• 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:
    1. A method of determining the density of a fibre bundle wherein the fibre bundle is brought to a defined cross-section, characterised in that a value corresponding to the modulus of elasticity is measured ; and in that the density of the fibre bundle is derived therefrom.
    公开号:SU1431689A3
    申请号:SU823461103
    申请日:1982-07-09
    公开日:1988-10-15
    发明作者:Феликс Эрнст
    申请人:Целльвегер Устер Аг (Фирма)；
    IPC主号:
    专利说明:

    ABOUT)
    WITH
    s
    This invention relates to the textile industry.
    The purpose of the invention n increasing measurement accuracy, 5
    Fig. 1 shows a diagram explaining the principle of operation of the device; Fig. 2 shows the load-strain profile; on FIG. 3 - the equivalent circuit of the device; FIG. 4 is the end structure of the device; FIG. FIG. 3 is a temporal pattern of sound wave propagation; FIG. a device embodiment; Fig. 7 shows the measuring circuit of the device; 8 to 15, the measuring part of the device, cross section; FIG. 9 is the same; an embodiment; figure 10 is the same cross section; Fig. II shows a device, a transverse section; in fig. 20
    12 - the device case, section. The device comprises a housing 1 in which a passage for the passage of fiber 2 is complete, having a measuring part of a constant cross section 25 NIN in which the source 3 and the receiver 4 of mechanical oscillations are located.
    The receiver and the radiation source can be combined in one block 30 5 located on one wall of the measuring part of the channel, on the other wall of which screen 6 (membrane) is placed. The screen 6 may be a membrane, which is the wall of the measuring part of the channel.
    In the general case, the receiver 4 is connected by its output to the input of the phase meter: 7, the output of which is connected to the input of: the generator 8 of the source 3 mechanical | Q kih fluctuations. The phase meter is also a device output recorder. Source 3 and receiver 4 are scored 9 in the direction 10 of product movement.
    45
    The source 3 and the receiver 4 can be made in the form of piezocrystals 11 and 12 connected to the membrane b through a hub 13. The connection of the piezocrystals with external devices (not shown) is carried out using a wire 14 housed in a housing. The crystals are pre-compressed with screw 15, positions 16 and 17 in fig. 5 show pulses, position 18 shows the load (fig. 3), and position 19 shows the surface of the source 3 and the receiver 4. mechanical oscillations.
    The device works as follows.
    As a rule, a textile fiber product, such as a tape, consists of a large number of fibers separated by air gaps. If you place the product in the directional funnel of the carding machine, the fibers themselves occupy 20% in it (the rest is air). If the fibers are compressed by force P, the fibers are deformed (compressed). The dependence P f (), where is the deformation of the fibers, is presented in FIG. The elastic modulus E of a fiber is defined in the usual way: E tgei. Based on the foregoing, a fibrous product placed in the measuring part of a channel made in housing 1 can be considered as a mechanical oscillatory system, for example. Exciting spring (fiber) oscillations by acting on it with a load (mass) 18, it is possible to determine the spring modulus (fibers) by the resonant frequency of the system: spring (fiber) - mass 18, Thus, if the density (quantity) of fibers in the section changes of the measuring part, then the value of E will change, and, consequently, the resonant frequency of the oscillating system.
    It is known that the speed from the sound in the medium is determined by the formula -1 Е
    where D is the density of the medium.
    If using the source 3 of mechanical oscillations to act on the fibrous product 2, then these lines will be perceived by the receiver 4. Oscillations will propagate with a certain speed c. Impulse 16 (FIG. 3) from the output of source 3 will reach receiver 4 after some time & . The value of t is determined by the density D of the fiber product. Thus, with an increase in D (increases with), t decreases and vice versa.
    You can combine the source 3 and receiver 4 in the form of a block 3 (6). In this case, the probe pulse passes through the product twice due to the screen 6, which is the wall of the measuring channel.
    According to the switching circuit of the device shown in Fig. 7, the output signal of the device is a resonant frequency fixed by a phase meter 7. The resonant frequency in the device is achieved by feedback, organized by connecting the output of receiver 4 to the input of the phase meter 7, which changes the frequency of the generator 8 nick 3 mechanical vibrations. Such an insertion circuit is the most robust.
    For the convenience of passing the product, it is advisable to carry out the surfaces of the source 3 and 4 with bevels 9 in the direction 10 of the movement of the product. It is also preferable that the active surfaces 19 of the source 3 and the receiver 4 are flat and parallel to each other. The measuring part of the device can be round, rectangular, oval and. etc.
    FIG. 11 shows the placement of the source 3 and the receiver 4 directly in the walls of the forming funnel used, for example, on a carding machine.
    The source 3 and the receiver 4 can be filled in the form of piezocrystals 11 and 12 mounted one above the other and protected from external influences by the screen (membrane) 6. To increase the sensitivity of the measurement, a capacitor 13 is used. 14.
    权利要求:
    Claims (6)
    [1]
    1. An apparatus for determining the mass of a fibrous product, comprising
    ./ХХ ХХХХУ / ./
    The product guide, the source and receiver of mechanical vibrations and the recorder, characterized in that, in order to improve the measurement accuracy, the product guide consists of a body in which a channel having a measuring part with a constant cross section is made in the direction of movement of the fiber product placed the source and receiver of mechanical oscillations, and the recorder is made in the form of a phase meter, the input of which is connected to the output of the receiver of mechanical oscillations, and the output to the input of the source of mechanical oscillations their oscillations.
    [2]
    2. The device according to Clause I., of which is that the source and receiver of mechanical vibrations are placed on opposite sides of the direction of movement of the product.
    [3]
    3. A device according to Claims 1 and 2, characterized in that the surfaces of the source and receiver of mechanical vibrations facing one another of the bevels have bevels in the direction of movement of the product,
    [4]
    4. The device according to claim 1, characterized in that the source and receiver of mechanical oscillations are placed on one wall of the measuring part of the channel, and the opposite wall is provided with a screen.
    [5]
    5. The device according to PP.1-4, t - characterized by the fact that the source and receiver of mechanical vibrations are made in the form of piezocrystals.
    [6]
    6. The device according to PP.1,4 and 5, based on the fact that the screen is made in the form of a membrane rigidly connected with piezo-cristaps.
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    Editor L. Veselovska
    Compiled by B. Kisin Tehred A. Kravchuk
    Order 5358/59
    Circulation 847
    VNIIPI USSR State Committee
    for inventions and discoveries 113035, Moscow, Zh-35, Raushsk nab. 4/5,
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    Corrector C, Cherni
    Subscription
    类似技术:
    公开号 | 公开日 | 专利标题
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    US4716764A|1988-01-05|Method and device for determining the cross-section of elongated objects using a sound field
    US4875373A|1989-10-24|Temperature compensated fiber optic vibration sensor
    US2779191A|1957-01-29|Frequency discriminator employing multiply resonant piezoelectric vibrator
    SU1534408A1|1990-01-07|Fiber-optic sensor of vibration accelerations
    SU1254384A1|1986-08-30|Device for determining the breaking load of cotton fibre,paritcularly,in piles
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    SU632972A1|1978-11-15|Mechanical oscillation-to-light wave converter
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    同族专利:
    公开号 | 公开日
    DE3264649D1|1985-08-14|
    CS536482A2|1991-11-12|
    AU562474B2|1987-06-11|
    IN157380B|1986-03-15|
    EP0069833A1|1983-01-19|
    ES8401253A1|1983-12-01|
    EP0069833B1|1985-07-10|
    JPS5810652A|1983-01-21|
    AU8591782A|1983-01-20|
    JPH0153420B2|1989-11-14|
    ES513903A0|1983-12-01|
    CH651669A5|1985-09-30|
    CA1182899A|1985-02-19|
    引用文献:
    公开号 | 申请日 | 公开日 | 申请人 | 专利标题
    US3599543A|1964-12-02|1971-08-17|Stothert & Pitt Ltd|Vibratory machines|
    DE2167255C3|1970-08-20|1982-03-11|Deutsche Itt Industries Gmbh, 7800 Freiburg|Vibration densitometer|
    JPS4924180A|1972-06-03|1974-03-04|
    AT331539B|1972-10-25|1976-08-25|Kratky Otto Dr Dr E H|DEVICE FOR MEASURING DENSITY|
    JPS5723383B2|1974-06-27|1982-05-18|
    CH635373A5|1979-04-06|1983-03-31|Zellweger Uster Ag|MEASURING AND CONTROL DEVICE WITH A MEASURING FUNNEL FOR DETERMINING THE PULLING FORCE OF FIBER TAPES.|DE3237357C2|1982-01-18|1985-12-19|Zellweger Uster Ag, Uster|Device for measuring characteristic features of fiber material|
    CH656960A5|1982-02-19|1986-07-31|Zellweger Uster Ag|DEVICE FOR DETERMINING THE AMOUNT OF SUBSTANCE OR DENSITY OF FIBER TAPES, IN PARTICULAR THE SUBSTANCE CROSS SECTION OF FIBER TAPES.|
    CH668833A5|1986-01-16|1989-01-31|Zellweger Uster Ag|DEVICE FOR MEASURING AND / OR COMPARISONING THE TAPE THICKNESS OF FIBER TAPES.|
    US4766647A|1987-04-10|1988-08-30|Spinlab Partners, Ltd.|Apparatus and method for measuring a property of a continuous strand of fibrous materials|
    JPH0913237A|1995-06-29|1997-01-14|Zellweger Luwa Ag|Apparatus for obtaining thickness or unevenness of sliver|
    法律状态:
    优先权:
    申请号 | 申请日 | 专利标题
    CH457381A|CH651669A5|1981-07-13|1981-07-13|METHOD AND DEVICE FOR DETERMINING THE SUBSTANCE QUANTITY OR DENSITY OF FIBER QUANTITIES, IN PARTICULAR THE SUBSTANCE CROSS-SECTION OF FIBER TAPES.|
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