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CT Radiation Dose: Units and Measurement Methods Walter Huda PhD SUNY Upstate Medical University, Syracuse NY. Computed Tomography Dose Index (CTDI) Effective Dose Why is CT dose important?. Conventional radiography. x-ray skin dose 2 mGy/0.2 rad. Body CT scan. Head CT scan.
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CT Radiation Dose: Units and Measurement MethodsWalter Huda PhDSUNY Upstate Medical University, Syracuse NY
Computed Tomography • Dose Index (CTDI) • Effective Dose • Why is CT dose • important?
Conventional radiography x-ray skin dose 2 mGy/0.2 rad
Body CT scan Head CT scan
Cataracts Deterministic effect
Carcinogenesis Stochastic effect
In CT, CTDI is "radiation concentration" Effective dose is the "total radiation"
Dose distributions in CT measured in phantoms (center & periphery)
16 cm and • 32 cm • diameter • Acrylic • phantoms • = 1.19 Z = 6.56 100 mm ionization chamber
Computed Tomography Dose Index (CTDI) CTDI = 1/h D(z) dz
Integration limits for D(z) dz 7T for CTDIFDA 50 mm for CTDI100 CTDI100 = (f X L) /T f is exposure to dose factor X is measured exposure L is ionization chamber length T is slice thickness
CTDIw (weighted)CTDIw =(1/3 CTDI100)center + (2/3 CTDI100)periphery
CTDI100 is Proportional to mAsApproximately independent of slice thickness
CTDIw (mGy) 300 mAs/10 mm
Pitch of 1.0 has dose axial scan Pitch of 0.75 has 33% more dose Pitch of 1.5 has 66% less dose
Volume CTDIvol CTDIvol = CTDIw/Pitch Pitch defined as: Table distance traveled in 360 rotation Total collimated width of x-ray beam
Multi-slice CT ‘Overbeaming’ caused by wider collimator settings to avoid penumbral effects;
Body CTWIw values (300 mAs/120 kV)
Dose-length product (DLP)DLP = CTDIvol x Scan LengthDLP has units of mGy-cmGiven on console of some CTsCan be used to obtain effective dose E
CTDI is independent of section thickness T & number of sections N Patient risk does depend on section thickness T & number of sections N
Dose (risk) in CTis best measured by effective dose (E) E = i wi x Di
Moderately sensitive organs (wi = 0.05)BladderBreastLiverEsophagusThyroid
Organ doses can be measured in phantoms, or computed using MC
Effective doses can be estimated using DLP conversion factors mSv/mGy-cm Nagel HD: Radiation Exposure in CT (2001) cocir@zvei.org
Model patient as cylinder of waterDetermine energy impartedConvert energy imparted into effective dose Huda et al, Radiology 1997; 203:417-422
Head CT scan ~1 mSv 120 kVp 340 mAs 18 x 7 mm
Chest CT ~5 mSv 120 kVp 280 mAs 43 x 7 mm
Abdominal CT scan ~4 mSv 120 kVp 280 mAs 32 x 7 mm
Doses from CT are a major concern
Frequency of CT examinations Germany 1994
CT contribution to collective medical dose Germany 1994
In US HospitalsCT ~10% of examsCT contributes 2/3rd of patient doseFred Mettler – 2000 study in New Mexico
Dose is related to image quality
High dose scan Low dose scan
Doses should be As Low As Reasonably Achievable (ALARA) 120 kVp 5 mm 206 mAs
120 kVp 5 mm 43mAs C Small gas inclusion D ureter opacified c contrast A Metastasis in vertebral body B Subcutaneous gluteal metastatis
Conclusions The Beatles Godfrey Hounsfield
CTDI parametersquantify CT scanner dose characteristics,not patient dosesCTDIw & CTDIvol
Stochastic risks are important in CTDeterministic riskshould not occurDoses should be keptALARA
Effective doses in CT~1 mSv for head~5 mSv for bodyCT doses dominatemedical exposures
Radiation Dose in CTMF McNitt-GrayRadiographics (2002) 22:1541-1553