Christopher E. Morriss
Schlumberger
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Featured researches published by Christopher E. Morriss.
Magnetic Resonance Imaging | 1996
Robert Freedman; Christopher E. Morriss
When a pulsed nuclear magnetic resonance (NMR) well logging tool is traversing a wellbore, a NMR well logging method includes magnetizing the hydrogen nuclei in a formation traversed by the tool with a static magnetic field, waiting for a first period of time W1, energizing the formation with oscillating RF pulses, collecting a first plurality of spin echo signals, waiting a second period of time W2 which is different from the first period of time W1, energizing the formation with oscillating RF pulses, collecting a second plurality of spin echo signals, waiting a third period of time W3 which is different from both the second period of time W2 and the first period of time W1, energizing the formation with oscillating RF pulses, collecting a third plurality of spin echo signals, etc. The first, second and third, etc. plurality of spin echo signals corresponding to the different wait times are input to a signal processing apparatus disposed in the tool. Window sums of spin-echo signals are computed and transmitted uphole to a surface oriented signal processing apparatus. In response to the window sums, the surface signal processing apparatus determines an apparent formation T2 -distribution for each wait time in the multi-wait time pulse sequence. The apparent T2 -distributions are used to construct a cost function. When the cost function is minimized, the surface oriented signal processing apparatus determines estimates of the true T1 /T2 ratios and intrinsic T2 -distributions of the formations being logged. The surface signal processing apparatus uses the new T2 -distribution to generate new, more accurate, output record medium.
ieee antennas and propagation society international symposium | 2003
Jaideva C. Goswami; Denis Heliot; Jacques R. Tabanou; Christopher E. Morriss
Earth formations can be modeled as a layered medium with each layer having its own dip angle and conductivity. In a typical exploration environment, a wellbore (about 15 to 30 cms in diameter) is drilled to a depth that may extend to a few kilometers. Formation properties are measured using a sensor that moves along the wellbore trajectory. The sensor is remotely controlled from the surface. Formation resistivity is an important property, which is measured by a sensor consisting of several transmitters and receivers and operating at a frequency of a few MHz. Estimating dip angles provides valuable information in positioning the wellbore trajectory. We present a novel method for estimating dip angles and formation properties using a wavelet-based processing of well log data in conjunction with an inversion method.
Archive | 1998
Robert Freedman; Christopher E. Morriss; Austin Boyd; Charles Flaum
Archive | 2006
Jacques R. Tabanou; Christopher E. Morriss
Archive | 2003
Jaideva C. Goswami; Denis Heliot; Jacques R. Tabanou; Christopher E. Morriss
SPWLA 38th Annual Logging Symposium | 1997
R. Freedman; Austin Boyd; Greg Gubelin; D. Mckeon; Christopher E. Morriss; Charles Flaum
Archive | 2015
Sushil Shetty; John Rasmus; Christopher E. Morriss; Koji Ito; Shahzad Asif; Vittorio Picco
Archive | 2014
Keli Sun; Roger Griffiths; Steve F. Crary; Christopher E. Morriss; Koji Ito
Archive | 2016
Keli Sun; Koji Ito; Christopher E. Morriss; Roger Griffiths; Steve F. Crary; Shahzad Asif
Archive | 2016
Joan Abadie; Adrien Chassard; Mohammad Taghi Salehi; David Maggs; Shahzad Asif; Christopher E. Morriss; Koji Ito