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    • 1. 发明申请
    • SINGLE DRIVE BETATRON
    • 单驱动BETATRON
    • WO2009079063A1
    • 2009-06-25
    • PCT/US2008/077738
    • 2008-09-25
    • SERVICES PETROLIERS SCHLUMBERGERSCHLUMBERGER CANADA LIMITEDSCHLUMBERGER HOLDINGS LIMITEDSCHLUMBERGER TECHNOLOGY B.V.PRAD RESEARCH AND DEVELOPMENTCHEN, Felix
    • CHEN, Felix
    • H05H11/00H05H11/04
    • H05H11/00H05H11/04
    • A betatron includes a betatron magnet with a first guide magnet having a first pole face and a second guide magnet having a second pole face. Both the first and the second guide magnet have a centrally disposed aperture and the first pole face is separated from the second pole face by a guide magnet gap. A core is disposed within the centrally disposed apertures in an abutting relationship with both guide magnets. The core has at least one core gap. A drive coil is wound around both guide magnet pole faces. An orbit control coil has a contraction coil portion wound around the core gap and a bias control portion wound around the guide magnet pole faces. The contraction coil portion and the bias control portion are connected but in opposite polarity. Magnet fluxes in the core and guide magnets return through peripheral portions of the betatron magnet.
    • 贝塔管包括具有带有第一极面的第一引导磁体和具有第二极面的第二引导磁体的贝塔通磁体。 第一和第二引导磁体都具有居中设置的孔,并且第一极面通过引导磁体间隙与第二极面分离。 芯部设置在与两个导向磁体邻接的中心设置的孔内。 核心至少有一个核心缺口。 驱动线圈缠绕在两个导向磁极面上。 轨道控制线圈具有缠绕在芯间隙上的收缩线圈部分和缠绕在导磁体磁极面上的偏置控制部分。 收缩线圈部分和偏压控制部分连接但具有相反的极性。 铁芯和导向磁体中的磁通量通过该铂电磁体的周边部分返回。
    • 2. 发明申请
    • METHOD OF EXTRACTING FORMATION DENSITY AND PE USING A PULSED ACCELERATOR BASED LITHO-DENSITY TOOL
    • 使用基于加速器的LITHO-DENSITY工具提取形成密度和PE的方法
    • WO2009058501A2
    • 2009-05-07
    • PCT/US2008/078225
    • 2008-09-30
    • SERVICES PETROLIERS SCHLUMBERGERSCHLUMBERGER CANADA LIMITEDSCHLUMBERGER HOLDINGS LIMITEDSCHLUMBERGER TECHNOLOGY B.V.PRAD RESEARCH AND DEVELOPMENT LTDZHOU, TongCHEN, FelixCASE, Charles, R.ELLIS, Darwin, V.ROSCOE, Bradley, Albert
    • ZHOU, TongCHEN, FelixCASE, Charles, R.ELLIS, Darwin, V.ROSCOE, Bradley, Albert
    • G01V5/125
    • A method for a pulsed gamma - gamma density tool to simultaneously compensate for interactions due to the photoelectric effect and density variations caused by standoff enables a more precise determination of bulk formation density. This method includes the steps of providing a source of energetic particles and directing those energetic particles at a formation having a known photoelectric factor and electron density and capturing one or more photons either emitted or deflected from the formation either a first detector or a second detector. The first detector is spaced a first distance from the source, the second detector is spaced a second distance from the detector and a third distance separates the first detector from the second detector. Measuring a first total energy of the photons striking the first detector during a time interval and measuring a second total energy of the photons striking the second detector as a function of the time interval and disposing a first filter between the first detector and the formation effective to cause Pe response to match standoff influence thereby compensating for both effects simultaneously. In addition to the first filter, the required compensation may include a second filter between the second detector and the formation as well as adjustments to the respective first distance, second distance and third distance.
    • 用于同时补偿由于光电效应引起的相互作用和由间隔引起的密度变化的脉冲伽马伽马密度工具的方法使得能够更准确地确定体积形成密度。 该方法包括以下步骤:提供能量粒子源,并将具有已知光电因子和电子密度的地层中的能量粒子引导并捕获从第一检测器或第二检测器的地层发射或偏转的一个或多个光子。 第一检测器与源极隔开第一距离,第二检测器与检测器隔开第二距离,第三距离将第一检测器与第二检测器分开。 测量在时间间隔内撞击第一检测器的光子的第一总能量,并测量作为时间间隔的函数的撞击第二检测器的光子的第二总能量,并且在第一检测器和地层之间设置第一过滤器, 导致Pe响应匹配对立影响,从而同时补偿两种效应。 除了第一滤波器之外,所需的补偿可以包括在第二检测器和地层之间的第二滤波器以及对相应的第一距离,第二距离和第三距离的调整。
    • 8. 发明申请
    • METHOD OF COMPENSATING FOR THE PHOTOELECTRIC EFFECT IN PULSED, ACCELERATOR-BASED LITHO-DENSITY TOOL
    • 基于加速器的LITHO-DENSITY工具中的光电效应补偿方法
    • WO2009058501A8
    • 2012-01-26
    • PCT/US2008078225
    • 2008-09-30
    • SCHLUMBERGER SERVICES PETROLSCHLUMBERGER CA LTDSCHLUMBERGER HOLDINGSSCHLUMBERGER TECHNOLOGY BVPRAD RES & DEV LTDZHOU TONGCHEN FELIXCASE CHARLES RELLIS DARWIN VROSCOE BRADLEY ALBERT
    • ZHOU TONGCHEN FELIXCASE CHARLES RELLIS DARWIN VROSCOE BRADLEY ALBERT
    • G01V5/12
    • G01V5/125
    • A method for a pulsed gamma - gamma density tool to simultaneously compensate for interactions due to the photoelectric effect and density variations caused by standoff enables a more precise determination of bulk formation density. This method includes the steps of providing a source of energetic particles and directing those energetic particles at a formation having a known photoelectric factor and electron density and capturing one or more photons either emitted or deflected from the formation either a first detector or a second detector. The first detector is spaced a first distance from the source, the second detector is spaced a second distance from the detector and a third distance separates the first detector from the second detector. Measuring a first total energy of the photons striking the first detector during a time interval and measuring a second total energy of the photons striking the second detector as a function of the time interval and disposing a first filter between the first detector and the formation effective to cause Pe response to match standoff influence thereby compensating for both effects simultaneously. In addition to the first filter, the required compensation may include a second filter between the second detector and the formation as well as adjustments to the respective first distance, second distance and third distance.
    • 用于同时补偿由于光电效应引起的相互作用和由间隔引起的密度变化的脉冲伽马伽马密度工具的方法使得能够更准确地确定体积形成密度。 该方法包括以下步骤:提供能量粒子源,并将具有已知光电因子和电子密度的地层中的能量粒子引导并捕获从第一检测器或第二检测器的地层发射或偏转的一个或多个光子。 第一检测器与源极隔开第一距离,第二检测器与检测器隔开第二距离,第三距离将第一检测器与第二检测器分开。 测量在时间间隔内撞击第一检测器的光子的第一总能量,并测量作为时间间隔的函数的撞击第二检测器的光子的第二总能量,并且在第一检测器和地层之间设置第一过滤器, 导致Pe响应匹配对立影响,从而同时补偿两种效应。 除了第一滤波器之外,所需的补偿可以包括在第二检测器和地层之间的第二滤波器以及对相应的第一距离,第二距离和第三距离的调整。
    • 9. 发明申请
    • METHOD OF COMPENSATING FOR THE PHOTOELECTRIC EFFECT IN PULSED, ACCELERATOR-BASED LITHO-DENSITY TOOL
    • 基于加速器的LITHO-DENSITY工具中的光电效应补偿方法
    • WO2009058501A3
    • 2009-08-27
    • PCT/US2008078225
    • 2008-09-30
    • SCHLUMBERGER SERVICES PETROLSCHLUMBERGER CA LTDSCHLUMBERGER HOLDINGSSCHLUMBERGER TECHNOLOGY BVPRAD RES & DEV LTDZHOU TONGCHEN FELIXCASE CHARLES RELLIS DARWIN VROSCOE BRADLEY ALBERT
    • ZHOU TONGCHEN FELIXCASE CHARLES RELLIS DARWIN VROSCOE BRADLEY ALBERT
    • G01V5/12
    • G01V5/125
    • A method for a pulsed gamma - gamma density tool to simultaneously compensate for interactions due to the photoelectric effect and density variations caused by standoff enables a more precise determination of bulk formation density. This method includes the steps of providing a source of energetic particles and directing those energetic particles at a formation having a known photoelectric factor and electron density and capturing one or more photons either emitted or deflected from the formation either a first detector or a second detector. The first detector is spaced a first distance from the source, the second detector is spaced a second distance from the detector and a third distance separates the first detector from the second detector. Measuring a first total energy of the photons striking the first detector during a time interval and measuring a second total energy of the photons striking the second detector as a function of the time interval and disposing a first filter between the first detector and the formation effective to cause Pe response to match standoff influence thereby compensating for both effects simultaneously. In addition to the first filter, the required compensation may include a second filter between the second detector and the formation as well as adjustments to the respective first distance, second distance and third distance.
    • 用于同时补偿由于光电效应引起的相互作用和由间隔引起的密度变化的脉冲伽马伽马密度工具的方法使得能够更准确地确定体积形成密度。 该方法包括以下步骤:提供能量粒子源,并将具有已知光电因子和电子密度的地层中的能量粒子引导并捕获从第一检测器或第二检测器的地层发射或偏转的一个或多个光子。 第一检测器与源极隔开第一距离,第二检测器与检测器隔开第二距离,第三距离将第一检测器与第二检测器分开。 测量在时间间隔内撞击第一检测器的光子的第一总能量,并测量作为时间间隔的函数的撞击第二检测器的光子的第二总能量,并且在第一检测器和地层之间设置第一过滤器, 导致Pe响应匹配对立影响,从而同时补偿两种效应。 除了第一滤波器之外,所需的补偿可以包括在第二检测器和地层之间的第二滤波器以及对相应的第一距离,第二距离和第三距离的调整。