Gantry
The gantry assembly is the largest of these systems. It is made up of all the equipment.
X-ray Tube Housing
Decreases leakage radiation to maximum level of 100 mR/hour at a distance of 1 meter
- Minimizes exposure dose to patient and radiographer
Provides mechanical support for x-ray tube
Oil circulates around x-ray tube
- Insulator protecting from electric shock
- Dissipates heat
Detectors
- The detectors in a CAT scanner measure radiation attenuated from the body structures due to their interaction with X-rays. Capture energy that has not been attenuated by the patient.
- Detectors Made up of multiple discrete cells or detectors.
Two types of detectors are used:
- Crystal Scintillation Detectors (Solid State Detectors) :
- Photodiode
- Photomultiplier Tubes
- Gas Filled Detectors
The detector array of more modern scanners uses tungsten plates, a ceramic substrate, and xenon gas.
Scintillation Detectors with photodiode (Crystal)
- Crystal converts incident x-rays to light
- Photodiode semiconductor current proportional to light
Coupled optically to photodiode
Materials Used:
- Calcium tungstate
- Sodium Iodide
- Bismuth Germanium Oxide
- Cesium Iodide
- Calcium tungstate + SI Photodiode (more frequent)
- Scintillation crystal detector used in III and IV gen. CT scanners
Scintillation crystals used with pm tubes
- X-ray energy converted to light
- Light converted to electrical signal
- Sodium Iodide – afterglow+ Hygroscopic+ Low dynamic range (used in the past)
- Calcium fluoride
- Cesium iodide(Csl)
- Bismuth geremanate
- Short decay time-afterglow not a problem
Scintillation crystal detector (PM Tube) used in I & II gen. CT scanners
Data Acquisition System
The DAS consists of the following parts:
Other scan configurations
Interest in faster scan times evolves from a desire to image moving structures such as, the wall of the heart and contrast material in blood vessel and heart chambers and to overcome motion artifacts due to cardiac rhythm and patient breathing
- Electron beam computed tomography
- Dynamic Spatial Reconstructor(DSR)
Fifth generation
Electron-beam computed tomography (EBCT)
- EBCT does not use an X-ray tube; instead it uses a beam of electrons generated outside the gantry.
- Inside the gantry there are 180-degree rows of fixed detectors on one side and 180 degrees of tungsten arcs opposite. The electron beam is rapidly moved to bombard the tungsten arcs, producing an x-ray beam.
- The x-rays then pass through the patient and transmission information is collected by the detectors. These units are very fast because they have no moving parts.
- For a number of years they were the only scanners fast enough for cardiac imaging. However, two additional developments resulted in significant scan time reduction and minimized the use of EBCTs.
- Developed for cardiac imaging, the EBCT reduces scan time to as little as 50 ms, fast enough to image the beating heart.
Scan modes
- Once the patient is on the table and the table is moved into the gantry, the technologist performs a preliminary scan called the CT radiograph. CT systems can scan anterior-posterior (AP), posterior-anterior (PA), or lateral.
There are 2 common scan modes:
Axial
Helical
Helical (Sixth Generation)
- The helical (also called spiral) scanning, the table moves at a constant speed while the gantry rotates around the patient. This geometry results in the X-ray source forming a helix around the patient.
- The advantage of helical scanning is speed—by eliminating the start/stop motion of the table as in axial CT, there are no inertial constraints to the procedure. Similar to the threads on a screw, the pitch describes the relative advancement of the CT table per rotation of the gantry.
Three technological developments:
- Slip-ring gantry designs
- Very high power x-ray tubes
- Interpolation algorithms to handle projection data
Pitch
- Pitch (P) is a term used in helical CT. It has two terminologies depending on whether single slice or multislice CT scanners are used.
Single slice CT (SSCT)
The term detector pitch is used and is defined as table distance traveled in one 360° gantry rotation divided by beam collimation.
For example, if the table traveled 5 mm in one rotation and the beam collimation was 5 mm then pitch equals 5 mm / 5 mm = 1.0.
Multislice CT (MSCT)
Beam pitch is defined as table distance traveled in one 360° gantry rotation divided by total thickness of all simultaneously acquired slices.
Choice of pitch affects both image quality and patient dose:
- P = 1.0: x-ray beams are contiguous for adjacent rotations
- P >1.0: x-ray beams are not contiguous for adjacent rotations, i.e. there are gaps in between the x-ray beams and tissue is not irradiated
- P <1.0: there is x-ray beam overlap; i.e. a volume of tissue is irradiated more than once per scan. Thus a pitch >1.0 results in decreased patient dose but also decreased image quality (through fewer projections obtained, resulting in lower SNR). A pitch of <1.0 results in better image quality, but a higher patient dose.
Seventh Generation of CT
Multidetector /Multislice /Multirow CT
- Most recent advancement, introduced in 1998.
- In 2000, 8 slice CT were presented, followed by 16 slice in 2001
- This uses usually 64-128 adjacent multiple detector arrays in conjunction with a helical CT scanner , the collimator spacing is wider and more of the x-rays that are produced by the tube are used in producing image data.
- Scanning time: 0.25 second
- The collimator spacing is wider and more of the x-rays that are produced by the tube are used in producing image data
Opening up the collimator in a single array scanner increases slice thickness, reducing spatial resolution in the slice thickness dimension
With multiple detector array scanners, slice thickness is determined by detector size, not by the collimator
PIXEL & VOXEL
- Cross sectional layer of the body is represented as an image matrix.
- Each square of the image matrix is called pixel(picture element) and it represents tiny block of tissue called voxel (volume element)
- The linear attenuation coefficient (µ) of each pixel is determined by:
- Composition of the voxel
- Thickness of the voxel µ
- Quality of the radiation beam