Method for using neutron interaction cross section to interpret neutron measurements

Patent metadata

Field	Value
Publication number	US-2016349398-A1
Application number	US-201514726050-A
Country	US
Kind code	A1
Filing date	May 29, 2015
Priority date	May 29, 2015
Publication date	Dec 1, 2016
Grant date	—

Abstract

A method for determining a fractional volume of at least one component of a formation includes entering into a computer a number of detected radiation events resulting from imparting neutrons into the formation at an energy level of at least 1 million electron volts (MeV). The detected radiation events correspond to at least one of an energy level of the imparted neutrons and thermal or epithermal energy neutrons. A measurement of at least one additional petrophysical parameter of the formation is made. The at least one additional petrophysical parameter measurement and at least one of a fast neutron cross-section and a thermal neutron cross-section determined from the detected radiation events are used in the computer to determine the fractional volume of the at least one component of the formation. In another embodiment, the fast neutron cross-section and the thermal neutron cross-section may be used on combination to determine the fractional volume.

First claim

What is claimed is:

1 . A method for determining a fractional volume of at least one component of a formation, comprising:
entering into a computer a number of detected radiation events resulting from imparting neutrons into the formation at an energy level of at least 1 million electron volts (MeV), the detected radiation events corresponding to at least one of an energy level of the imparted neutrons, and thermal or epithermal energy neutrons; and at least one of,
(i) in the computer, using a fast neutron cross-section and a thermal neutron cross-section determined from the detected radiation events to determine a fractional volume of the at least one component of the formation, and
(ii) entering into the computer a measurement of at least one additional petrophysical parameter and in the computer using (a) the measurement of the at least one petrophysical parameters and (b) at least one of the fast neutron cross-section and the thermal neutron cross-section to determine the fractional volume of the at least one component of the formation.

2 . The method of claim 1 wherein the at least one additional petrophysical parameter comprises bulk density.

3 . The method of claim 1 wherein the at least one additional petrophysical parameter comprises thermal neutron capture cross-section (Sigma).

4 . The method of claim 1 wherein the imparting neutrons comprises operating a pulsed neutron source.

5 . The method of claim 4 wherein an energy of neutrons emitted by the pulsed neutron source is approximately 14 MeV.

6 . The method of claim 1 wherein the detected radiation events comprise gamma rays resulting from interaction of the imparted neutrons with the formation.

7 . The method of claim 6 wherein the gamma rays comprise inelastic scattered gamma rays.

8 . The method of claim 6 wherein the gamma rays comprise capture gamma rays.

9 . The method of claim 1 wherein the thermal neutron cross-section is determined using an empirical relationship between numbers of detected thermal neutron radiation events and at least one other petrophysical parameter.

10 . The method of claim 9 wherein the thermal neutron radiation events are detected at two different distances from a position of the imparting neutrons and the empirical relationship with the at least one other petrophysical parameter is with a ratio of numbers of thermal neutron radiation events at each of the two different distances.

11 . The method of claim 10 wherein the thermal neutron radiation events comprise capture gamma rays.

12 . The method of claim 1 wherein the fast neutron cross-section is determined as a weighted linear combination of a 14-MeV neutron elastic cross section, a 14-MeV neutron inelastic cross section, and an atom density of a formation material.

13 . The method of claim 1 wherein the component of the formation comprises at least one of rock matrix, porosity, gas filled porosity and liquid filled porosity.

14 . A method for well logging, comprising:
moving a well logging instrument along a wellbore drilled through subsurface formations, the well logging instrument comprising a source of neutrons having emitted energy of at least million electron volts (MeV) and at least two radiation detectors spaced apart from the source at different distances along the instrument; imparting neutrons from the source into formations adjacent to the well logging instrument; detecting neutron induced radiation events at each of the two detectors; entering into a computer a number of the detected radiation events, the detected radiation events corresponding to at least one of an energy level of the imparted neutrons, and thermal or epithermal energy neutrons; and at least one of,
(i) in the computer, using a fast neutron cross-section and a thermal neutron cross-section determined from the detected radiation events to determine a fractional volume of the at least one component of the formation, and
(ii) entering into the computer a measurement of at least one additional petrophysical parameter and in the computer using (a) the measurement of the at least one petrophysical parameters and (b) at least one of the fast neutron cross-section and the thermal neutron cross-section to determine the fractional volume of the at least one component of the formation.

15 . The method of claim 14 wherein the at least one additional petrophysical parameter comprises bulk density.

16 . The method of claim 14 wherein the at least one additional petrophysical parameter comprises thermal neutron capture cross-section (Sigma).

17 . The method of claim 14 wherein the neutron source comprises a pulsed neutron source.

18 . The method of claim 17 wherein an energy of neutrons emitted by the pulsed neutron source is approximately 14 MeV.

19 . The method of claim 17 wherein the detected radiation events comprise gamma rays resulting from interaction of the imparted neutrons with the formations.

20 . The method of claim 19 wherein the gamma rays comprise inelastic scattered gamma rays.

21 . The method of claim 19 wherein the gamma rays comprise capture gamma rays.

22 . The method of claim 14 wherein the thermal neutron cross-section is determined using an empirical relationship between numbers of detected thermal neutron radiation events and at least one other petrophysical parameter.

23 . The method of claim 22 wherein the empirical relationship with the at least one other petrophysical parameter is with a ratio of numbers of thermal neutron radiation events at each of the two different distances.

24 . The method of claim 23 wherein the thermal neutron radiation events comprise capture gamma rays.

25 . The method of claim 14 wherein the fast neutron cross-section is determined as a weighted linear combination of a 14-MeV neutron elastic cross section, a 14-MeV neutron inelastic cross section, and an atom density of a formation material.

26 . The method of claim 14 wherein the component of the formation comprises at least one of rock matrix, porosity, gas filled porosity and liquid filled porosity.

27 . The method of claim 14 wherein the moving the well logging instrument comprises moving an electrical cable in the wellbore, the well logging instrument connected to the electrical cable.

28 . The method of claim 14 wherein the moving the well logging instrument comprises moving a drill string along the wellbore, the well logging instrument disposed in a part of the drill string.

Assignees

• Schlumberger Technology Corp

Inventors

• Zhou Tong
• Stoller Christian
• Thornton James Leslie
• Rose David Alan

Classifications

• G01N33/24

  Earth materials (G01N33/42 takes precedence) · CPC title

• G01V5/10 Primary

  using neutron sources {(neutron generating tubes H05H5/00; neutron sources using isotopes G21G4/00)} · CPC title

• G01V5/104

  and detecting secondary Y-rays as well as reflected or back-scattered neutrons · CPC title

• G01V5/108

  the neutron source being of the pulsed type · CPC title

• G01V5/107

  and detecting reflected or back-scattered neutrons · CPC title