GB2294604A - Thermal imaging using electro-magnetic induction - Google Patents
Thermal imaging using electro-magnetic induction Download PDFInfo
- Publication number
- GB2294604A GB2294604A GB9520969A GB9520969A GB2294604A GB 2294604 A GB2294604 A GB 2294604A GB 9520969 A GB9520969 A GB 9520969A GB 9520969 A GB9520969 A GB 9520969A GB 2294604 A GB2294604 A GB 2294604A
- Authority
- GB
- United Kingdom
- Prior art keywords
- waves
- screen
- resistive
- region
- imaging
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
- 230000005674 electromagnetic induction Effects 0.000 title 1
- 238000001931 thermography Methods 0.000 title 1
- 238000003384 imaging method Methods 0.000 claims abstract description 20
- 238000010438 heat treatment Methods 0.000 claims abstract description 5
- 238000000034 method Methods 0.000 claims description 10
- 239000002689 soil Substances 0.000 claims description 8
- 230000000694 effects Effects 0.000 claims 1
- 230000005284 excitation Effects 0.000 abstract 1
- 239000000463 material Substances 0.000 description 3
- 239000011248 coating agent Substances 0.000 description 1
- 238000000576 coating method Methods 0.000 description 1
- 238000005286 illumination Methods 0.000 description 1
- 238000007689 inspection Methods 0.000 description 1
- 239000004033 plastic Substances 0.000 description 1
- 229920003023 plastic Polymers 0.000 description 1
- 230000003252 repetitive effect Effects 0.000 description 1
Classifications
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J5/0003—Radiation pyrometry, e.g. infrared or optical thermometry for sensing the radiant heat transfer of samples, e.g. emittance meter
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N22/00—Investigating or analysing materials by the use of microwaves or radio waves, i.e. electromagnetic waves with a wavelength of one millimetre or more
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N25/00—Investigating or analyzing materials by the use of thermal means
- G01N25/72—Investigating presence of flaws
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V11/00—Prospecting or detecting by methods combining techniques covered by two or more of main groups G01V1/00 - G01V9/00
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01V—GEOPHYSICS; GRAVITATIONAL MEASUREMENTS; DETECTING MASSES OR OBJECTS; TAGS
- G01V8/00—Prospecting or detecting by optical means
- G01V8/005—Prospecting or detecting by optical means operating with millimetre waves, e.g. measuring the black losey radiation
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04N—PICTORIAL COMMUNICATION, e.g. TELEVISION
- H04N23/00—Cameras or camera modules comprising electronic image sensors; Control thereof
- H04N23/20—Cameras or camera modules comprising electronic image sensors; Control thereof for generating image signals from infrared radiation only
- H04N23/23—Cameras or camera modules comprising electronic image sensors; Control thereof for generating image signals from infrared radiation only from thermal infrared radiation
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01J—MEASUREMENT OF INTENSITY, VELOCITY, SPECTRAL CONTENT, POLARISATION, PHASE OR PULSE CHARACTERISTICS OF INFRARED, VISIBLE OR ULTRAVIOLET LIGHT; COLORIMETRY; RADIATION PYROMETRY
- G01J5/00—Radiation pyrometry, e.g. infrared or optical thermometry
- G01J2005/0077—Imaging
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Health & Medical Sciences (AREA)
- Life Sciences & Earth Sciences (AREA)
- Chemical & Material Sciences (AREA)
- Immunology (AREA)
- Multimedia (AREA)
- Geophysics (AREA)
- General Life Sciences & Earth Sciences (AREA)
- Engineering & Computer Science (AREA)
- Toxicology (AREA)
- Analytical Chemistry (AREA)
- Biochemistry (AREA)
- General Health & Medical Sciences (AREA)
- Signal Processing (AREA)
- Pathology (AREA)
- Electromagnetism (AREA)
- Spectroscopy & Molecular Physics (AREA)
- Radar Systems Or Details Thereof (AREA)
- Geophysics And Detection Of Objects (AREA)
Abstract
An imaging method comprises directing electromagnetic waves at a resistive surface 2 so as to induce currents within the surface and cause heating thereof. The resulting thermal image is observed by means of a thermal imager 3. Objects passing across the plane of these waves cause distortions in the thermal image from which the presence of an object 8 within an item of luggage 7 may be detected. A further embodiment (fig 3) invokes direct excitation of an object e.g. the ground (9) to detect the presence of objects (8) beneath its surface. <IMAGE>
Description
IMAGING METHOD AND SYSTEM
This invention relates to an imaging method and system, in particular though not exclusively, for use in locating hidden objects. Electromagnetic (EM) waves at frequencies lower than those of rnillimetric waves, and also low impedance magnetic waves of any frequency, have the ability to penetrate media such as soil or vegetation, and hence can be used for detecting the presence of reflective objects buried within the medium such as wires pipes and the like. The conventional way of designing such an imaging radar is to consider a plurality of antenna elements, each element corresponding to a single pixel in the subsequent radar image.
Such an array, along with the consequential signal amplifiers, is large complicated and expensive.
In a first aspect this invention provides an imaging method which comprises directing
EM waves at a region to be imaged in such a way as to form, on a resistive surface, a spatially varying interference pattern between EM waves reflected from an object within the region and
EM waves directly incident on the surface, and observing, using a thermal imager, the thermal image formed on the surface resulting from heating by the interference pattern.
As used herein the term "EM waves" is intended to encompass waves not only having a substantial electrical component, but also waves of a more magnetic nature having little or no such component. The resistive surface may be provided by a sheet of electrically resistive material, or may be the medium being investigated, for example soil.
The invention also provides an imaging system comprising a source of EM waves, a resistive surface within which currents can be induced by the source of EM waves to generate heat, and a thermal imager for imaging the heated surface.
Embodiments of the invention will now be described by way of example with reference to the accompanying drawings in which;
Figure 1 shows schematically a system according to one embodiment of the invention for use in imaging, for example, baggage at an airport;
Figure 2 shows a system according to another embodiment of the invention for use, for example, in detecting objects buried underground;
Figure 3 shows an alternative embodiment to that of Figure 2;
Figure 4 shows a yet further alternative embodiment to that of Figure 2; and
Figure 5 shows a still further embodiment of the invention incorporating means for generating a magnetic field; and
Figure 6 is a plan view of the resistive surface for use with the embodiment of Figure 5.
Referring to Figure 1 a source of EM waves 1 is arranged to illuminate a screen 2 formed from a thin resistive material. The EM waves may vary widely in frequency but are typically between 1 and 2GHz. The source 1 may be pulsed, repetitive or a single shot device. The screen 2 may be formed, e.g., from a plastics material having a thin metallic coating. A thermal imager 3 is located on the other side of the resistive sheet 2. The thermal imager 3 is connected to image processing equipment 4 and a display 5. The arrangement shown is suitable for use within a baggage inspection system where an item of luggage 7 within which a metallic object 8 is located passes through a beam of EM waves 6. A pattern is generated at the screen which is due to variations in density of the waves caused by scattering from the metallic object 8, and directly hitting the screen.Because of the resistance of the screen 2 the waves induce electrical conduction currents which are converted into heat, the heat pattern across the surface corresponding to the image density variations of the waves. By using a relatively short burst of high intensity waves, the heat pattern is formed in a time which is short compared to the thermal flows within the sheet 2. The heat pattern is captured by the thermal imager 3 before it diffuses away by the thermal flows. It is noted that in this respect the method differs from known methods in which thermal anomalies imaged occur as a result of heat flows, requiring heating of an object. In this invention thermal anomalies do not arise from the thermal properties of the object being imaged.The processor 4, knowing the features of the illumination such as wavelength and polarisation, calculates the boundary conditions giving rise to the pattern and an image of the object 8 is then displayed on the screen 5.
The embodiment shown in Figure 2 is intended for locating objects 8 buried below the ground or located on the surface, but hidden by vegetation. The arrangement is generally similar to that shown in Figure 1 and the same parts are identified by the same reference numerals. The resistive screen 2, which is partially transmissive, is located adjacent the ground with the thermal imager 3 and EM source 1 located on the same side above the screen. The arrangement is such that waves 6 pass through the screen 2 and into the soil 9 and are reflected from objects 8 onto the screen 2 to generate an interference pattem in the same way as that described with reference to Figure 1.
Figure 3 shows a variation in which no screen in used, instead the resistance of the soil, or other like medium 9, is used to create a surface heat pattern which is imaged and processed as described previously. The heat pattern is present within even a textured surface such as would be observed from vegetation 10. This texture may be substantially removed by image subtraction techniques. By taking one image frame just before the burst of electromagnetic energy, then a second frame just after the burst, subtraction of the two will leave only those areas which have changed temperature as a result of the electromagnetic waves.
The embodiment shown in Figure 4 is generally similar to that shown in Figure 2 except that the screen 2 is of smaller area and is located further away from the ground 9. A lens 11 is arranged to focus waves reflected from the ground 9.
In the embodiment shown in Figure 5 a coil 12 located beneath a resistive sheet 13 is arranged to generate magnetic waves, typically of the order of lKHz, which can be reflected from metallic objects 8 onto a resistive surface or screen 13. Because the waves are more magnetic in nature the screen 13 is constructed of a plurality of discrete or isolated resistive patches 14, as shown in Figure 6. Magnetic eddy currents are induced around the periphery of each patch and are then converted to heat, and in this way each patch 14 can be considered as a pixel element. The coil 12 could be located ahead of a vehicle so that large areas of ground could be quickly surveyed.
Claims (15)
1. An imaging method which comprises directing EM waves at a region to be imaged in
such a way as to form on a resistive surface a spatially varying interference pattern
between EM waves reflected from an object within the region and EM waves directly
incident on the surface, and observing, using a thermal imager, the thermal image
formed on the surface resulting from heating by the interference pattern.
2. An imaging method according to claim 1 in which the method comprises locating a
resistive screen to one side of a region to be imaged, directing the electromagnetic waves
through the region onto one side of the screen and observing the resultant thermal image
from the other side of the screen.
3. An imaging method according to claim 1 in which the method comprises locating a
partially transmissive resistive screen to one side of a region to be imaged, directing the
EM waves through from one side of the screen onto the region, and observing the
thermal image from the one side of the screen.
4. A method according to claim 1 which comprises directing the EM waves at soil, or a like
resistive medium, for imaging objects on or within the soil.
5. A method according to claim 4 which comprises the preliminary step of taking a thermal
image prior to directing the EM waves at the soil and subtracting the final image from
the preliminary image to remove the effects of vegetation located upon the soil.
6. A method according to claim 1 comprising locating the imager relative to the source of
EM waves such that the waves reflect from a region to be imaged and onto a resistive
screen designed to absorb substantially all of the incident EM energy.
7. A method according to claim 6 including the step of locating a lens to one side of the
screen so as to focus the incident EM energy.
8. A method according to claim 1 in which the EM waves are substantially magnetic waves
and in which the resistive surface comprises a screen subdivided into a plurality of
discrete regions, heating of the regions then being induced by eddy currents within each
region.
9. An imaging system comprising a source of EM waves, a resistive surface within which
currents can be induced by the source of EM waves to generate heat, and a thermal
imager for imaging the heated surface.
10. An imaging system according to claim 9 in which the resistive surface comprises a
screen, the EM source and thermal imager being located on opposite sides of the screen.
11. An imaging system according to claim 9 in which the resistive surface comprises a
screen, the EM source and the thermal imager both being located on the same side of the
screen.
12. An imaging system according to claim 9 or 10 in which a lens is located in front of the
resistive surface for focusing rays onto the surface.
13. An imaging system according to claim 9 in which the EM source is arranged to generate
magnetic waves and in which the resistive surface is sub divided into a plurality of
discrete regions.
14. An imaging method substantially as described with reference to any one of the drawings.
15. An imaging system substantially as described with reference to any one of the drawings.
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
GB9421493A GB9421493D0 (en) | 1994-10-24 | 1994-10-24 | Imaging method and system |
Publications (3)
Publication Number | Publication Date |
---|---|
GB9520969D0 GB9520969D0 (en) | 1995-12-13 |
GB2294604A true GB2294604A (en) | 1996-05-01 |
GB2294604B GB2294604B (en) | 1999-04-28 |
Family
ID=10763366
Family Applications (2)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB9421493A Pending GB9421493D0 (en) | 1994-10-24 | 1994-10-24 | Imaging method and system |
GB9520969A Expired - Fee Related GB2294604B (en) | 1994-10-24 | 1995-10-13 | Imaging method and system |
Family Applications Before (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
GB9421493A Pending GB9421493D0 (en) | 1994-10-24 | 1994-10-24 | Imaging method and system |
Country Status (3)
Country | Link |
---|---|
DE (1) | DE19539368A1 (en) |
FR (1) | FR2726145B1 (en) |
GB (2) | GB9421493D0 (en) |
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2003060561A1 (en) * | 2002-01-18 | 2003-07-24 | Intelligence Devices S.R.L. | Method and relevant device for revealing objects |
CN102607715A (en) * | 2012-04-11 | 2012-07-25 | 四川省众望科希盟科技有限公司 | Thermomagnetic imaging method and device |
WO2015002618A1 (en) | 2013-07-05 | 2015-01-08 | Gencer Nevzat Guneri | Method and system for dual-band active thermal imaging using multi-frequency currents |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2007358A (en) * | 1977-11-04 | 1979-05-16 | Elkem Spigerverket As | Method of flaw detection in metal members |
US4965451A (en) * | 1988-06-21 | 1990-10-23 | Soelter Hans Joachim | Method and apparatus for the contactless testing of the surface and inner structure of a solid workpiece |
GB2235604A (en) * | 1989-06-23 | 1991-03-06 | Atomic Energy Authority Uk | Transient thermography |
Family Cites Families (6)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
DE2917796C2 (en) * | 1979-05-03 | 1981-12-17 | Hochtief Ag Vorm. Gebr. Helfmann, 4300 Essen | Process and system for the determination of reinforcing bars in a reinforced concrete structure |
DE3824441A1 (en) * | 1988-07-19 | 1990-01-25 | Jastram Werke | Method and device for the identification of mines and of the earth surface contour and for making them visible |
JPH02184098A (en) * | 1989-01-10 | 1990-07-18 | Yoshiyuki Naito | Wide band radio wave absorber |
US5032727A (en) * | 1990-09-14 | 1991-07-16 | Digital Equipment Corporation | Product defect detection using thermal ratio analysis |
US5417494A (en) * | 1992-05-01 | 1995-05-23 | Exid, Inc. | Contactless testing of electronic materials and devices using microwaves |
JPH06235599A (en) * | 1993-02-09 | 1994-08-23 | Mitsubishi Heavy Ind Ltd | Mine surveying device |
-
1994
- 1994-10-24 GB GB9421493A patent/GB9421493D0/en active Pending
-
1995
- 1995-10-13 GB GB9520969A patent/GB2294604B/en not_active Expired - Fee Related
- 1995-10-23 DE DE19539368A patent/DE19539368A1/en not_active Withdrawn
- 1995-10-24 FR FR9512488A patent/FR2726145B1/en not_active Expired - Fee Related
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
GB2007358A (en) * | 1977-11-04 | 1979-05-16 | Elkem Spigerverket As | Method of flaw detection in metal members |
US4965451A (en) * | 1988-06-21 | 1990-10-23 | Soelter Hans Joachim | Method and apparatus for the contactless testing of the surface and inner structure of a solid workpiece |
GB2235604A (en) * | 1989-06-23 | 1991-03-06 | Atomic Energy Authority Uk | Transient thermography |
Non-Patent Citations (1)
Title |
---|
SPIE Volume 520 Thermosense VII,1984,pages 197 to 206 * |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2003060561A1 (en) * | 2002-01-18 | 2003-07-24 | Intelligence Devices S.R.L. | Method and relevant device for revealing objects |
JP2005517156A (en) * | 2002-01-18 | 2005-06-09 | インテリジェンス デバイセズ エス.アール.エル. | Method for revealing an object and related apparatus |
US7010455B2 (en) | 2002-01-18 | 2006-03-07 | Intelligence Devices S.R.L. | Method and relevant device for revealing objects |
CN102607715A (en) * | 2012-04-11 | 2012-07-25 | 四川省众望科希盟科技有限公司 | Thermomagnetic imaging method and device |
CN102607715B (en) * | 2012-04-11 | 2013-06-05 | 四川省众望科希盟科技有限公司 | Thermomagnetic imaging method and device |
WO2015002618A1 (en) | 2013-07-05 | 2015-01-08 | Gencer Nevzat Guneri | Method and system for dual-band active thermal imaging using multi-frequency currents |
US10123704B2 (en) | 2013-07-05 | 2018-11-13 | Nevzat Guneri Gencer | Method and system for dual-band active thermal imaging using multi-frequency currents |
Also Published As
Publication number | Publication date |
---|---|
FR2726145B1 (en) | 1998-03-27 |
GB2294604B (en) | 1999-04-28 |
GB9520969D0 (en) | 1995-12-13 |
DE19539368A1 (en) | 1996-08-14 |
GB9421493D0 (en) | 1994-12-07 |
FR2726145A1 (en) | 1996-04-26 |
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Legal Events
Date | Code | Title | Description |
---|---|---|---|
PCNP | Patent ceased through non-payment of renewal fee |
Effective date: 20011013 |