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    • 2. 发明授权
    • Wheel spin prevention system
    • 车轮防旋转系统
    • US4583611A
    • 1986-04-22
    • US645044
    • 1984-08-28
    • Rudiger FrankHerbert SchrammWerner KopperDieter Worner
    • Rudiger FrankHerbert SchrammWerner KopperDieter Worner
    • B60T8/72B60K28/16B60T8/175B60T8/66F02D29/02F16D66/00B60Q1/00B60K31/00
    • B60T8/175F16D2066/001
    • A versatile system for preventing spinning of driving wheels, especially for commercial road vehicles, is provided by a braking control system in which a logic system responds not only to positive slip (overdriving) of each driven wheel, but also to negative slip (overbraking) thereof and, likewise, not only to over-acceleration, but also to excessive deceleration of the driven wheels. The cycle of control is started by an over-acceleration signal and terminates by the timing-out of a control phase in which hydraulic brake pressure is reduced. Within a control cycle, brake pressure builds up for a driven wheel in response to the simultaneous occurrence of any one of the following four pairs of conditions at that wheel: (a) presence of over-acceleration and of negative slip; (b) presence of over-acceleration and of positive slip; (c) presence of over-acceleration and absence of negative slip, and (d) presence of over-deceleration and of positive slip. For purposes of braking, but not for purposes of reducing engine torque, when over-acceleration occurs at a first driving wheel at one side of the vehicle, a pseudo-positive-slip signal is generated for the driving wheel on the other side, but that pseudo-signal is suppressed if at the first driving wheel there appears a slip signal or an overdeceleration signal.
    • 一种用于防止驱动轮旋转的通用系统,特别是用于商业道路车辆的驱动轮,由制动控制系统提供,其中逻辑系统不仅响应每个从动轮的正滑移(过驱动),而且还响应于负滑动(过度制动) 并且同样地,不仅是过度加速,而且还导致从动轮的过度减速。 控制循环由过加速度信号开始,并且终止于液压制动压力降低的控制阶段的超时。 在控制周期内,响应于同时发生以下四对条件中的任何一个,轮对制动压力建立起来:(a)存在过加速度和负滑差; (b)存在过度加速和正滑移; (c)存在过度加速和没有负滑差,以及(d)存在过度减速和正滑移。 为了制动的目的,但是为了减少发动机扭矩,当在车辆的一侧的第一驱动轮处发生过加速时,对另一侧的驱动轮产生伪正滑信号,但是 如果在第一驱动轮处出现滑移信号或过减速信号,则该伪信号被抑制。
    • 4. 发明授权
    • Method and apparatus for turbidity measurement
    • 用于浊度测量的方法和装置
    • US08576399B2
    • 2013-11-05
    • US12736379
    • 2009-04-09
    • Edin AndelicRudiger Frank
    • Edin AndelicRudiger Frank
    • G01N21/00
    • G01N21/49G01N2021/4711G01N2021/4726
    • A method for turbidity measurement in a measured medium uses a turbidity sensor, which comprises at least a first and a second emitter and at least a first and a second detector. The first and the second emitters are excited one after the other to produce light signals directed into the measured medium; wherein each light signal travels along a first propagation path through the measured medium to the first detector, and is converted by such into a first detector signal; and travels along a second propagation path through the measured medium to the second detector, and is converted by such into a second detector signal. A turbidity value is ascertained based on the first and the second detector signals; wherein, by means of at least one additional detector, to which at least one of the light signals travels along an additional propagation path, an additional detector signal is ascertained, and, on the basis of the additional detector signal, the turbidity value is checked as regards its plausibility.
    • 在测量介质中用于浊度测量的方法使用浊度传感器,其包括至少第一和第二发射器以及至少第一和第二检测器。 第一和第二发射体一个接一个地被激发以产生被引导到测量介质中的光信号; 其中每个光信号沿着通过所述测量的介质的第一传播路径传播到所述第一检测器,并且被转换成第一检测器信号; 并且沿着第二传播路径行进通过所测量的介质到第二检测器,并且被这样转换成第二检测器信号。 基于第一和第二检测器信号确定浊度值; 其中,通过至少一个额外的检测器,光信号中的至少一个沿附加的传播路径行进,确定附加检测器信号,并且基于附加的检测器信号检查浊度值 关于它的合理性。
    • 5. 发明授权
    • Turbidity measuring device and a method for determing a concentration of a turbidity-causing material
    • 浊度测量装置和确定浊度物质浓度的方法
    • US08213016B2
    • 2012-07-03
    • US12805071
    • 2010-07-12
    • Andreas MullerRudiger Frank
    • Andreas MullerRudiger Frank
    • G01N21/00
    • G01N21/53G01N15/06G01N21/274G01N2015/0693G01N2201/061G01N2201/0662
    • A turbidity measuring device having a four-beam, alternating light arrangement for registering turbidity of a measured medium includes first and second light sources L1, L2; and first and second receivers R1, R2. The direct measuring paths extend from light sources Li, through a measured medium, to receivers Ri, and indirect measuring paths extend from light sources Li, through the measured medium, to second receivers Rj; wherein i≠j; wherein turbidity can be ascertained as a function of a quotient A/B by means of an evaluating circuit; wherein A and B are functions at least of signals registered via the direct or indirect measuring paths; wherein at least a first monitor signal, which depends on the first light source, enters into one of the two terms A or B; wherein the light reaches the monitor from the first light source without interaction with the measured medium; and wherein the monitor signal is added to at least one of the signals registered via the measuring paths and entering into the term A or B.
    • 具有用于记录测量介质的浊度的四光束交替光布置的浊度测量装置包括第一和第二光源L1,L2; 以及第一和第二接收器R1,R2。 直接测量路径从光源Li延伸通过测量介质到接收器Ri,并且间接测量路径从光源Li延伸通过测量的介质到第二接收器Rj; 其中i≠j; 其中可以通过评估电路将浊度确定为商A / B的函数; 其中A和B至少是经由直接或间接测量路径登记的信号的功能; 其中依赖于第一光源的至少第一监视信号进入两个项A或B中的一个; 其中所述光从所述第一光源到达所述监视器,而不与所述测量介质相互作用; 并且其中所述监视信号被添加到经由所述测量路径登记的信号中的至少一个并输入到所述术语A或B.
    • 7. 发明申请
    • Turbidity Measuring Device
    • 浊度测量装置
    • US20120022794A1
    • 2012-01-26
    • US13260398
    • 2010-03-15
    • Edin AndelicRudiger Frank
    • Edin AndelicRudiger Frank
    • G06F19/00
    • G01N21/49G01N2021/4711G01N2021/4726
    • A turbidity measuring device for determining the concentration Kj of a substance Sj in a medium includes measuring arrangements, in which the intensities of scattered light at different angles are registered and convertable into current values of at least a first measured variable M1 and a second measured variable M2, which have different dependences on the concentration Kj of a substance Sj (Mi(Kj)=fij(Kj)). The turbidity measuring device has stored for the measured variables Mi for a number of substances Sj calibration functions gij, with which, in each case, a concentration of a substance Sj is determinable (Kj=gij(Mi)). The turbidity measuring device further includes a computing unit, which is suitable for evaluating the ascertained concentration values gaj(Ma), gbj(Mb), wherein a≠b, for different substances Sj as regards their plausibility and so to identify a plausible substance Sj, or to check the plausibility of an earlier identified or predetermined substance Sj.
    • 用于确定介质中物质Sj的浓度Kj的浊度测量装置包括其中登记不同角度的散射光的强度并将其转换为至少第一测量变量M1和第二测量变量的电流值的测量装置 M2与物质Sj(Mi(Kj)= fij(Kj))的浓度Kj有不同的依赖关系。 浊度测量装置为多个物质Sj校准函数gij存储测量变量Mi,在每种情况下,可以确定物质Sj的浓度(Kj = gij(Mi))。 浊度测量装置还包括计算单元,其适用于评估确定的浓度值gaj(Ma),gbj(Mb),其中a≠b,对于不同物质Sj,关于它们的合理性,并且因此识别合理的物质Sj ,或检查较早确认或预定物质Sj的合理性。
    • 8. 发明申请
    • METHOD AND APPARATUS FOR TURBIDITY MEASUREMENT
    • 方法和装置的涡度测量
    • US20110043807A1
    • 2011-02-24
    • US12736379
    • 2009-04-09
    • Edin AndelicRudiger Frank
    • Edin AndelicRudiger Frank
    • G01N21/00
    • G01N21/49G01N2021/4711G01N2021/4726
    • A method for turbidity measurement in a measured medium uses a turbidity sensor, which comprises at least a first and a second emitter and at least a first and a second detector. The first and the second emitters are excited one after the other to produce light signals directed into the measured medium; wherein each light signal travels along a first propagation path through the measured medium to the first detector, and is converted by such into a first detector signal; and travels along a second propagation path through the measured medium to the second detector, and is converted by such into a second detector signal. A turbidity value is ascertained based on the first and the second detector signals; wherein, by means of at least one additional detector, to which at least one of the light signals travels along an additional propagation path, an additional detector signal is ascertained, and, on the basis of the additional detector signal, the turbidity value is checked as regards its plausibility.
    • 在测量介质中用于浊度测量的方法使用浊度传感器,其包括至少第一和第二发射器以及至少第一和第二检测器。 第一和第二发射体一个接一个地被激发以产生被引导到测量介质中的光信号; 其中每个光信号沿着通过所述测量的介质的第一传播路径传播到所述第一检测器,并且被转换成第一检测器信号; 并且沿着第二传播路径行进通过所测量的介质到第二检测器,并且被这样转换成第二检测器信号。 基于第一和第二检测器信号确定浊度值; 其中,通过至少一个附加检测器,光信号中的至少一个沿着附加传播路径传播,确定附加检测器信号,并且基于附加检测器信号检查浊度值 关于它的合理性。