Method and apparatus for measuring the inside diameter of a metallic pipe in a well

• US 4,546,314 A
• Filed: 12/13/1982
• Issued: 10/08/1985
• Est. Priority Date: 12/13/1982
• Status: Expired due to Term

• Current Assignee: Schlumberger Technology Corporation (Schlumberger NV)
• Original Assignee: Schlumberger Technology Corporation (Schlumberger NV)
• Inventors: Minerbo, Gerald N., McCann, R. Bruce
• Primary Examiner(s): Strecker, Gerard R.
• Assistant Examiner(s): EDMONDS, WARREN
• Application Number:
  US06/449,016
• Time in Patent Office: 1,030 Days
• Field of Search: 324/219-221, 324/345, 324/346, 33/178 F, 33/178 E, 33/DIG. 1
• US Class Current: 324/221
• CPC Class Codes: E21B 47/085 using radiant means, e.g. acoustic, radioactive or electromagnetic
• CPC Class Codes: G01B 7/10 using magnetic means, e.g. by measuring change of reluctance

Abstract

A method and apparatus is disclosed for electrically measuring the inside diameter of a metallic pipe such as oil or gas well casing. The transimpedance of two coaxial coils within the pipe is determined and then resolved into its inphase and quadrature components. The difference of the magnitudes of the two components, ΔZ, is approximated by a function independent of the electrical properties of the pipe but which is a function of the inside diameter of the pipe. The inside diameter is determined from the function in response to the measured ΔZ and may be recorded as a function of travel distance in the pipe.

Claims

1. Apparatus for measuring the inside diameter of a metallic pipe in a well, comprising

a support member, adapted for displacement through the pipe,

transmitter means including a transmitter coil disposed on said support member for generating an a.c. transmitter current,

receiver means including a receiver coil disposed on said support member a distance from said transmitter coil for producing a receiver voltage in response to the effect of said transmitter current on the pipe, said voltage including a component in-phase with the transmitter current and a component in quadrature to the transmitter current,

means responsive to said receiver means and said transmitter means for deriving a signal Δ

Z representative of the difference between the real and imaginary components of the impedance, defined as the ratio of the receiver voltage to the transmitter current, said real component being in phase with the transmitter current and said imaginary component being in quadrature to the transmitter current, and

means for deriving a signal representative of the inside diameter of the pipe from said difference signal Δ

Z, based on a predetermined relationship between the difference signal and the inside diameter.

2. The apparatus of claim 1 wherein the frequency of said a.c. transmitter current is about 65 kHz.

3. The apparatus of claim 1 further including means for moving the support member within the pipe.

4. The apparatus of claim 3 further including means for recording said inside diameter signal as a function of distance along the pipe.

5. The apparatus of claim 1 wherein said transmitter and receiver coils are coaxially supported on said support member.

6. The apparatus of claim 5 where the diameter of said transmitter coil and the diameter of the receiver coil are substantially the same.

7. The apparatus of claim 5 wherein said inside diameter of the pipe signal is obtained from computational means for solving the equation:

##EQU9## where ##EQU10## and a₁ represents the inside radius of the pipe,

b represents the radius of the transmitter and receiver coils,

L is the distance between the transmitter coil and the receiver coil,

I₁ (λ

b) is a modified Bessel function of the first kind,

K₁ (λ

b) is a modified Bessel function of the second kind,

λ

is a variable of integration,

μ

₀ is the permeability of free space, and

ω

=2π

f, is the radian frequency of the a.c. transmitter current.

8. The apparatus of claim 7 wherein the equation, ##EQU11## is precomputed over a range of values of Δ

Z and a₁ to produce a polynomial function

space="preserve" listing-type="equation">a.sub.1 =f(Δ

Z), and

a signal, a₁, representative of the inside radius of the pipe is generated by solving said polynomial as a function of Δ

Z.

9. The apparatus of claim 7 wherein the equation ##EQU12## is predetermined over a range of values of Δ

Z and a₁ to produce a table of values, and

said table of values is stored in a digital memory, and

wherein said apparatus further includes means for addressing said digital memory with said a measured Δ

Z value to generate a signal a₁ representative of the inside radius of the pipe.

10. A method for determining the inside diameter of a metallic pipe located in a well, comprising

applying a current to a transmitter coil positioned inside the pipe and coaxially thereto,

detecting the voltage induced by said current in a receiver coil longitudinally spaced from, and coaxial to, the transmitter coil, said voltage including a component in-phase with the transmitter current and a component in quadrature to the transmitter current,

deriving a signal Δ

Z representative of the difference between the real and imaginary components of the impedance, defined as the ratio of the receiver voltage to the transmitter current, said real component being in phase with the transmitter current and said imaginary component being in quadrature to the transmitter current,

deriving a signal representative of the inside diameter of the pipe from said difference signal Δ

Z based on a predetermined relationship between the difference signal and the inside diameter.

11. The method of claim 10, wherein said relationship between the difference signal Δ

Z and the inside diameter is;

space="preserve" listing-type="equation">Δ

Z=2ω

μ

.sub.0 b.sup.2 (ZINT0-ZINT1)

where ##EQU13## and a₁ represents the inside radius of the pipe,

b represents the radius of the transmitter and receiver coils,

L is the distance between the transmitter and the receiver coil,

I₁ (λ

b) is a modified Bessel function of the first kind,

K₁ (λ

b) is a modified Bessel function of the second kind,

λ

is a variable of integration,

μ

₀ is the permeability of free space, and

ω

=2π

f, is the radian frequency of the a.c. transmitter current.

12. A method for producing a signal related to the inside diameter of a pipe located in a well, comprising

applying a current to a transmitter coil positioned inside the pipe and coaxially thereto,

detecting the voltage induced by said current in a receiver coil longitudinally spaced from, and coaxial to, the transmitter coil, said voltage including a component in-phase with the transmitter current and a component in quadrature to the transmitter current,

deriving a signal Δ

Z representative of the difference between the real and imaginary components of the impedance, defined as the ratio of the receiver voltage to the transmitter current, said real component being in phase with the transmitter current and said imaginary component being in quadrature to the transmitter current, said difference signal Z being related to the inside diameter of the pipe and having a reduced sensitivity to the permeability and conductivity of the pipe.

13. The method of claim 12, wherein said deriving step includes the steps of,

deriving said in-phase and said quadrature voltage components from said receiver voltage, and

measuring said transmitter current.

14. An apparatus for producing a signal related to the inside diameter of a pipe located in a well, comprising

a support member, adapted for displacement through the pipe,

transmitter means including a transmitter coil disposed on said support member for generating an a.c. transmitter current,

receiver means including a receiver coil disposed on said support member a distance from said transmitter coil for producing a receiver voltage in response to the effect of said transmitter current on the pipe, said voltage including a component in-phase with the transmitter current and a component in quadrature to the transmitter current,

means responsive to said receiver means and to said transmitter means for generating a signal Δ

Z equal to the difference between the real and the imaginary parts of an impedance signal defined as the ratio of the receiver voltage to the transmitter current, said real part being the component in-phase with the transmitter current and said imaginary part being the component in quadrature to the transmitter current, said difference signal Δ

Z being related to the inside diameter of the pipe and having a reduced sensitivity to the permeability and conductivity of the pipe.

15. The apparatus of claim 14, wherein said generating means includes a phase sensitive detector having inputs connected to the receiver coil, and means for generating phase reference signals respectively in phase with, and in quadrature to the transmitter current, said reference signals being applied to the phase sensitive detector.

16. The apparatus of claim 15, comprising switch means connected between the receiver coil and the phase sensitive detector and having an input connected to the transmitting means, whereby a signal indicative of the transmitter current can be applied to the phase sensitive detector.

17. The apparatus of claim 16, wherein said switch means includes an additional input connected to the ground.