ID microwave holographic sensor

• US 5,327,139 A
• Filed: 09/11/1992
• Issued: 07/05/1994
• Est. Priority Date: 09/11/1992
• Status: Expired due to Term

• Current Assignee: The Boeing Co.
• Original Assignee: The Boeing Co.
• Inventors: Johnson, Walter J.
• Primary Examiner(s): Sotomayor, John B.
• Application Number:
  US07/944,163
• Time in Patent Office: 662 Days
• Field of Search: 342/22, 342/27
• US Class Current: 342/22
• CPC Class Codes: G01R 27/267 Coils or antennae arrangements, e.g. coils surrounding the sample or transmitter/receiver antennae
• CPC Class Codes: G01S 13/0209 Systems with very large relative bandwidth, i.e. larger than 10 %, e.g. baseband, pulse, carrier-free, ultrawideband
• CPC Class Codes: G01S 13/34 using transmission of continuous, frequency-modulated waves while heterodyning the received signal, or a signal derived therefrom, with a locally-generated signal related to the contemporaneously transmitted signal
• CPC Class Codes: G01S 13/885 for ground probing prospecting or detecting using electromagnetic waves G01V3/12
• CPC Class Codes: G01S 13/90 using synthetic aperture techniques , e.g. synthetic aperture radar [SAR] techniques

Abstract

A method and apparatus for measuring both physical and electrical properties of a dielectric object using sequential spatial and spectral microwave data. The apparatus is a step CW microwave transmitter and receiver with a spatially modulated antenna positioned linearly in the Poynting vector direction. The method removes the antenna dispersion, removes the antenna image, transfers the image plane to the surface, removes diffraction and then removes the nuisance multipath by spatially integrating along the Poynting vector. The result is a clean complex surface reflection coefficient that contains only the subsurface or object plane information. This clean complex surface reflection coefficient may be compared to reflection coefficients of known objects in order to ascertain physical characteristics of the object.

Claims

1. A method for characterizing a target within a medium, comprising the steps of:

a) radiating an unmodulated electro-magnetic wave from an electro-magnetic wave source towards said medium;

b) changing the frequency of said electro-magnetic wave over a plurality of successive frequencies;

c) measuring electro-magnetic waves reflected from said medium at said plurality of successive frequencies for a single perpendicular distance form said medium to said electro-magnetic wave source to produce measured signals, respectively;

d) processing said measured signals to obtain a reflection coefficient dependent on both frequency of said electro-magnetic wave and said perpendicular distance;

e) repeating steps c) and d) to produce a plurality of reflection coefficients for a predetermined number of perpendicular distances;

f) averaging all said reflection coefficients over said predetermined number; and

g) integrating said averaged reflection coefficients over space, resulting in a true reflection coefficient which is only a function of frequency.

2. A method as recited in claim 1, further comprising the steps of:

h) comparing said true reflection coefficient with theoretical reflection coefficients for respective objects each having known characteristics; and

i) outputting said known characteristics of an object which correlates best with said target based on said comparing step.

3. A method as recited in claim 1, wherein said processing step comprises the steps of:

correcting said measured signals by removing antenna dispersion to produce corrected signals; and

dividing said corrected signals by a spatial delay term.

4. A method as recited in claim 2, wherein said comparing step further comprises the steps of:

transforming said true reflection coefficient into a time domain;

gating out all information on either side of a range centered on a main peak in said time domain to produce a gated true reflection coefficient; and

transforming said gated true reflection coefficient back to a frequency domain for comparison with said theoretical reflection coefficients.

5. A method as recited in claim 2, wherein said target is characterized by thickness and dielectric constant.

6. An apparatus for characterizing a target within a medium, comprising:

an antenna for both transmitting electro-magnetic waves at different unmodulated carrier frequencies towards said medium and receiving reflected electro-magnetic waves from said medium; and

means for processing said reflected electro-magnetic waves comprising

means for obtaining, from said reflected electro-magnetic waves, a true reflection coefficient dependent only on said frequencies;

means for comparing said true reflection coefficient with theoretical reflection coefficients for respective objects, each of said object having known characteristics and

means for outputting said known characteristics of an object which said comparing means determines correlates best with said target.

7. An apparatus as recited in claim 6, wherein said obtaining means comprises:

means for accounting for antenna transfer functions in said reflected electro-magnetic waves to produce accounted signals;

means for dividing said accounted signals by a spatial delay term and outputting reflection coefficients dependent on both said frequencies of said electro-magnetic waves and distance between said antenna and said medium;

means for averaging said reflection coefficients over a number of distances over which signals were received to produce an averaged reflection coefficient; and

means for integrating said averaged reflection coefficient over space.

8. An apparatus as recited in claim 6, further comprising:

means, receiving said true reflection coefficient and outputting a clean true reflection coefficient to said comparing means, for removing unwanted reflections comprising

means for transforming said clean true reflection coefficient into a time domain

means for gating out all information on either side of a range centered on a main peak in said time domain to produce a gated true reflection coefficient and

means for transforming said gated true reflection coefficient back to a frequency domain.

9. An apparatus as recited in claim 6, wherein said target is characterized by thickness and dielectric constant.

10. A method for characterizing a target within a medium, comprising the steps of:

a) successively radiating electro-magnetic waves from a source towards said medium, said source being at a single perpendicular distance from said medium, said electro-magnetic waves being at different frequencies, respectively, and each of said electro-magnetic waves being unmodulated;

b) successively receiving reflected electro-magnetic waves from said medium at said single perpendicular distance, said reflected electro-magnetic waves being at said different frequencies, respectively;

c) converting said reflected electro-magnetic waves to received signals, respectively;

d) processing each of said received signals to produce a respective reflection coefficient dependent on each frequency of said reflected electro-magnetic waves and said single perpendicular distance;

e) repeating steps a) to d) for a plurality of additional perpendicular distances to produce additional reflection coefficients, said single perpendicular distance and said additional perpendicular distances together constituting a predetermined number of perpendicular distances;

f) averaging all said reflection coefficients over said predetermined number to produce an averaged reflection coefficient; and

g) integrating said averaged reflection coefficient over space to produce a true reflection coefficient, which is a function of only frequency, to output characteristics of a known reflection coefficient which compares best with said true reflection coefficient.

11. An apparatus for characterizing a target within a medium, comprising:

antenna means for radiating a plurality of transmitted electro-magnetic waves to said medium at each of a number of perpendicular distances from said medium, said transmitted electro-magnetic waves being at successive frequencies and each of said transmitted electro-magnetic waves being unmodulated, said antenna means receiving reflected electro-magnetic waves from said medium including said target, each of said reflected electro-magnetic waves corresponding to one of said transmitted electro-magnetic waves, and said antenna means converting said reflected electro-magnetic waves into respective received signals;

means for processing said received signals to produce a plurality of reflection coefficients, each of said reflection coefficients being for each of said number of perpendicular distances, for averaging said reflection coefficients over said number to obtain a true reflection coefficient, and for comparing said true reflection coefficient with known reflection coefficients for specific objects to output known characteristics of one of said specific objects which has a known reflection coefficient which best compares with said true reflection coefficient.