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    • 2. 发明申请
    • COMPENSATING TURBIDITY MEASURING DEVICE
    • 补偿浊度测量装置
    • WO2017173020A1
    • 2017-10-05
    • PCT/US2017/024900
    • 2017-03-30
    • TINTOMETER GMBHPALUMBO, Perry
    • PALUMBO, Perry
    • G01J1/00G01J1/16G01N11/02G01N21/00G01N21/01
    • Embodiments of the present invention can be implemented to (i) verify that a liquid within a turbidity measuring device during an assay process is of the same origin of that upon which the assay was performed, (ii) verify a flow through the turbidity measuring device including, but not limited to, a turbidimeter, a nephelometer, a fluorimeter, or the like, and (iii) enact an alteration to measurement step(s) and/or determination step(s) of an assay process in correlation with one or more variables associated with the liquid sample including, but not limited to, flow rate, temperature, and pressure to reduce a standard error of the assay.
    • 可以实施本发明的实施方式以(i)验证测定过程期间浊度测量装置内的液体与进行测定的相同来源,(ii) 验证通过浊度测量装置的流量,所述浊度测量装置包括但不限于浊度计,浊度计,荧光计等,并且(iii)实施对(一个或多个)测量步骤和/或(多个)测量步骤的 与与液体样品相关的一个或多个变量相关的测定过程,包括但不限于流速,温度和压力,以减少测定的标准误差。
    • 5. 发明申请
    • ANNULAR OPTICAL DEVICE
    • 环形光学器件
    • WO2012018717A2
    • 2012-02-09
    • PCT/US2011046105
    • 2011-08-01
    • HACH COPALUMBO PERRY A
    • PALUMBO PERRY A
    • G01N21/01G01N21/47
    • G02B19/0076G01N15/06G01N21/01G01N21/53G01N33/18G01N2015/0693G01N2201/064G02B3/04G02B5/001G02B13/18G02B19/0028G02B19/008G02B26/0808G02B2003/0093Y10T29/49826
    • An annular optical device (100) includes an annular meso-optic (1) including an annulus (11) centered about an axis of revolution (A) and a secondary optical structure (2) substantially coaxial within the annulus (11). The secondary optical structure (2) and the annular meso-optic (1) are separated by a media (12) including a media refractive index that is lower than the refractive index of the secondary optical structure. The secondary optical structure (2) holds a specimen to be radiated by impinging electromagnetic radiation. Scattered radiation from the secondary optical structure (2) and within the annulus (11) of the annular meso-optic (1) is allowed into the annular meso-optic (1) if an angle of incidence of the scattered radiation exceeds a predetermined incidence threshold. The annular meso-optic (1) re-directs the scattered radiation to comprise re-directed radiation that is substantially parallel to the axis of revolution (A).
    • 环形光学装置(100)包括环形介质光学器件(1),其包括以旋转轴线(A)为中心的环形空间(11)和在所述环形空间(11)内基本同轴的次级光学结构(2)。 二次光学结构(2)和环形中视镜(1)由介质折射率低于第二光学结构的折射率的介质(12)分开。 二次光学结构(2)通过撞击电磁辐射而保持待辐射的样本。 如果散射辐射的入射角超过预定的入射角,则允许来自环形介质光学器件(1)的二次光学结构(2)和环形空间(11)内的散射辐射进入环形中视镜(1) 阈。 环形介质光学器件(1)重新引导散射辐射,以包括基本上平行于旋转轴线(A)的重新定向的辐射。
    • 6. 发明申请
    • MESO-OPTIC DEVICE
    • WO2011031730A1
    • 2011-03-17
    • PCT/US2010/048091
    • 2010-09-08
    • HACH COMPANYPALUMBO, Perry, A.
    • PALUMBO, Perry, A.
    • G02B5/00G02B13/06G02B17/08G02B17/06
    • G02B5/001G02B13/06G02B19/0028G02B19/008
    • A meso-optic device (1) includes a substantially annular meso-optic body (100) including an axis of revolution (2), a divergent conic optical surface (112) substantially coaxial with the axis of revolution (2), with the divergent conic optical surface (112) configured to receive electromagnetic radiation propagating along an optical axis (3) from an impingent direction, wherein the optical axis (3) is coincident with or intersects the axis of revolution (2), and with the divergent conic optical surface (112) configured to divergently re-direct the electromagnetic radiation away from the axis of revolution (2), and a convergent conic optical surface (114) substantially coaxial with the axis of revolution (2), with the convergent conic optical surface (114) configured to receive the electromagnetic radiation divergently re-directed by the divergent conic optical surface (112) and with the convergent conic optical surface (114) configured to convergently re-direct the electromagnetic radiation toward the axis of revolution (2).
    • 中视光学装置(1)包括基本上环形的中等光学主体(100),其包括旋转轴线(2),与旋转轴线(2)基本同轴的发散锥形光学表面(112),发散的 锥形光学表面(112),被配置为接收沿着光轴(3)从碰撞方向传播的电磁辐射,其中所述光轴(3)与所述旋转轴线(2)重合或相交,并且与所述发散锥形光学 配置成将电磁辐射远离旋转轴线(2)发散的表面(112)和与旋转轴线(2)基本上同轴的会聚锥形光学表面(114)与会聚锥形光学表面 114),其被配置为接收由发散锥形光学表面(112)发散地重新引导的电磁辐射,并且会聚的锥形光学表面(114)被配置成会聚地重新引导电磁辐射 朝向革命轴线(2)。
    • 8. 发明申请
    • STANDARD MEDIA SUSPENSION BODY, OPTICAL PARTICULATE MEASUREMENT INSTRUMENT, AND VERIFICATION METHOD FOR AN OPTICAL PARTICULATE MEASUREMENT INSTRUMENT
    • 标准介质悬挂体,光学测量仪器和光学测量仪器的验证方法
    • WO2009035894A2
    • 2009-03-19
    • PCT/US2008075188
    • 2008-09-04
    • HACH COPALUMBO PERRY A
    • PALUMBO PERRY A
    • G01N21/4785G01N21/278
    • A standard media suspension body (150) for verification of an optical particulate measurement instrument and configured to be at least partially immersed in a sample fluid is provided according to the invention. The body (150) includes a substantially solid outer surface including a first end (151) and a second end (152) disposed along an axis of illumination A and at least one outer surface (153). The first end (151) is configured to admit impinging light. The suspension body further includes an inner volume. At least a portion of the inner volume includes a substantially suspended light scattering material (155) that is configured to scatter a predetermined quantum of the admitted light. The suspension body (150) further includes an end cap (156) formed on the second end (152) and comprising a light absorbing material. Light exiting the second end (152) is substantially absorbed by the end cap (156).
    • 根据本发明提供了用于验证光学颗粒测量仪器并被配置为至少部分地浸入样品流体中的标准介质悬架体(150)。 主体(150)包括基本上实心的外表面,其包括沿着照明轴线A和至少一个外表面(153)设置的第一端(151)和第二端(152)。 第一端(151)被配置为允许入射光。 悬架体还包括内部容积。 内部体积的至少一部分包括基本上悬浮的光散射材料(155),其被配置为散射预定量的入射光。 悬挂体(150)还包括形成在第二端(152)上并包括光吸收材料的端盖(156)。 离开第二端(152)的光基本上被端盖(156)吸收。