GB1582833A - Radiography - Google Patents

Radiography Download PDF

Info

Publication number
GB1582833A
GB1582833A GB1720476A GB1720476A GB1582833A GB 1582833 A GB1582833 A GB 1582833A GB 1720476 A GB1720476 A GB 1720476A GB 1720476 A GB1720476 A GB 1720476A GB 1582833 A GB1582833 A GB 1582833A
Authority
GB
United Kingdom
Prior art keywords
frame
axis
sub
main frame
radiation
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.)
Expired
Application number
GB1720476A
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
EMI Ltd
Original Assignee
EMI Ltd
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by EMI Ltd filed Critical EMI Ltd
Priority to GB1720476A priority Critical patent/GB1582833A/en
Priority to US05/948,301 priority patent/US4177382A/en
Publication of GB1582833A publication Critical patent/GB1582833A/en
Expired legal-status Critical Current

Links

Classifications

    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B6/00Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
    • A61B6/02Arrangements for diagnosis sequentially in different planes; Stereoscopic radiation diagnosis
    • A61B6/03Computed tomography [CT]
    • A61B6/032Transmission computed tomography [CT]
    • AHUMAN NECESSITIES
    • A61MEDICAL OR VETERINARY SCIENCE; HYGIENE
    • A61BDIAGNOSIS; SURGERY; IDENTIFICATION
    • A61B6/00Apparatus or devices for radiation diagnosis; Apparatus or devices for radiation diagnosis combined with radiation therapy equipment
    • A61B6/40Arrangements for generating radiation specially adapted for radiation diagnosis
    • A61B6/4021Arrangements for generating radiation specially adapted for radiation diagnosis involving movement of the focal spot

Landscapes

  • Health & Medical Sciences (AREA)
  • Life Sciences & Earth Sciences (AREA)
  • Engineering & Computer Science (AREA)
  • Medical Informatics (AREA)
  • Radiology & Medical Imaging (AREA)
  • Molecular Biology (AREA)
  • Biophysics (AREA)
  • Nuclear Medicine, Radiotherapy & Molecular Imaging (AREA)
  • Optics & Photonics (AREA)
  • Pathology (AREA)
  • Physics & Mathematics (AREA)
  • Biomedical Technology (AREA)
  • Heart & Thoracic Surgery (AREA)
  • High Energy & Nuclear Physics (AREA)
  • Surgery (AREA)
  • Animal Behavior & Ethology (AREA)
  • General Health & Medical Sciences (AREA)
  • Public Health (AREA)
  • Veterinary Medicine (AREA)
  • Pulmonology (AREA)
  • Theoretical Computer Science (AREA)
  • Apparatus For Radiation Diagnosis (AREA)

Description

(54) IMPROVEMENTS IN OR RELATING TO RADIOGRAPHY (71) We, E.M.I. LIMITED, a British company of Blyth Road, Hayes, Middlesex, do hereby declare the invention, for which we pray that a patent may be granted to us, and the method by which it is to be performed, to be particularly described in and by- the' following statement: The present invention relates to radiography, and it relates especially to that branch of radiography which has become known as computerised axial tomography. Apparatus for performing computerised axial tomography is described and claimed in British Patent Specification No. 1,283,915.
In essence, computerised axial tomography is performed by measuring the absorption suffered by x-radiation on traversing each of many substantially co-planar, pencil-like beam paths through a body and processing signals indicative of the various absorption values to evaluate the absorption coefficient, with respect to the radiation used, at each of a number of locations distributed over the irradiated plane of the body. The processing is preferably effected without transforming the absorption values out of the spatial domain, and suitable processing techniques are described in the aforémentioned British Patent Specification and in British Patent Specification No.
1,471,-531. A visual representation of the evaluated coefficients is provided in any convenient manner.
In some circumstances, it'is preferable to evaluate the absorption coefficients with high accuracy only for locations distributed over a particular region of interest in the body, instead of evaluating the coefficients over- an entire irradiated plane. This is particularly the case when the absorption coefficiènts have already been evaluated for locations' distributed over an irradiated plane and examination of the corresponding visual representation indicates that an anode maly exists at a certain region of the plane.
It is then desirable to obtain more detailed information about - the certain region, and possibly also its immediate surroundings.
This could be effected by further irradiating the region, either by a single examination with an increased radiation dosage or by effecting a number of examinations, each of relatively low dosage, and combining the information derived from all the examinations. These techniques, however, if effected in the originally irradiated plane of the body, are subject to a serious difficulty, namely that because the region of interest will, in almost all cases be disposed entirely within the body, and because of the attenuation of the radiation by the body tissue and other matter, such as bones, disposed outside the region of interest but in the irradiated plane, the radiation dosage through the region of interest which is necessary to provide the required accuracy of information for said region requires that the patient's skin be subjected to unacceptably high radiation dosages.
It is an object of this invention to provide the facility for obtaining accurate information about a selected region of the body without subjecting the patient's skin to unacceptably high radiation dosage.
According to the invention there is provided a method of radiographically examining the body of a patient, the method comprising the steps of: rotating a source of at least one substantially planar, fan-shaped distribution of Xradiation around said body about an axis extending internally and longitudinally of said body and intersecting said at least one distribution of X-radiation; detecting radiation emergent from the body along a plurality of substantially linear paths, within said at least one distribution, from each of à plurality of different angular locations, ar0und the body, adopted by the source during'its rotational movement; and causing the radiation to propagate into the body, from each of said locations, through one or more regions extending over a relatively large distance in the direction of said axis and through a common region of the body, in the vicinity of said axis, extending over a relatively small distance in said direction.
In order that the invention may be clearly understood and readily carried into effect, an embodimeht thereof will now be de scribed, by way of example only, with reference to the drawings filed with the Provisional Specification of which: Figure l(a) shows, in schematic, cross sectional view, radiological apparatus in accordance with one example of the inven tion, Figure 1 (b) shows a view taken on arrows B-B of Figure 1(a), Figure 2 shows, in perspective view, a typical arrangement of detectors and an attenuator, and Figure 3 shows an alternative embodi ment of the invention.
Referring now to Figures 1(a) and 1(b), a radiographical apparatus in accordance with one example of this invention comprises a main housing 1 which has a base 2 secured to the floor and which supports a two-part table 3, 4 which also is static. The main housing 1 is formed with an opening 5 to accommodate the body 6 of a patient to be examined; the body 6 being supported on a platter which is slidably movable relative to the table 3, 4 so t'hat the patient can be moved through the opening 5 to position the - body 6 appropriately for the examination.
The body 6 is strapped to the platter by means of a strap (not shown) of plastics material, the strap being preferably transpa rent to light, as well as to X-radiation, so that a mark on the body 6 'which indicates where the examination is to be made can be seen through the strap. This permits the body to be positioned properly by alignment of the mark with a finely focussed beam of light generated by a lamp (not shown) fixed to the main housing 1.
Fixedly mounted within the housing 1 is a main bearing support ring 8 which supports a main bearing 9 in which runs a circular frame 10. Frame 10 is formed with gear teeth 11 which co-operate with gear teeth 12 on a gear wheel driven by an electric motor 13. Mounted in the frame 10 so as to rotate th'erewith is a sub-frame 14. The sub-frame 14 is pivottably mounted to the frame 10 at two diametrically opposite locations such as 15 in Figure 1(b), and the angle of tilt of the sub-frame 14 relative to the frame 10 is controlled by a pair of actuators 16, only one of which can be seen in the drawing, which rotates with the frame 10 and urges against respective flanges such as 17 attached to the sub-frame 14.
The sub-frame 14 supports an X-ray source 18 and an array 19 of collimated radiation sensitive detectors such as sodium iodide scintillator crystals with associated photo-diodes or photo-multipliers. The col limators are shown at 19a. The array 19 typically contains a hundred or more detec tors.
The source 18 comprises an X-ray tube which emits a fan-like spread of radiation indicated at 20 in Figure 1(b); the centre line of the fan being shown at 21. The source 18 is preferably of the kind described in British Patent Specifications Nos. 1,529,799 and 1,558,062, i.e. in which the electron beam thereof can b scanned over the - X-ray producing target thereof to shift the fan of radiation, relative to the body, in a lateral direction. This not necessarily the case, however. If a scanned source is used, however, the line 21 represents the position occupied by the central beam of the fan when the electron beam position is half-way across the target.
Clearly the source has to be supplied with electrical, power and with coolant for- the target thereof, and the necessary cable connections are allowed for by means of a suitable cable handling system as indicated generally at 22 in Figure 1(a). Typically such a system is required to accommodate suffi cient cable to allow the source 18 to execute five or six revolutions about the body without stopping.
The apparatus can operate conventional ly, with the sub-frame 14 disposed so that the fan 20 is in a vertical plane, the motor, 18 being actuated to cause the source 18 and the detector array 19' to orbit around 'the body with the fan 20 remaining in a vertical plane, about an axis 23 which is horizontal and intersects the body longitudinally there of; that is the axis of frame 10. The scanning motion of the frame 10 and its attachments and the deflection of the electron beam of the X-ray source 18 are synchronised as described in either of the aforementioned British Patent Specifications Nos. 1,529,799 or 1,558,062 and the data so acquired are processed in the manner described in the appropriate one of the two specifications to evaluate the absorption coefficient at each of a plurality of locations distributed over the irradiated plane of the body.
Assuming however, that a visual repre sentation of the evaluated coefficients in a planar section of the body indicates a particular region in the interior of the body 6 which is deemed worthy of further investi -gation, the present invention is invoked to provide more detailed information about that region. The height and lateral position of the body 6 within - the opening 5 is adjusted so as to place the region . of particular interest as close as possible to the intersection of axis 23 and the line between the mountings 15.
The actuators 16 are then operated so as to tilt the sub-frame 14 by a predetermined angle within the frame 10. The angle of tilt used depends on a number of factors such as the operating conditions of, the X-ray source 11 and the resolution with which it is required to investigate the region of interest. The angle of tilt may in some circumstances be'has much as 40 , although: this would' not be possible with the dimensions shown in the drawing, where a tilt of about 25 can be accommodated.
With the angle of tilt having been selected by suitable operation of the actuators 16, the motor 13 is energised to cause the frame 10, and thus the sub-frame 14 and its attachments, to rotate around the body.
Because of the tilt introduced by the actuator 16, the source 18 and the detector array 19 rotate in respective vertical planes, the radiation being projected through the body along a figure of revolution which resembles an hour-glass; the waist of the hour-glass being arranged to coincide with the aforementioned region of interest within the patient's body. By adjusting the angle of tilt between successive revolutions of the frame 10, by means of the actuators 16, the radiation can be projected through the body along successive figures of revolution, all of which resemble hour-glasses with their waists being coincident, but the figures of revolution being of varying dimensions in the direction parallel to the actuator move ment. Thus, effectively, as the angle of tilt decreases; the planes of rotation of the source 18 and of the detector array 19 become closer together. In the limit, i.e.
when the'sub-frame 14 is disposed vertically within the frame 10, the figure of revolution is a single plane, which can be regarded as a completely flat hour-glass; the plane in tersecting the waists of the previously irradi ated figures' of revolution.
In practice, it is more convenient to cause the actuators 16 to vary the angle of tilt of the sub-frame' 14 relative to the frame 10 gradually and smoothly rather than step wise between successive revolutions as sug gested above. This introduces a slight distor tion into the irradiated figures of revolution but the distortion is not significant as it occurs mainly in the peripheral regions of the body, away from the region of interest.
Again, in practice, it is usual to cause the apparatus to rotate a number of times, say ten or twelve, about the patient whilst the patient remains in a fixed position, half of the revolutions being in one direction and half in the other. -In either case, the first revolution in one direction is used to accel erate the apparatus to its desired operation al speed and the last revolution in that direction is used for deceleration; the intermeditate revolutions in that direction (i.e.
three or four as the case may be) being used; for irradiating the body. It is desirable (though not absolutely necessary) for the irradiation to be effected symmetrically about the single vertical plane which is irradiated with the sub-frame 14 vertical.
Thus it is preferable to commence wth an angle of tilt of +a and, after the appropriate number of active revolutions, to end with an angle of tilt of -a", the sub-frame 14 having passed through the vertical position exactly half-way through the scanning sequ ence.
There would be little significance in attempting to use the absorption readings obtained from the detector array 19 during a single revolution of the frame 10 to evaluate the absorption coefficients of elements of the body disposed on the figure of revolu tion irradiated during that revolution, although this could be done if desired. It is preferable, however, to combine the absorption values derived at the same angu lar position of the frame 10 for each of the active revolutions thereof around the body, so as to synthesise data relating to waisted beam paths which are relatively broad in passing through peripheral regions of the body but narrow in passing through the aforementioned region of interest. These combined values (one for each detector at each of a large number, say five hundred, of angular positions of the frame 10 around the body) are processed, for example as de scribed in British Patent Specification No.
1,471,531, as if they were absorption read ings relating to a single plane. In practice, of course, the combined absorption readings relate to a concave lens-shaped region of the body; the thinnest part of the lens coinciding with the region of interest in the body.
The use of combined data as described above has advantages in regard to signal-to noise ratio and also enables the region of interest to be investigated with higher accur acy than the surrounding, peripheral regions of the body. This enables the absorption coefficients evaluated for said region of interest to be displayed on an enlarged scale (blown up in photographic parlance) if desired.
This advantageously increased accuracy of evaluation and higher resolution in the region of interest is achieved because that region is irradiated a number of times. A corresponding increase in dosage to a parti cular region of the skin is avoided however, by means of the invention, because the tilting action of the sub-frame 14 ensures that the radiation enters the body through different areas of skin during different revolutions of the scanning frame 10.
As an extra facility, which is available because of the provision of the tilting sub-frame 14, the actuators 16 can be caused to operate sinusoidally so that the source 18 and the detector array 19 can rotate around the body in a common plane which is tilted with respect to the vertical plane which would be irradiated with the sub-frame 14 vertical. All such tilted planes will, of course, intersect the region of interest of the body provided that this is located at the junction of the axis of rotation 23 of the frame 10 and the axis of tilt. The sinusoidal movement of the actuators 16 is synchronous with the rotation of frame 10, so that precisely one cycle of the sinusoidal motion occurs during one revolution of the frame 10. The angle of tilt relative to the aforementioned vertical plane is determined by the amplitude of the sinusoidal motion, whereas the attitude of tilted plane is determined by the phase of the sinusoidal motion relative to the rotation of frame 10.
It will be appreciated that a display of the absorption coefficients disposed on an inclined plane in the body can be useful in determining the extent and/or shape of an anomaly discovered in an examination of a corresponding display for a vertical plane.
As the detectors towards the extremities of the array 19 are not required to provide highly defined information, they can be made larger than the detectors in the centre of the array, with corresponding reduction in associated circuits and equipment. This broad principle is disclosed in British Patent specification No. 1,478,123, which describes and claims an arrangement in which the spacing and/or size of detectors increases towards the extremities of an array adapted to receive radiation projected along a fanshaped beam. In the present case, the detectors are also made larger in the direction perpendicular to the fan, as shown in highly schematic form in Figure 2 to fit the hour-glass shape of the cross section irradiated. The outer detectors of the array 19 thus have a large collecting surface for X-rays from the source 18 and accordingly it is possible to attenuate the X-radiation at the edges of the fan quite considerably (e.g.
by a factor of 100) as compared with the attentuation of X-radiation in the centre of the fan by means of an attenuator 24 of the kind shown in Figure 2; this attenuator being interposed between the source 18 and the patient's body to further reduce the dosage of radiation to the patient's skin.
In order to reduce the extent of the housing 1, to reduce the risk of causing concern to patients having claustrophobic tendencies, whilst still permitting the required amount of tilt of the sub-frame 14 relative to the frame 10, it can be advantageous to turn the X-ray tube 18 through 90" so that the aspect presented by the X-ray tube in the view of Figure 1(a) would be similar to that presented in the view of Figure 1(b), except that it would probably be turned through 1800 with respect to the position shown in Figure 1(b). This would mean that the thinnest profile of the tube would lie in the direction of tilt.
As described hitherto, the array 12 has comprised a single array of detectors, but if the source 11 is arranged to produce a square, pyramidal shaped beam of radiation then several arrays of such defectors could be used, so as to enable a number of angled planes to be irradiated at one and the same time.
In the event that the region of particular interest in the body in closely adjacent the skin (for example if the spine is to be studied), it can be advantageous to cause the unit 10 and its attachments td only usefully rotate through say 1800 or more in each plane, by turning off the X-ray tube during part of the rotation. The arrangement is made such that the radiation never meters the body through the back of the patient in the region of the spine. This reduces radiation dosage to the skin behind the spine.
In another embodiment of the invention, as shown in schematic side elevation in Figure 3, the use of the tilting sub-frame 14 (Figure la) and the necessity for the source and detectors to perform multiple rotations about the patient, are avoided by using instead of the X-ray tube 18 (Figure la) an X-ray tube 25 having a long line focus, say eighteen inches long, measured in a direction parallel to the axis 23 (Figure la).
Suitable collimators are used, as indicated at 26, to focus the X-rays from the tube 25 at the centre of the patient's body. The detectors 27 would 'comprise, say, 400 detector elements, each eighteen inches long to allow for the divergence of the X-rays after they - have traversed the centre of the body. It will be understood that the source tube 25 produces a fan-shaped swath of radiation, extending into and out of the plane of Figure 3, at each point along the anode thereof. The detectors 27 accordingly extend above and below the plane of the Figure. As a compromise between the arrangement just described and that described with respect to Figure 1, the source 25 could be such as to have an elongated anode of the kind shown in Figure 3 but, instead of this anode representing a line focus which simultaneously produces several fan-shaped swaths of the radiation, the electron beam of the X-ray tube is focused at a single point of the anode and the beam can be deflected so that said point' moves along the anode. This techniques would avoid the need for the tilting sub-frame 14 required with the Figure 1 arrangement but would require that the source and detectors execute multiple rotations around the patient as the deflection would be such as to hold the said point in one position on said anode for one revolution, to shift said point for the next revolution and so-on. A fixed bank of source collimators such as those shown in Figure 3 would be used.
An alternative technique for achieving the aim of the invention is to demount the main housing 1 from the bed 3, 4 and to rigidly fix the frame 10 relative to said housing. The entire main housing and contents can then be mounted on vertical and horizontal gimbals which can be driven by suitable actuators to effect the required angle or angles of tilt.
WHAT WE CLAIM IS; 1. A method of radiographically examining the body of a patient, the method comprising the steps of: rotating a source of at least one substantially planar, fan-shaped distribution of Xradiation around said body about an axis extending internally and longitudinally of said body and intersecting said at least one distribution of X-radiation; detecting radiation emergent from the body along a plurality of substantially linear paths, within said at least one distribution, from each of a plurality of different angular locations, around the body, adopted by the source during its rotational movement; and causing the radiation to propagate into the body, from each of said locations, through one or more regions extending over a relatively large distance in the direction of said axis and through a common region of the body, in the vicinity of said axis, extending over a relatively small distance in said direction.
2. Apparatus for carrying out the method according to Claim 1 wherein said rotating step is effected by rotating means which comprises a main frame having an aperture of sufficient size to accommodate said body, means for rotating said main frame about said axis, said axis passing through said aperture, a sub-frame secured to said main frame for rotation therewith, said sub-frame having an aperture of sufficient size to accommodate said body means mounting said generating means and said detector means to said sub-frame and tilt means for controllably tilting said sub frame, relative to said main frame, in a direction substantially parallel to said axis.
3. Apparatus according to Claim 2 in cluding two pivotal mounts, disposed at diametrically opposite locations of said main frame, by means of which said sub-frame is pivotably mounted to said main frame.
4. Apparatus according to either of claims 2 or 3 wherein said tilt means includes a pair of actuators.
5. Apparatus according to any of claims 2-4 wherein, in operation, the angle of tilt of said sub-frame relative to said main frame is held substantially constant for a first revolution of said main frame about said axis and is changed for the next and for each subsequent revolution.
6. Apparatus according to any of claims 2-4 wherein, in operation, the angle of tilt of said sub-frame relative to said main frames changed gradually during revolution of said main frame about said axis.
7. Apparatus for carrying out the method according to claim 1 wherein said source includes an X-ray tube having an X-ray emissive anode which is elongated in a direction substantially parallel to said axis and collimator means for selecting, from the X-radiation emitted by said elongated anode, a plurality of mutually inclined, substantially planar, fan-shaped distributions of X-radiation each directed towards a respective detector means.
8. Apparatus according to Claim 7 wherein said distributions are generated simultaneously.
9. Apparatus according to claim 7 wherein said distributions are generated sequentially,'one for each of a number of successive revolutions of said main frame about said axis.
10. Radiographic apparatus substantially as herein described with reference to Figures 1(a) and 1(b) of the drawings filed with the Provisional Specification or modified as herein described with reference to Figures 2 or 3 of the drawings filed with the Provisional Specification.
**WARNING** end of DESC field may overlap start of CLMS **.

Claims (10)

**WARNING** start of CLMS field may overlap end of DESC **. required with the Figure 1 arrangement but would require that the source and detectors execute multiple rotations around the patient as the deflection would be such as to hold the said point in one position on said anode for one revolution, to shift said point for the next revolution and so-on. A fixed bank of source collimators such as those shown in Figure 3 would be used. An alternative technique for achieving the aim of the invention is to demount the main housing 1 from the bed 3, 4 and to rigidly fix the frame 10 relative to said housing. The entire main housing and contents can then be mounted on vertical and horizontal gimbals which can be driven by suitable actuators to effect the required angle or angles of tilt. WHAT WE CLAIM IS;
1. A method of radiographically examining the body of a patient, the method comprising the steps of: rotating a source of at least one substantially planar, fan-shaped distribution of Xradiation around said body about an axis extending internally and longitudinally of said body and intersecting said at least one distribution of X-radiation; detecting radiation emergent from the body along a plurality of substantially linear paths, within said at least one distribution, from each of a plurality of different angular locations, around the body, adopted by the source during its rotational movement; and causing the radiation to propagate into the body, from each of said locations, through one or more regions extending over a relatively large distance in the direction of said axis and through a common region of the body, in the vicinity of said axis, extending over a relatively small distance in said direction.
2. Apparatus for carrying out the method according to Claim 1 wherein said rotating step is effected by rotating means which comprises a main frame having an aperture of sufficient size to accommodate said body, means for rotating said main frame about said axis, said axis passing through said aperture, a sub-frame secured to said main frame for rotation therewith, said sub-frame having an aperture of sufficient size to accommodate said body means mounting said generating means and said detector means to said sub-frame and tilt means for controllably tilting said sub frame, relative to said main frame, in a direction substantially parallel to said axis.
3. Apparatus according to Claim 2 in cluding two pivotal mounts, disposed at diametrically opposite locations of said main frame, by means of which said sub-frame is pivotably mounted to said main frame.
4. Apparatus according to either of claims 2 or 3 wherein said tilt means includes a pair of actuators.
5. Apparatus according to any of claims 2-4 wherein, in operation, the angle of tilt of said sub-frame relative to said main frame is held substantially constant for a first revolution of said main frame about said axis and is changed for the next and for each subsequent revolution.
6. Apparatus according to any of claims 2-4 wherein, in operation, the angle of tilt of said sub-frame relative to said main frames changed gradually during revolution of said main frame about said axis.
7. Apparatus for carrying out the method according to claim 1 wherein said source includes an X-ray tube having an X-ray emissive anode which is elongated in a direction substantially parallel to said axis and collimator means for selecting, from the X-radiation emitted by said elongated anode, a plurality of mutually inclined, substantially planar, fan-shaped distributions of X-radiation each directed towards a respective detector means.
8. Apparatus according to Claim 7 wherein said distributions are generated simultaneously.
9. Apparatus according to claim 7 wherein said distributions are generated sequentially,'one for each of a number of successive revolutions of said main frame about said axis.
10. Radiographic apparatus substantially as herein described with reference to Figures 1(a) and 1(b) of the drawings filed with the Provisional Specification or modified as herein described with reference to Figures 2 or 3 of the drawings filed with the Provisional Specification.
GB1720476A 1976-04-28 1976-04-28 Radiography Expired GB1582833A (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
GB1720476A GB1582833A (en) 1976-04-28 1976-04-28 Radiography
US05/948,301 US4177382A (en) 1976-04-28 1978-10-03 Radiography

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
GB1720476A GB1582833A (en) 1976-04-28 1976-04-28 Radiography

Publications (1)

Publication Number Publication Date
GB1582833A true GB1582833A (en) 1981-01-14

Family

ID=10091054

Family Applications (1)

Application Number Title Priority Date Filing Date
GB1720476A Expired GB1582833A (en) 1976-04-28 1976-04-28 Radiography

Country Status (1)

Country Link
GB (1) GB1582833A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2538114A1 (en) * 1982-12-20 1984-06-22 Commissariat Energie Atomique FILM TOMOGRAPHY METHOD AND DEVICE
WO2008053402A1 (en) * 2006-11-03 2008-05-08 Koninklijke Philips Electronics N.V. Multiple rotation c-arm

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2538114A1 (en) * 1982-12-20 1984-06-22 Commissariat Energie Atomique FILM TOMOGRAPHY METHOD AND DEVICE
EP0115721A1 (en) * 1982-12-20 1984-08-15 Commissariat à l'Energie Atomique Method and apparatus for tomography
WO2008053402A1 (en) * 2006-11-03 2008-05-08 Koninklijke Philips Electronics N.V. Multiple rotation c-arm
US8047715B2 (en) 2006-11-03 2011-11-01 Koninklijke Philips Electronics N.V. Multiple rotation C-arm

Similar Documents

Publication Publication Date Title
US4296329A (en) Alignment device for computerized tomography phantoms
US5023895A (en) Three dimensional tomographic system
US4117337A (en) Patient positioning indication arrangement for a computed tomography system
US6674834B1 (en) Phantom and method for evaluating calcium scoring
US7778383B2 (en) Effective dual-energy x-ray attenuation measurement
EP1016375B1 (en) Imaging system for generating high quality images
US4384209A (en) Method of and device for determining the contour of a body by means of radiation scattered by the body
JP4545144B2 (en) Computer controlled tomographic imaging system
KR101477543B1 (en) APPARATUS AND METHOD OF PHOTOGRAPHING USING X-ray
US4538289A (en) Reflective alignment light for computerized tomography
US20060153328A1 (en) Computed tomography device and method with three-dimensional backprojection
JPH1043172A (en) Method and device for preparing tomography synthesized photographic image
JPH0228818B2 (en)
JPS63501735A (en) Improved X-ray attenuation method and device
US4914588A (en) Computer tomography apparatus for generating an image of a portion of a sectional slice of a subject for use with a lithotripsy apparatus
JPH09285462A (en) Computer for computer type tomography system
US4138611A (en) Fan beam CT apparatus with post-processing weighting of picture element signals
JPH06181918A (en) Transmission type three-dimenisonal tomograph
US4177382A (en) Radiography
JP2825352B2 (en) CT device
JP2002000589A (en) Method and system for positioning radiology apparatus
CA1071773A (en) Method and apparatus for computerized tomography
GB1589469A (en) Radiography
GB1582833A (en) Radiography
WO1992006636A1 (en) Three-dimensional tomographic system

Legal Events

Date Code Title Description
PS Patent sealed
732 Registration of transactions, instruments or events in the register (sect. 32/1977)
PCNP Patent ceased through non-payment of renewal fee