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    • 1. 发明授权
    • Method for processing the lapse measurements
    • 处理流逝测量的方法
    • US06344746B1
    • 2002-02-05
    • US09454690
    • 1999-12-03
    • Raghu K. ChunduruAlberto G. MezzatestaRainer Busch
    • Raghu K. ChunduruAlberto G. MezzatestaRainer Busch
    • G01V318
    • G01V11/00
    • Resistivity data acquired at two different epochs using different types of tools are jointly inverted. For example, a multiple propagation resistivity (MPR) tool is run first, preferably at several frequencies and several transmitter-receiver spacings. At a later epoch, an induction tool may be run, preferably on a wireline. The joint inversion process identifies bed boundaries based on inflection points in the propagation resistivity and induction logging raw data. An initial guess for an uninvaded earth model is generated using the selected bed boundaries and the apparent raw resistivity values. An inversion run using shallow measurements of propagation resistivity logging data is performed to estimate a resistivity structure representative of the near borehole zone resistivity (invaded zone). The bed boundary positions of the layers are also updated as part of the inversion process. Synthetic data for both the shallow and deep measurements are generated to delineate the invasion zones. If the data match is good for both shallow and deep subarrays, then the model obtained from the shallow data is used as the final model for the inversion. In the event the data match is good for short subarrays and not for long subarrays, a final inversion run is performed by introducing invasion in the earth model. The method may be used for inverting data obtained from wireline, MWD or permanently implanted sensors at two or more epochs.
    • 使用不同类型工具在两个不同时期获取的电阻率数据被共同反转。 例如,首先运行多传播电阻率(MPR)工具,优选地在几个频率和几个发射器 - 接收器间隔处运行。 在稍后的时代,可以运行感应工具,优选在有线上运行。 联合反演过程基于传播电阻率和感应测井原始数据中的拐点识别床边界。 使用选定的床边界和表观原始电阻率值产生无侵蚀地球模型的初始猜测。 进行使用传播电阻率测井数据的浅测量的反演运行,以估计代表近钻孔区电阻率(入侵区)的电阻率结构。 层的床边界位置也作为反演过程的一部分被更新。 产生浅和深测量的合成数据,以描绘入侵区。 如果数据匹配对浅层和深层子阵列都有好处,则从浅层数据获得的模型被用作反演的最终模型。 如果数据匹配对于短的子阵列而言不利于长的子阵列,则通过在地球模型中引入入侵来执行最终的反演运行。 该方法可以用于在两个或更多个时期反转从有线,MWD或永久植入的传感器获得的数据。
    • 3. 发明授权
    • Method for determining earth formation shear wave anisotropy parameters
by inversion processing of signals from a multiple-component dipole
array acoustic well logging instrument
    • 通过对来自多组分偶极阵列声测井仪器的信号的反演处理确定地层剪切波各向异性参数的方法
    • US5712829A
    • 1998-01-27
    • US696668
    • 1996-08-14
    • Xiaoming TangRaghu K. Chunduru
    • Xiaoming TangRaghu K. Chunduru
    • G01V1/44G01V1/52G01V1/40G01V1/28
    • G01V1/52G01V1/44
    • A method for determining orientations and velocities of slow and fast waves in an anisotropic earth formation. Signals are used from an acoustic logging tool including dipole transmitters and receiver arrays. An initial value of angle subtended between orientation of the fast wave and one of the transmitters is selected. A waveform of a fast principal wave and slow principal wave at first and second selected receiver positions are calculated from received signals at each of these positions and the selected subtended angle. A derivative waveform with respect to subtended angle is calculated for both fast and slow principal waves. An initial velocity of slow waves is selected and the calculated waveforms of the slow principal wave and its derivative waveform at the first position are time shifted by a time corresponding to distance between first and second receiver positions and the selected value of velocity. A value of difference in velocity between slow waves and fast waves is selected, and the time-shifted slow principal wave and its derivative waveform are adjusted by a time corresponding to the value of difference in velocities. Differences between the time-adjusted wave and its derivative waveform are determined between the calculated fast principal wave and its derivative waveform calculated at that receiver position. The value of velocity, value of difference in velocity and subtended angle are adjusted and calculating waveforms and derivative waveforms, time shifting and time adjusting are repeated until the difference between waveforms reaches a minimum.
    • 一种用于确定各向异性地层中慢波和快波的方向和速度的方法。 信号用于包括偶极发射器和接收器阵列的声学测井工具。 选择快速波的方向与发射机之一对准的初始角度值。 在这些位置和所选择的对置角度的接收信号中计算第一和第二选择的接收机位置处的快速主波和慢主波形的波形。 针对快速和慢速主波计算相对于对角的导数波形。 选择慢波的初始速度,并且将第一位置处的慢主波及其导数波形的计算波形时间移位一个对应于第一和第二接收器位置之间的距离和所选择的速度值的时间。 选择慢波和快波之间的速度差值,并将时移慢主波及其导数波形调整到与速度差值相对应的时间。 在计算的快速主波及其在该接收机位置处计算的导数波形之间确定时间调整波及其导数波形之间的差异。 调整速度值,速度和对角度差值,并重复计算波形和导数波形,时移和时间调整,直到波形之间的差值达到最小值。
    • 4. 发明授权
    • Method for determining acoustic velocity of earth formations by
simulating receiver waveforms for an acoustic array well logging
instrument
    • 通过模拟声阵列测井仪器的接收器波形来确定地层声速的方法
    • US5740124A
    • 1998-04-14
    • US752327
    • 1996-11-19
    • Raghu K. ChunduruXiaoming Tang
    • Raghu K. ChunduruXiaoming Tang
    • G01V1/46G01V1/40G01V1/36
    • G01V1/46
    • A method of determining the acoustic propagation velocities of earth formations using signals generated by an acoustic array well logging instrument. The method includes generating a model of the acoustic velocities including a value of velocity for each propagation mode for which the velocity is to be determined Acoustic waveforms are synthesized for a plurality of receiver locations on the acoustic logging instrument by using the values of the acoustic velocities in the model. A difference is determined between the synthesized waveforms and measured waveforms generated by acoustic energy detected at corresponding receiver locations on the acoustic logging instrument. The model is adjusted and the waveforms are resynthesized until the difference is determined to be at a minimum. The step of adjusting the model is performed by very fast simulated annealing.
    • 使用由声阵列测井仪产生的信号来确定地球地层声传播速度的方法。 该方法包括生成声速模型,其包括要为其确定速度的每个传播模式的速度值。通过使用声速的值,在声学测井仪器上为多个接收器位置合成声波形 在模型中。 在声波测井仪器上的相应接收器位置处检测到的声能产生的合成波形和测量波形之间确定差异。 调整模型,并重新合成波形,直到将该差值确定为最小值。 通过非常快速的模拟退火进行调整模型的步骤。