* Your assessment is very important for improving the workof artificial intelligence, which forms the content of this project
Download APPLICATION OF THE ABOVE TO RADIOGRAPHY
Electromagnetism wikipedia , lookup
Magnetotactic bacteria wikipedia , lookup
Electromagnet wikipedia , lookup
Magnetoreception wikipedia , lookup
Magnetotellurics wikipedia , lookup
Electromagnetic field wikipedia , lookup
History of geomagnetism wikipedia , lookup
APPLICATION OF THE ABOVE TO RADIOGRAPHY In radiography the X-rays are going to pass right through parts of the body, in order to create images of the inside. Softer components of the total beam leaving the tube, say in the 20 keV region, would have a linear attenuation coefficient of about 79 m-1 in soft tissue. From this you can show that only about 0.04% of these photons would penetrate through 10 cm of the body. (The equivalent figures for 150 keV photons are 15 m -1 and 22%) These photons would be worse than useless because their ionising effect on the tissue would produce damage. Therefore we want to make the radiation harder by filtration before it reaches the body of the patient. Some of the lower energy photons will not get through the wall of the tube, but more filtering is needed. To get the filtering effect, we use the fact that photoelectric absorption increases as Z3, while simple and Compton scattering increase less rapidly. Hence we choose a filter with large enough Z so that most of the absorption in it will be by the photoelectric effect Aluminium turns out to be suitable. Since photoelectric absorption decreases very rapidly with photon energy, the higher energy photons will tend to survive. The energy range we try to establish is up to about 30 keV. (This requires that we have a tube voltage of about 900 kV; the glass wall is equivalent to about 1 mm of Aluminium, and another few mm of Aluminium are needed as the rest of the filter) The X-rays will pass far more easily through air spaces in the body, because as the density of the medium decreases we have seen that attenuation decreases - there are less atoms present per unit volume for the photons to hit. The average proton number Z of renal tissue and of fatty tissue, are approximately the same - about 6 or 7. But since absorption increases with density we can distinguish the kidney from the superficial layer of fat surrounding it. Muscle has a larger Z than the above soft tissues - about 7.5, while bone is larger still (about 13 to 14), as well as being denser, so their attenuation coefficient is further enlarged - they show up very clearly on the radiograph. Above 30 keV photon energy, Compton scattering is the dominant process of absorption, which is roughly independent of Z so discrimination would rely on density differences alone. But if we can use photons filtered into the region below 30 keV (see above), then simple scattering and the photoelectric effect will predominate; these increase rapidly as Z increases, and therefore will discriminate well between bones and soft tissues. In the radiogram, regions of high attenuation (bone) appear white, medium (tissue) appear grey, and negligible (air) appear black. Natural contrast is sufficient for the diagnosis of fractures and dislocations of bones. If the natural contrast offered by the relevant body parts under study is insufficient, artificial contrast agents may be used. For example, the radio-opaque barium sulphate in an aqueous suspension is widely administered for gastrointestinal tract examinations. When the diagnosis concerns a hand, it can be immobilised and an exposure of several seconds is possible without movement, and hence without blurring. But when a stomach is to be investigated, its involuntary movements would cause the radiograph to be uselessly blurred unless the exposure time is less than 0.5 s. To achieve this and still get good contrast on the exposure, the intensity of the beam has to be increased, which means increasing the current through the tube. Grid to reduce detection of scattered radiation Compton scattering of X-rays from tissue and bones leads to a generalised spread of radiation uniformly across the film. This is useless for diagnosis; it merely reduces the contrast between the dark and light regions on the film. The simplest way to prevent these scattered X-rays reaching the film is to arrange a grid of lead sheets, so arranged that only rays which are travelling more or less in the original direction can get through. Since the grid inevitably also absorbs some of the directed X-rays, the intensity of the original beam unfortunately needs to be increased to compensate. The grid is made of many long parallel strips of lead held together by an interspace material transparent to X-rays; there are about three strips of lead per mm., each one being about 0.05 mm thick and 5 mm deep (this depth is vital to the function of absorbing radiation that is going in the 'wrong' direction. X-RAYS FOR TREATMENT X-ray Megavoltage Radiotherapy: The 70 keV X-rays are used for diagnosis , hoping to affect the person's body as little as possible. X-rays produced by electrons that have been accelerated through more than 1 MV will be energetic enough to pass through the body without showing up useful detail of bones and muscle. Instead of diagnosis, they can be used for treatment , for therapy - in particular, for the destruction of cancers. The beam of X-rays is collimated, using, say, lead cylinders with holes drilled in them. Then it is aimed at the cancer, within the body. The beam will damage and kill the cancerous cells, but unfortunately it will equally damage and kill the healthy cells that it meets along the path through the body. Various methods of reducing this collateral damage are used: (i) Several beams can be used simultaneously, aiming at the cancer from different directions, only crossing at the cancer. (ii) The critical dose is carefully assessed; the patient is given the treatment which is only just enough to kill the cancer cells. (iii) The body is given time to recover, to repair damage, caused by the Xrays to previously healthy cells; clearly this is a compromise, since the cancer may also recover (iv) The patient, or the X-ray machine, can be rotated , so that the beam is aimed at the cancer from various directions, producing the same effect as (i). It might seem much easier to move the machine, but a megavoltage X-ray source is a sizeably machine; the patient can quite easily be strapped onto a couch and moved. Note that the energy of these X-ray photons is similar to that of g-ray photons; the two photons only differ in the way they are produced. {Grolier's Encyclopedia (CD-Rom): Malignant tissues are more sensitive than normal tissues to radiation exposure and can be treated if they have not spread throughout the body and are not surrounded by normal tissue that is especially sensitive to radiation, such as the spinal cord. Sophisticated physical and biological techniques are used for radiation therapy, often accompanied by computer analyses. A radiation therapist develops a treatment plan that permits the absorption of a fatal amount of radiation by all tumor cells but causes relatively minor damage to normal tissue. The usual mode of therapy is an external high-energy beam directed at the tumor site for a few minutes a day for 2 to 6 weeks, depending on the type of malignancy. X-rays, gamma rays, and such isotopes as cobalt-60 and iodine131 are often used} Nuclear Magnetic Resonance Imaging (NMR) This is a method of scanning parts of the body, including the brain, without using X-rays or Ultrasound. Very strong magnetic fields are produced using electromagnets in which the current-carrying coils are cooled low enough to become superconductors. The patient is put into a combination of a strong uniform magnetic field, and a non-uniform magnetic field which increases in strength across her body. Each nucleus of the atoms of the various elements in the body has a magnetic 'moment'; it behaves as a small magnet, and tends, therefore, to line up in the resultant magnetic field. The nucleus is now like a little compass, held in one position by the field of a magnet; it has a set of natural frequencies at which it would oscillate, if given the energy to do so (these are quantised, like the energy levels of an electron in an atom). If then a pulse of electromagnetic waves of various frequencies are projected into the body, the nucleus will 'pick up', absorb, and then re-radiate, just those photons of the electromagnetic radiation which are at the right energy. Thus the frequency absorbed and re-radiated is characteristic of the element. The absorption spectrum can be detected, and analysed to identify which kind of elements are present. Because the strength of the magnetic field varies across the body, the frequency absorbed and re-emitted by the same element also varies, in a predictable way. Therefore the position of the nucleus can also be worked out and displayed. By computer analysis, given, for example, the known combination of elements in various types of tissue, the cocktail of elements located at various positions can be converted into images on a computer monitor of the various tissues in the body. The different tissues can be given artificial colours by the computer, to aid visual recognition. {Grolier's Encyclopedia (CD-ROM): Magnetic resonance imaging (MRI) is a sophisticated medical diagnostic technique based on the principles of Nuclear Magnetic Resonance imaging. A patient is placed inside a cylinder that contains a strong magnet. Radio waves are then introduced into the cylinder, which cause the atoms of the body to resonate. Each type of body tissue emits characteristic signals from the nuclei of its atoms, and a computer translates these signals into a two-dimensional picture. Unlike traditional X rays or CAT scans {which use low-energy X-rays} used in Radiology, MRI does not use ionizing radiation. It also does not require the use of radioactively labeled dyes. In addition, MRI can see through bone and produce images of blood vessels, cerebrospinal fluid, cartilage, bone marrow, muscles, and ligaments. MRI is particularly useful to detect tumors in the posterior fossa (the region at the back of the brain between the ears), lesions associated with multiple sclerosis, joint injuries, and herniated disks. MRI is a harmless procedure except for persons with metal objects implanted in their bodies, such as pacemakers, joint pins, or artificial heart valves. These objects may be dislodged by the powerful magnetic field} {New Scientist CD-ROM: MRI works by subjecting the body to an intense magnetic field which causes the hydrogen nuclei in water in the body to line up like bar magnets. The nuclei are then slightly disturbed using pulses of radio waves. When the radio waves are removed, the nuclei relax back to their original state, giving off signals that depend on their chemical environment and their magnetic properties. Deoxygenated haemoglobin in the blood is paramagnetic, and so slightly distorts the magnetic field around it. Oxygenated haemoglobin is not paramagnetic, so appears different to deoxyhaemoglobin in an MRI image. This difference allows a type of scan called blood oxygen level dependent imaging, or BOLD. Seiji Ogawa at AT&T discovered BOLD in 1988. In 1991 researchers at Massachusetts General Hospital in Charlestown found they could image the brain by injecting a paramagnetic substance into the bloodstream. But this substance can prove toxic if used more than a few times. In these latest experiments the blood itself is imaged. David Tank of AT&T's biological computation research department says that when an area in the brain becomes more active, the blood flow to it increases. But the uptake of oxygen does not seem to change, so the amount of oxyhaemoglobin in the veins increases, and this is imaged by MRI.