays
    I.
    2, Method of forming a control signal for adjusting the parameter of rocks, dimming light rays, receiving the scanning light rays by photoconverters, converting the scanning light rays into electric 913
    a signal, measuring the aperture of the scanning light rays, generating an error signal of the scanning light rays by comparing the electrical signal of the aperture of the scanning light rays relative to the electrical signal of the aperture of the reference light beam, characterized in that, in order to improve the formation of the control signal for adjusting the aperture of the scanning light rays, conversion of scanning light rays into an electrical signal is done by generating an electrical signal a, corresponding to the scanning light beams, by successively moving across a diaphragm of a given width and equal to the size of the diaphragm of the first phototransducer, and the second photoelectric converter converts the scanning light beams into an electrical signal by generating an electric signal corresponding to the scanning light beam signal, signals of the first and second photovoltaic cells into a digital code, memorizing the digital codes of the first and second photovoltaic cells, read stored digital codes corresponding to scanning light beams located at the same distance from each other in the scanning light beam, compare the digital codes of the first and second photovoltaic converters by normalizing the intensity of the electrical signal of the first photoconverter relative to the electrical signal of the second photoconverter, and the signal The intensity distribution of the scanning light rays is determined by the formula
    F (I. - | 5) IIxl..A25U
    F -Gh - - -A2 „h
     I CH „9
    ABOUT
    5 0 5 o Q s
    five
    0
    where FJ (x) is a function of the intensity distribution in the light beam; X is the direction of the scan-shift.
    radiating rays; S - width of the diaphragm of the first
    photoconverter; Ah - distance between centers
    apertures scanning light. commodity rays; F (x) - measured signals of the intensity of the scanning light rays,
    with the subsequent selection of the maximum signal is distributed. the x-ray intensity of the scanning rays form from the selected maximum scanning signal; - the light rays a threshold signal corresponding to the extreme fronts of the scanning light rays form a signal corresponding to the increment of the distance when the scanning light rays move along the aperture of the first photoconverter by multiplying the memorized maximum intensity distribution signal light rays to a signal corresponding to the distance between the centers of the apertures of the scanning light they compare the generated signal corresponding to the increment of the distance when the scanning light travels through the diaphragm of the first photoconverter with the threshold signal, memorize the signals obtained when comparing, form a signal corresponding to the difference of the increments of the signals of two neighboring scanning light beams by subtracting the stored signal corresponding to the distance, the other scanned light beam travels through the diaphragm of the first photoconverter; a control signal is generated scanning aperture apertures comparing the generated signal corresponding to the difference of the increments of the signals of both adjacent scanning light beams with the threshold signal
    opch
    I s.
    I I I
    Jl
    29
    Fig, 1
    FIG. 2
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    引用文献:
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