Showing posts with label Physics. Show all posts
Showing posts with label Physics. Show all posts

December 21, 2010

Dual Energy CT (2)

One Basic Reason for Use of Dual Energy CT: Material Differentiation

  • By scanning a patient at two different energy spectra (on an example above, at 56 kV and 76 kV), the attenuation difference of the same material is different.
  • Iodine has higher attenuation difference, compared to bone
  • With this nature, scanning allows the computer to process bone and iodine content on images differently.
Routine Use of Dual-energy CT for Material Differentiation
  • Creation of 3D vascular images ("Direct Angio") by easy removal of bony structures
  • Plaque analysis (calcified vs. soft plaques)
  • Lung perfusion
  • Virtual unenhanced scan (creation of unenhanced scan from enhanced images by deleting iodine content from the images)
  • Calculi characterization (uric acid vs. others)

Reference: Fletcher JG, Takahashi N, Hartman R, et al. Dual-energy and dual-source CT: is there a role in the abdomen and pelvis? Radiol Clin N Am 2009; 47:41-57.

December 18, 2010

Dual Energy CT (1)


A Growing Need for a New Kind of CT
  • We need a better delineation of tissue components than just simple Hounsfield Units
  • We need to scan faster to image the beating heart (decrease temporal resolution), esp. in cases with high heart rate, irregular heart rate
What Is Dual Energy CT?
  • CT that uses the data of two different energy spectra to display anatomy and physiology (regular CT scans utilize one energy spectrum to create images)
  • Dual-source CT describes CT that has two x-ray sources and two detectors mounted on a single gantry. The x-ray sources can produce two different energy spectra, or one spectrum. Dual-source CT can run in either dual- or single-energy mode
What Are Possible Hardware Configurations for Dual Energy CT?
  • Two x-ray sources (dual-source CT)
  • Rapid kV switching (single-source CT)
  • Sandwich detector CT (two layers of detectors detecting x-rays at different energy spectra)
Image credit: medical.siemens.com

Reference:
Fletcher JG, Takahashi N, Hartman R, et al. Dual-energy and dual-source CT: is there a role in the abdomen and pelvis? Radiol Clin N Am 2009; 47:41-57.

April 3, 2010

CT Slice Thickness

Single Detector Array Scanners

  • Determined by physical collimation of the x-ray beam (green structure in the picture)
  • As this gap widens, the slice thickness increases
  • Upper limit of slice thickness depends on the width of the detector
Multiple Detector Array Scanners
  • Determined by width of the detectors (between blue lines in the picture)
  • Width of the detectors can be changed by 'binning' different numbers of individual detector elements together
  • Can be used in conventional axial scanning (no table movement) and in helical scanning protocols
Tradeoffs Respect to Slice Thickness
  • Number of detected x-ray photons increases linearly with slice thickness, for scans performed at the same kV and mAs
  • As number of detected x-ray photons increases, the signal-to-noise ratio (SNR) increases.
  • Higher SNR means better contrast resolution
  • Example: going from a 1-mm to 3-mm slice thickness triples the number of detected photons, and the SNR increases by square root of 3 = 73%
  • Increased slice thickness will reduce spatial resolution and increase volume averaging in the thickness dimension
References:
Bushberg, et al. Essential Physics of Medical Imaging, 2nd ed, 2001

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September 18, 2009

Acoustic Noise in MRI

Acoustic (Sound) Noise in MRI

  • One of the most disturbing obstacles for patients receiving an MRI particularly children and psychiatric patients
  • Interferes with communication between MRI technologists and patients
  • Interferes with functional MRI studies by producing unwanted stimulus. Noise may introduce changes in oxygenation in cortex and blood capillaries that may in turn affect signal receiving during fMRI.
  • They were anecdotal reports of temporary hearing loss related to MRI, but these have never been proven.
  • Depends on pulse sequence, types of scanner (coil structures and coil supports)
  • Average relative noise = 94-107 dB (in MRI bore) and 87-98 dB (in MR scanning room)
  • Noise from gradient recalled echo (GRE) sequences typically is louder than spin echo (SE) and echo planar imaging (EPI).
Etiology
  • Main source: Lorentz forces acting on gradient coils and pulsing particularly two gradients along x- (frequency encode) and y- (phase encode) axes
  • Other sources: vibrations of conducting cryostat inner bore of MR machine due to eddy current, vibrations of radiofrequency body coil, etc (including several "unknown" pathways)

Image from www.noise-busters.com

References:
1. Cho ZH, Park SH, Kim JH, et al. Analysis of acoustic noise in MRI. Magn Reson Imaging 1997;15:815-822.
2. Edelstein WA, Hedeen RA, Mallozzi RP, et al. Making MRI quieter. Magn Reson Imaging 2002; 20:155-163.

December 16, 2008

Hounsfield Unit

What is Hounsfield Unit?

  • CT number
  • Unit used to measure attenuation of tissue on CT
  • A representative of relative attenuation coefficient of tissues, using water as a reference
  • Water is defined as zero Hounsfield unit
  • Matters with higher physical density (g/cm3), higher electron density (e/cm3) than water will have higher HU; and vice versa
  • HU depends on kV peak (used in CT image acquisition) and filtration technique (used in CT image reconstruction)
  • HU values on an image are only approximate (because it will change if kV changes)
Who is Hounsfield?
  • Godfrey Hounsfield is a British electrical engineer
  • He shared a 1979 Nobel Prize in physiology or medicine with Allan Cormack for the development of computed tomography (CT)
Reference:
Huda W, et al. Review of radiology physics. 2003

www.wikipedia.com

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