Range information from signal distortions

• US 5,153,595 A
• Filed: 03/26/1990
• Issued: 10/06/1992
• Est. Priority Date: 03/26/1990
• Status: Expired due to Fees

• Current Assignee: Geophysical Survey Systems, Inc.
• Original Assignee: Geophysical Survey Systems, Inc.
• Inventors: Harmuth, Henning F.
• Primary Examiner(s): Sotomayor, John B.
• Application Number:
  US07/499,014
• Time in Patent Office: 925 Days
• Field of Search: 342/145, 342/22, 342/189, 342/124
• US Class Current: 342/22
• CPC Class Codes: G01S 13/10 using transmission of interrupted, pulse modulated waves determination of distance by phase measurement G01S13/32

Abstract

An electromagnetic signal having originally the time variation of a rectangular pulse is transmitted into a medium with conductivity σ. It is distorted by the medium to a signal f(σ,d,t) if it traveled the distance d from a transmitter to a scattering or reflecting object and the same distance d back to the transmitter. The time variation f(σ,d,t) of the distorted signal can be calculated for any conductivity σ and distance d. Using the conductivity σ known from previous measurements, the returned, distorted signal f(t) is compared with computed distorted signals f(σ,d,t) for various distances d. The computed signal f(σ,d,t) that is most similar to the actually received signal f(t) determines the distance d to the scattering or reflecting object. The comparison between the computed, distorted signals and the actually received signal is done by cross-correlations. The peak amplitude or the energy of the received signal becomes unimportant if cross-correlation is used, which means the physical size or radar cross-section of the scattering or reflecting object becomes unimportant.

Claims

1. A method for range determination in a lossy medium, comprising the steps of:

radiating an electromagnetic pulse into the lossy medium;

receiving a distorted electromagnetic pulse reflected from a target at a distance in the medium;

determining the range of the target by comparing the received pulse to a plurality of distorted sample pulses each representing a different travel distance through the medium, without regard to travel time through the medium and without determination of any pulse arrival time.

2. The method of claim 1 wherein the step of comparing includes the steps of;

determining the mean-square-difference between the received pulse and each sample pulse;

selecting the sample pulse which yields the smallest mean-square-difference; and

assigning as the distance travelled by the received pulse, the distance associated with the selected sample pulse.

3. The method of claim 1 wherein the step of comparing includes the step of finding the maximum valve of the function ##EQU6## for the received pulse of field strength E(y,t), and the sample pulses of field strength E(y_n,t), for a plurality of values of the variable y_n, representing distances into the media.

4. The method of claim 1 wherein the radiated electromagnetic pulse is not a periodic sinusoidal wave.

5. The method of claim 1 or claim 4 wherein the radiated electromagnetic pulse is a rectangular pulse.

6. The method of claim 1 wherein the distortion of the received electromagnetic pulse is substantially caused by the electromagnetic pulse traveling through the lossy medium.

7. The method of claim 1 wherein the step of comparing includes the steps of;

finding peak values of a function that correlates the received pulse and each sample pulse; and

selecting the sample pulse associated with the largest peak value.

8. The method of claim 7 wherein the step of selecting the sample pulse associated with the largest peak value is followed by the step of assigning as the distance travelled by the received pulse, the distance through the media associated with the selected sample pulse.

9. The method of claim 8 wherein the step of assigning the distance travelled by the received pulse, is followed by equating the range of the target to one half of the distance travelled by the pulse.

10. The method of claim 1 wherein the step of determining the distance that the pulse has travelled through the media is done in real time as echo information is being received.

11. The method of claim 1 wherein the step of comparing the received pulse with sample pulses, includes the steps of;

recording the received pulse; and

comparing the recorded received pulse with the sample pulses at a time after the received pulse was received.

12. The method of any of claims 1-3, wherein the step of comparing includes the step of computing the shape and amplitude of sample pulses for a plurality of distances through the media.

13. The method of any of claims 1-3, wherein the step of comparing includes the step of measuring the shape and amplitude of sample pulses that have travelled a plurality of distances through the media.