Range information from signal distortions

• US 5,159,343 A
• Filed: 02/13/1991
• Issued: 10/27/1992
• 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:
  US07/654,899
• Time in Patent Office: 622 Days
• Field of Search: 342/22, 342/123, 342/124, 342/145, 342/189, 342/191, 342/192, 342/193, 342/195, 342/118
• 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 radiated into a lossy medium with conductivity σ. It is distorted by the medium to the distorted electromagnetic pulse f(σ,y,t) when it travels the distance y/2, in time t/2, from a transmitter to a scattering or reflecting target and the same distance y/2, in time t/2, back to the receiver. The time variation f(σ,y,t) of the distorted pulse can be calculated for any conductivity σ and distance y using the conductivity σ known from previous measurements to determine the range to the target distorted pulse f(σ,y,t). Consequently, distorted pulses f(σ,y_n,t) can be computed and compared to the received distorted pulse f(σ,y,t). The computed pulse f(σ,y_n, t) that is most similar to the received pulse f(σ,y,t) determines the distance y_n /2 to the scattering or reflecting object, which is the range to the target. The comparison between the computed, distorted signals and the actually received signal can be done by cross-correlation. If cross-correlation is used, the peak amplitude or the energy of the received signal becomes unimportant which means the physical size or radar cross-section of the target has no effect on the distance determination.

Claims

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

radiating an electromagnetic pulse into the lossy media;

receiving a distorted electromagnetic pulse returned from a target at a time 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 time through the medium.

2. The method of claim 1 wherein the step of determining 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 time traveled by the received pulse, the time associated with the selected sample pulse.

3. The method of claim 1 wherein the step of determining includes the step of finding the maximum value of the function ##EQU7## for the received pulse of field strength E(τ

,t), and the sample pulses of field strength E(τ

_n,t), for a plurality of values of the variable τ

_n, representing times traveled in the media.

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

5. The method of either 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 determining includes the steps of:

finding a value of cross-correlation functions of the received pulse and each sample pulse; and

selecting the sample pulse associated with the value of the function that is greater than a predetermined detection threshold.

8. The method of claim 7 wherein the step of selecting the sample pulse associated with the value above the detection threshold is followed by the step of assigning as the time traveled by the received pulse, the time associated with the selected sample pulse.

9. The method of claim 8 wherein the step of assigning the time traveled by the received pulse is followed by the step of associating the range of the target to one-half of the time traveled by the pulse.

10. The method of claim 1 wherein the step of determining the range is done in real-time as the return signal is being received.

11. The method of claim 1 wherein the step of determining the range includes the steps of:

recording the received pulse; and

comparing the recorded pulses 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 determining the range includes the step of computing the time variation of sample pulses for a plurality of distances through the medium.