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Computed Tomography Physics, Instrumentation, and Imaging

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Presentation on theme: "Computed Tomography Physics, Instrumentation, and Imaging"— Presentation transcript:

1 Computed Tomography Physics, Instrumentation, and Imaging
Module F Computed Tomography Physics, Instrumentation, and Imaging

2 Disclaimer This workforce solution was funded by a grant awarded under the President’s Community-Based Job Training Grants as implemented by the U.S. Department of Labor’s Employment and Training Administration.  The solution was created by the grantee and does not necessarily reflect the official position of the U.S. Department of Labor.  The Department of Labor makes no guarantees, warranties, or assurances of any kind, express or implied, with respect to such information, including any information on linked sites and including, but not limited to, accuracy of the information or its completeness, timeliness, usefulness, adequacy, continued availability, or ownership.  This solution is copyrighted by the institution that created it.  Internal use by an organization and/or personal use by an individual for non-commercial purposes is permissible.  All other uses require the prior authorization of the copyright owner.

3 Pixels Represent segment of the anatomy scanned
Contain numerical information based on tissue density Two-dimensional representation Slice thickness turns pixels into voxels (volume elements) Expressed in Hounsfield units Hounsfield units are directly proportional to the attenuation coefficient of the tissue

4

5 Windowing and Leveling
The process of “windowing” in CT Defines the shades of gray of interest.

6 Water Cerebrospinal fluid Tumors Blood (fresh) Blood (coagulated) Brain (white matter) – 46 Brain (gray matter) – 40 Muscle/aorta – 50 Soft tissue – 70 ( liver, spleen, kidney, pancreas, etc. ) Bone (average) – 1000 Petrous bone Air Lung tissue – 400 Fat

7 Windowing and Leveling
Window level determines the center of the gray scale and is generally set at the average tissue density of the structures within the anatomy being scanned. Window width is normally set to include other structures or pathology that may also be located in the scan plane.

8 Water Cerebrospinal fluid Tumors Blood (fresh) Blood (coagulated) Brain (white matter) – 46 Brain (gray matter) – 40 Muscle/aorta – 50 Soft tissue – 70 ( liver, spleen, kidney, pancreas, etc. ) Bone (average) – 1000 Petrous bone Air Lung tissue – 400 Fat

9 Detectors Receive the attenuated x-ray photons
For detection to occur the attenuated photon must: Be captured by the detector chamber “collide” with an atom of the detector material “Collision” must produce an electromechanical conversion suitable for measurement Be able to be amplified and transmitted

10 Types of Detectors Gas Detectors Solid-state Detectors

11 Gas Detectors Xenon Inherent post-patient collimation 1 mm wide
Air-tight chambers Widely dispersed Xenon atoms Pressurized 30 times normal atmospheric pressure Sensitive to x-ray photons Generate electrical impulses Impulse is amplified and sent to ADC Digital signals sent to array processor NOT suitable for 4th generation CT scanners

12 Solid-State Detectors
Composed of numerous types of crystals Scintillation detectors Emit light in response to x-ray photons Convert the light into electrical signals using a photodiode Amplify the signals and transmit them to the ADC Sensitive to incoming attenuated photons Suitable for 3rd and 4th generation scanners

13 Hounsfield Units Also called CT number or an integer
An integer is assigned to each amplified electrical signal in the form of a Positive or Negative Whole number. The stronger the signal the greater the value of the integer

14 ADC ADC (Analog to Digital Converter)
Signals reaching the ADC are in analog form. Signals are converted to integers and sent to the Array Processor

15 Array Processor special purpose logical processing unit
used to perform rapid image reconstructions Computer computations solves all of the complex mathematical problems (reconstructive algorithms) Reconstructions, retrospectives, post processing techniques

16 Reconstructive Algorithms
Filtered-back projection Simple-back projection Convolution Convolution and filtered back projection are considered analytical reconstruction algorithm

17 Convolution Method Projection profiles are obtained
Logarithm of data obtained Logarithm values are multiplied by a digital or convolution filter (kernel) Filtered profiles are then back-projected Filtered profiles are added Results in “blur-free” images

18 Raw Data Convolution filters can only be applied to raw data or (scan data). Convolution filters can NOT use image data.

19 Image Data Image Data can be used for post-processing techniques:
3D reformations MIP’s Volume rendering etc.

20 Spiral CT The data is acquired in Volume rather than slice by slice.
Filtered-back projection cannot be used alone to generate images. Filtered-back-projection with linear interpolation is used as the reconstruction algorithm in single-detector-row spiral. (the exact process depends on the manufacturer)

21 Interpolation defined as a mathematical technique used to determine the value of a function from known values on either side of it. This is a mathematical estimation technique. Linear interpolation is the simplest form of interpolation.

22 Linear interpolation equation
Y3 = Y1 + (x3-x1)(Y2-Y1)(x2-x1) Multi-Detector rows Filtered-back-projection using interlaced sampling, longitudinal interpolation by Z-axis filtering, or ban-beam reconstruction is used in multi-detector-row CT scanning.

23 Spatial Resolution -the degree of blurring in an image
This is regarded as “the measure of the ability of a CT scanner to discriminate objects of varying densities located close together, against a uniform background”.

24 Spatial Resolution Represented by: Point Spread Function (PSF)
Line Spread Function (LSF) Modulation Transfer Function (MTF)

25 Geometric factors for Spatial resolution
Focal spot size Detector response curve Slice thickness Focal distance Iso-center (center of rotation of the gantry) Detector and sampling distance

26 Contrast resolution Contrast resolution, low-contrast resolution or tissue resolution is the ability of the CT scanner to demonstrate small changes in tissue contrast.

27 Factors which affect low-contrast resolution
Photon flux Slice thickness Patient size Detector sensitivity Reconstruction algorithm Image display Image recording Quantum noise

28 Reconstruction Limitations
The ability of the scanner to perform various reconstruction process is determined by the scanning parameters chosen by the Technologist as well as equipment characteristics!

29 Parameters Scan field of view (SFOV)
Reconstructed field of view (RFOV) (DFOV) Window settings Matrix size Slice thickness Radiographic tube output Scan time and rotational arch Focal spot size


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