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    • 2. 发明申请
    • Rate limiting and balancing control system for dual independent camshaft phasing
    • 双独立凸轮轴定相的限速和平衡控制系统
    • US20080230022A1
    • 2008-09-25
    • US11725768
    • 2007-03-20
    • Daniel L. McKayJames P. Waters
    • Daniel L. McKayJames P. Waters
    • F01L1/34
    • F02D13/00F01L1/053F01L1/185F01L1/2405F01L1/3442F01L2001/34496F01L2800/00Y02T10/18
    • A method for controlling dual independent camshaft phasers in an internal combustion engine. The method has three basic steps: a) first, determining if rate balancing between the two phasers is required; b) second, determining the optimal rate balancing commands; and c) third, applying the determined rate balancing commands to the appropriate phaser(s). In determining the rate balancing commands, there are three possible phaser options: the intake phaser requires priority; the exhaust phaser requires priority; or neither phaser requires priority. Lookup tables are stored in the engine controller for each option. When either phaser has priority, the other phaser is actuated after a delay based upon the position error of the priority phaser, generally at a lower phase rate. When neither phaser has priority, both phasers are actuated at a rate consistent with oil-delivery capabilities of the engine.
    • 一种用于控制内燃机中的双独立凸轮轴相移器的方法。 该方法有三个基本步骤:a)首先确定两个相位器之间的速率平衡是否需要; b)第二,确定最佳速率平衡命令; 和c)第三,将确定的速率均衡命令应用于适当的移相器。 在确定速率平衡命令时,有三种可能的移相器选项:摄像移相器需要优先; 排气移相器需要优先; 或者两者都不需要优先。 每个选项都会在引擎控制器中存储查找表。 当任一移相器具有优先权时,基于优先移相器的位置误差在延迟之后,另一个移相器通常以较低的相位速率被致动。 当两个移相器都不具有优先权时,两个相位器都以与发动机输油能力一致的速率启动。
    • 3. 发明授权
    • Light injector/extractor for multiple optical fibers
    • 多个光纤的注射器/提取器
    • US06665469B1
    • 2003-12-16
    • US10038396
    • 2002-01-02
    • Kenneth R. SchrollJames P. WatersJanet Armstrong
    • Kenneth R. SchrollJames P. WatersJanet Armstrong
    • G02B626
    • G02B6/2852
    • A device for injecting light from one of a first group of optical fibers into a corresponding one of a second group of optical fibers includes a holder for locating each of the fibers in the first and second groups, a clamp for securing fibers in the second group to the holder, and a depressor for laterally displacing each of the fibers in the second group, thus forming a bend in each of the fibers in the second group. The maximum curvature in the bend occurs where the fibers in the second group exit the clamp. Light is injected from fibers in the first group into corresponding fibers in the second group at the point of maximum curvature. An optical gel may be used to used to promote optical coupling between fibers in the first group and fibers in the second group. The optical fibers in the second group may include a lens for focusing the light to be injected. The device can function in reverse to extract light from fibers in the second group into fibers in the first group.
    • 用于将光从第一组光纤中的一个注入到第二组光纤中的对应的一个光纤的装置包括用于定位第一和第二组中的每个光纤的保持器,用于固定第二组中的光纤的夹具 以及用于横向移位第二组中的每个纤维的抑制器,从而在第二组中的每个纤维中形成弯曲。 弯曲的最大曲率发生在第二组中的纤维离开夹具的地方。 光在第一组中的纤维从最大曲率点的第二组中的相应纤维中注入。 可以使用光学凝胶来促进第一组中的纤维与第二组中的纤维之间的光学偶联。 第二组中的光纤可以包括用于聚焦待注入的光的透镜。 该装置可以相反地工作,将第二组中的纤维的光从第一组中提取成纤维。
    • 5. 发明授权
    • Noncontact optical gauging system
    • 非接触光学测量系统
    • US4299491A
    • 1981-11-10
    • US102310
    • 1979-12-11
    • James P. WatersRobert K. Thornton
    • James P. WatersRobert K. Thornton
    • G01B11/24
    • G01B11/24
    • A laser beam is focused to a spot on the surface of an object whose contour is to be measured. The spot is projected from the surface onto a detector by a reciprocating mirror which scans the spot across the detector. The detector produces two output signals consisting of sequential pulses at the frequency scan. The relative duration of these pulses or duty cycle reflects the change in contour dimension with respect to the scan centerline or mid point that corresponds to the base or zero dimension of the contour surface. The duty cycle is utilized to compute the change in contour dimension and to move the optics in such a way as to allow the spot to be continually scanned across the detector. The movement of the optics is made whenever there is a certain contour dimension change and by correlating the movement in the position of the optics and the instantaneous computed contour change reflected in the scan, the actual contour dimension is obtained.
    • 激光束被聚焦到要测量其轮廓的物体的表面上的点上。 该点通过往复式反射镜从表面投射到检测器上,该往复镜扫描检测器上的斑点。 检测器产生两个输出信号,由频率扫描的顺序脉冲组成。 这些脉冲或占空比的相对持续时间反映了轮廓尺寸相对于对应于轮廓表面的基础或零度尺寸的扫描中心线或中点的变化。 占空比用于计算轮廓尺寸的变化,并以这样一种方式移动光学元件,使斑点能够跨过检测器连续扫描。 只要存在一定的轮廓尺寸变化并且通过将光学器件的位置的移动与在扫描中反映的瞬时计算的轮廓变化相关联,则获得光学元件的运动,获得实际轮廓尺寸。
    • 7. 发明授权
    • System and method for performing dispersion compensation
    • 进行色散补偿的系统和方法
    • US07295738B2
    • 2007-11-13
    • US11008995
    • 2004-12-13
    • James P. Waters
    • James P. Waters
    • G02B6/28G02B6/26H04J14/02
    • G02B6/2932G02B6/29322G02B6/29394G02B6/29395H04B10/2519
    • An exemplary embodiment of the present invention includes an optical circulator. The circulator may have, for example, a first port, a second port, and a third port. The first port may be configured to introduce light into the optical circulator. The system may also include a tunable fiber filter Bragg grating connected to the second port of the circulator and a tunable dispersion-compensating fiber Bragg grating connected to the third port of the optical circulator. The tunable dispersion compensating fiber Bragg grating and the tunable fiber filter Bragg grating may be configured to be tuned by a single actuator. This tuning may be either compression or strain tuning.
    • 本发明的示例性实施例包括光循环器。 循环器可以具有例如第一端口,第二端口和第三端口。 第一端口可以被配置为将光引入到光循环器中。 该系统还可以包括连接到环行器的第二端口的可调谐光纤滤波器布拉格光栅和连接到光循环器的第三端口的可调色散补偿光纤布拉格光栅。 可调谐色散补偿光纤布拉格光栅和可调谐光纤滤波器布拉格光栅可以被配置为由单个致动器调谐。 该调谐可以是压缩或应变调谐。
    • 9. 发明授权
    • Method of and arrangement for measuring vibrations
    • 测量振动的方法和装置
    • US4892406A
    • 1990-01-09
    • US142889
    • 1988-01-11
    • James P. Waters
    • James P. Waters
    • G01B11/30G01B9/02G01B11/00G01D5/26G01H9/00
    • G01D5/268G01H9/00
    • The movement of a predetermined zone of a surface of a vibrating object is measured by separating a laser beam having a predetermined coherence length into a probe beam and a reference beam. The reference beam is then delayed relative to the probe beam by a predetermined time interval sufficient for the probe beam to travel through a predetermined distance at least corresponding to the coherence length, before being combined with the probe beam to form a combination beam. The combination beam is then subdivided into a plurality of substantially equal component beams each of which is conducted along a separate path to a location spaced from the predetermined zone substantially by one-half of the distance traveled by light in the predetermined time interval between the above location and the predetermined zone. A predetermined portion of each component beam is reflected at the respective location back into the respective path, while the remainder of each component beam is directed to the predetermined zone for return therefrom at least predominantly back toward the respective location and into the respective path with attendant coherent interference of the returned probe beam part with the reflected reference beam part of the same component beam. The return light beam are demodulated to obtain an indication of the movement of the predetermined zone.