dr. gunn ct lecture

Upload: nurdzihan-drkic

Post on 04-Jun-2018

225 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/13/2019 Dr. Gunn CT Lecture

    1/75

    Computed Tomography:Physics considerations for

    Quality and Dose

    Martin Gunn

  • 8/13/2019 Dr. Gunn CT Lecture

    2/75

    Outline

    Frequency of CT

    Bioeffects of radiation

    Radiation dose in the ER

    Image noise and radiation dose

    kV and intravenous contrast Shielding

    Z -Overscanning

    Protocol design Prediction rules and utilization

    Special considerations

  • 8/13/2019 Dr. Gunn CT Lecture

    3/75

    USA CT Procedures / Year

    0.0

    10.0

    20.0

    30.0

    40.0

    50.0

    60.0

    70.0

    1993

    1994

    1995

    1996

    1997

    1998

    1999

    2000

    2001

    2002

    2003

    2004

    2005

    2006

    CT

    Scans(millions)

    Hospital Non-Hospital

    Annual Growth > 10% / year. Pop growth < 1% / year

    NCRP Scientific Committee 6-2, 2008

  • 8/13/2019 Dr. Gunn CT Lecture

    4/75

    CT Scanners Per Million Population

    CT Scanners /million (OECD)

    20.62005

    15.91995

    10.81990

  • 8/13/2019 Dr. Gunn CT Lecture

    5/75

    % of ED Evaluations involving CT

    Broder and Warshauer, Emergency Radiology Sept 2006 13: 25-30

  • 8/13/2019 Dr. Gunn CT Lecture

    6/75

    CT Utilization in the ER 2000-2005

    Broder and Warshauer, Emergency Radiology Sept 2006 13: 25-30

  • 8/13/2019 Dr. Gunn CT Lecture

    7/75

    Radiation Exposure in BWH

    Brigham and Womens Hospital, BostonMA

    Longitudinal study looking retrospectivelyat 22 years of data.

    190,712 CT exams in 31,462 patients.

    Mean 6.1 CTs (54 mSv), max 132CTs (1375 mSv).

    15% > 100 mSv 4% > 250 mSv

    1% > 400 mSv

    Sodickson et al, American Society of Emergency Radiology Annual Meeting, Oct 2008, Houston TX

  • 8/13/2019 Dr. Gunn CT Lecture

    8/75

    BWH Longitudinal CT Survey *

    Max 1/15 (6.7%)Max 1/8 (12.5%)

    Mean 1/509 (0.2%)Mean 1 / 320(0.3%)

    1% of patients >1/62 (1.6%)

    1% of patients > 1/38 (2.6%)

    3% of patients >

    1/100

    7% of patients > 1

    / 100

    CANCER

    MORTALITY

    CANCER

    INCIDENCE

    * Sodickson A, American Society of Emergency Radiology Annual Meeting, Oct 2008, Houston TX

  • 8/13/2019 Dr. Gunn CT Lecture

    9/75

    Diagnostic Accuracy

  • 8/13/2019 Dr. Gunn CT Lecture

    10/75

    Increasing Utilization of CT

    Diagnostic accuracy Cx spine, appendicitis, renal colic, multi

    rule out.

    Replacement of othermodalities:

    Volume of CT > study it replaces.

    Renal CT vol. > IVU vol. for renal colic

    Increased availability

    Clinicans and Staff: ? Reduced tolerance for diagnosticuncertainty or delay.

    More rapid patient throughput

  • 8/13/2019 Dr. Gunn CT Lecture

    11/75

    BEIR VII Report 2005

    Supports Linear No Threshold (LNT)Risk Model

    Risk model for cancer development:

    1 person / 1000 would develop cancer from10 mSv (CT Abdomen / Pelvis)

    Committee to assess health risks from exposure to low levels of ionizing radiation, NationaResearch Council (2005) Health risks from exposure to low levels of tadiation: BEIR VII phas

    2, National Academies, Washington DC.

  • 8/13/2019 Dr. Gunn CT Lecture

    12/75

    Relative Biological Risk of Cancer

    0 50 100 250150 200

    1.01

    1.02

    1.03

    1.04

    1.05

    1.06

    1.00

    1.07

    BIER VII ReportEffective Dose (mSv)

    Lifetimeattributable

    risk(LAR)

    Linear No Threshold(LNT)

    Linear ThresholdHormesis

  • 8/13/2019 Dr. Gunn CT Lecture

    13/75

    The following organizations believe that the currentevidence supports the Linear No Threshold (LNT)model of radiation induced cancer and hereditarydisease.

    International Commission on Radiation Protection (IRCP) United National Scientific Committee on Effects of Atomic

    Radiation (UNSCEAR) Radiation Protection Division of the UK Health Protection Agency

    (formerly NRPB).

    National Council on Radiation Protection (NCRP) (USA) National Academy of Science (USA). Environmental Protection Agency (USA).

    International Organizations Supporting LNT Theory

  • 8/13/2019 Dr. Gunn CT Lecture

    14/75

    Hormesis

    Greek: hormaein: to excite.

    Low levels of radiation exposure have a

    beneficial effect, lowering the rate ofcancer compared to no exposure. Theory is that a small radiation dose up-

    regulates DNA repair mechanisms, adaptiveresponse.

    Supported mostly by plant, protozoal andfungal studies, a few mouse studies, and a

    few human observational studies. Nearly all studies have serious problems.

  • 8/13/2019 Dr. Gunn CT Lecture

    15/75

    Hormesis: Position ofNational Academy of Sciences (BEIR VII)

    BIER VII: The assumption that any

    stimulatory hormetic effects from lowdoses of ionizing radiation will have asignificant health benefit to humans that

    exceeds potential detrimental effectsfrom the radiation exposure isunwarranted at this time.

  • 8/13/2019 Dr. Gunn CT Lecture

    16/75

  • 8/13/2019 Dr. Gunn CT Lecture

    17/75

    Evidence of Radiation Risks

    Studies of humans exposed toradiation.

    Mostly from Atomic bomb survivors fromHiroshima and Nagasaki.

    Radiation Effects Research Foundation (RERF) and theAtomic Bomb Casualty Commission (ABCC)

    Insufficient statistical power at lowradiation doses (< 50-100 mSv).

    Linear response above these levels.

    Cellular and animal studies used forlower levels.

    Latency problem: some cancers take20-30 years to develop.

    Lif ti Att ib t bl Ri k f C D th d

  • 8/13/2019 Dr. Gunn CT Lecture

    18/75

    Brenner et al, NEJM 2007 357: 2277

    Lifetime Attributable Risk of Cancer Death andAge: Abdominal CT

  • 8/13/2019 Dr. Gunn CT Lecture

    19/75

    Brenner et al, NEJM 2007 357: 2277

    Lifetime Attributable Risk of Cancer (10mGy)

  • 8/13/2019 Dr. Gunn CT Lecture

    20/75

    Availability Utilization.

    Need fordiagnostic certainty

    Concerns about

    radiationRegulation

    What can we do?1.Use technology to reduce radiation exposure.2.Image patients appropriately

    3.Track per scan and per patient radiation dose.

    CT Dilemmas

  • 8/13/2019 Dr. Gunn CT Lecture

    21/75

    CMS PQRI Test Measures 2008:

    T144: COMPUTED TOMOGRAPHY (CT)

    RADIATION DOSE REDUCTION Percentage of final reports for CTexaminations performed withdocumentation of use of appropriate

    radiation dose reduction devices ORmanual techniques for appropriatemoderation of exposure.

    CMS 2008 PQRI Test Measure Specificationhttp://www.cms.hhs.gov/PQRI/Downloads/PQRI2008TestMeasureSpecifications.pdf

  • 8/13/2019 Dr. Gunn CT Lecture

    22/75

    New technologies.

    Getting more for

    less.ALARA

  • 8/13/2019 Dr. Gunn CT Lecture

    23/75

    Tube Current Modulation

    b d l

  • 8/13/2019 Dr. Gunn CT Lecture

    24/75

    Tube Current Modulation

    Longitudinal Tube CurrentModulation

    Angular tube current modulation

    Combined (Angular-Longitudinal)

    Tube Current Modulation

    Cardiac CT:

    ECG synchronized tube currentmodulation.

    Prospective cardiac gating.

    Longitudinal Tube Current

  • 8/13/2019 Dr. Gunn CT Lecture

    25/75

    Longitudinal Tube CurrentModulation

    Tube Current

    Varies the tube current

    (mA) along the z-axis

    Different mA / dose

    applied to differentregions

    Scout series used tocalculate mA along z-axisto yield a pre-determined

    setting for image qualityGE = Noise Index . 0 380

    A l T b C M d l i

  • 8/13/2019 Dr. Gunn CT Lecture

    26/75

    Angular Tube Current Modulation

    Radiation output (mA) is adjusted tominimize dose in lower density profiles of

    the patients. Occurs during each tube rotation.

    mA

    C bi d D M d l ti

  • 8/13/2019 Dr. Gunn CT Lecture

    27/75

    z axis of scan

    Tub

    ecurre

    nt(mA)

    Combined Dose Modulation

    Fixed mA

    Dosetoo

    highwithfixedmA

    Dose too low with fixed m

    D S i

  • 8/13/2019 Dr. Gunn CT Lecture

    28/75

    Dose Savings:

    1. McCullough CH Radiographics 2006; 26: 503-5122. Hausleiter et al, Circulation. 2006;113:1305-1310

    3. Shuman et al, Radiology 2008;248:431-437

    Retrospective< 77%3ProspectiveTriggering

    Fixed mA< 40%2RetrospectiveGating

    Fixed mA0-45%1Combinedmodulation

    Comparedto:

    SavingTechnique

    ECG G t d T b C t M d l ti

  • 8/13/2019 Dr. Gunn CT Lecture

    29/75

    ECG Gated Tube Current Modulation

    High TubeCurrent

    Low TubeCurrent

    Tube current reduced during parts of the cardiaccycle when data not used for coronary CTA isobtained.Beam is on during the whole acquisition.

    ECG Gated Current Modulation

  • 8/13/2019 Dr. Gunn CT Lecture

    30/75

    ECG Gated Current Modulation

    mA

    Prospective ECG Triggering

  • 8/13/2019 Dr. Gunn CT Lecture

    31/75

    Prospective ECG Triggering

    Tube on Tube off

    X-ray beam is on about 25% of the R-R interval.Step and shoot technique.Predicts timing of next R-wave.Mean dose 6.2 mSv (2.3-11.9 mSv)1

    Shuman et al, Radiology 2008;248:431-437

    Table movement

    Prospective ECG Triggering

  • 8/13/2019 Dr. Gunn CT Lecture

    32/75

    Prospective ECG Triggering

    Prospective Gated CCTA

  • 8/13/2019 Dr. Gunn CT Lecture

    33/75

    Prospective Gated CCTA

    Partial Scan

  • 8/13/2019 Dr. Gunn CT Lecture

    34/75

    Partial Scan

    Tube is turned off for part of the rotation toavoid exposure to radiosensitive organs.

    Occurs during each tube rotation.

    Tube on for about 232 degrees.

    Fig C: Vollmer and Kalender, Eur Radiol. 2008 Aug;18(8):1674-82

    Dose Distribution

  • 8/13/2019 Dr. Gunn CT Lecture

    35/75

    Bismuth ShieldingZ Over-scanning

    Bismuth Shielding

  • 8/13/2019 Dr. Gunn CT Lecture

    36/75

    Bismuth Shielding

    Noise Distribution with Bismuth Shielding

  • 8/13/2019 Dr. Gunn CT Lecture

    37/75

    Noise Distribution with Bismuth Shielding

    Adapted from Vollmar and Kalender, Eur Radiol. 2008 Aug;18(8):1674-82

    Z- Over-scanning

  • 8/13/2019 Dr. Gunn CT Lecture

    38/75

    Primary beam exposure in areas aboveand below the scan range.

    Ends of the helix.

    Wider detector arrays and higher pitches.Overscan

    Top axial slice Bottom axial slice

    Z Over scanning

    Adaptive Collimation

  • 8/13/2019 Dr. Gunn CT Lecture

    39/75

    Adaptive Collimation

    Top axial slice Bottom axial slice

    Collimator Collimator

  • 8/13/2019 Dr. Gunn CT Lecture

    40/75

    Adjusting the ScanParameters:

    kVp / Dual Energy CTmA,

    Effective mAs or Noise IndexReconstruction kernel.

    Display window.Reconstruction thickness

  • 8/13/2019 Dr. Gunn CT Lecture

    41/75

    Changing the kVp and DECT

    kVp: Iodine k Edge and Contrast

  • 8/13/2019 Dr. Gunn CT Lecture

    42/75

    kVp: Iodine k Edge and Contrast

    Attenuation of x-ray by contrast is affectedby the mean energy (keV) of the photon.

    This is lower than the kVp of the beam

    With increasing kVp, photon energy increases andattenuation decreases.

    At lower kVp, there is greater attenuation due toiodine, as more photons are close to the k-edge ofI (33.2 keV)

    Studies have shown an increase in contrastenhancement of vessels (CNR) with decreasingkVp (140 120 100 80.)

    kV: Polychromatic X-ray beam

  • 8/13/2019 Dr. Gunn CT Lecture

    43/75

    kV: Polychromatic X ray beam

    140Photon energy (keV)

    kVp

    Photonnumber k-edge of I

    33.2

    Same Patient, Different kVp

  • 8/13/2019 Dr. Gunn CT Lecture

    44/75

    100 kVp120 kVp

    CTDIvol = 419 CTDIvol = 362

    , p

    kVp and Dose: Exponential

  • 8/13/2019 Dr. Gunn CT Lecture

    45/75

    p p

    80 100 120 140

    0

    20

    40

    60

    80

    100

    Relativ

    eCTDI(%)

    120 kVp 140 kVp = 1.4 x in CTDI

    120 kVp

    80 kVp = 2.2 x

    in CTDI

    Dual Energy CT

  • 8/13/2019 Dr. Gunn CT Lecture

    46/75

    gy

    Dual energy scanning (typically 80and 140kVp):

    Dual source (two tubes at differentkV)

    Single source with rapid kV switching.Sandwich Detector.

    Single helical acquisition. Can generate 80kVp, 140 kVp and

    virtual 120kVp, and non-enhanced ima es.

  • 8/13/2019 Dr. Gunn CT Lecture

    47/75

    Graser et al Eur Radiol. 2008 Aug 2 Epub

    8080 kVpkVp / 400/ 400 mAsmAs 140140 kVpkVp / 96/ 96 mAsmAs

    SimSim UnUn--enhenh

    SimSim 120120 kVpkVp

    IodineIodine Iodine +Iodine + UnenhUnenh

    Radiation Dose and DE CT

  • 8/13/2019 Dr. Gunn CT Lecture

    48/75

    No silver bullet

    Dose from single DE CT ~ multiplephase single energy (SE) CT1,2

    Single phase DECT acquisition is higher

    dose than single phase SECT.Need studies comparing image noise,

    number of phases, and diagnosticaccuracy.

    1.Chandarana et al, Radiology. 2008 Sep 23. Epub ahead of print.2.Chae EJ et al, Radiology. 2008 Sep 16. Epub ahead of print.

  • 8/13/2019 Dr. Gunn CT Lecture

    49/75

    Increased Noise Index /Reduced Effective mAs

  • 8/13/2019 Dr. Gunn CT Lecture

    50/75

    Reduced Effective mAs

    DLP 853

    mA 4392.5mm Recon

    DLP 325

    mA 2445mm Recon

    Stab wound to left flankNI = 15.4 NI = 22.0

    Reducing the mAs

  • 8/13/2019 Dr. Gunn CT Lecture

    51/75

    Radiology 2003; 229:575580

    140 kVp, 170mA, 136mAs 140 kVp, 100mA, 80mAs

    CT KUB for Renal Calculi, single and 4 channel CTscanners with fixed mA

    Are Lower Dose Techniques Accurate?

  • 8/13/2019 Dr. Gunn CT Lecture

    52/75

    AJR 2008; 191:396-401

    Dose of IVU = 2.6 mSvLow dose CT 0.7-2.1 mSv

    Routinely used CT Abd Pelv = 8-16 mSv

    Sensitivity = 0.966Specificity = 0.949

    Ultra-Low Dose CT Colonography

  • 8/13/2019 Dr. Gunn CT Lecture

    53/75

    3D Colonoscopy

    ptical Colonoscopy

    Surgical Spec

    140 kVp; and 10 mAsTotal radiation exp. (prone + supine)1.7 mSv (M) and 2.3 mSv (F).

    Optical colonoscopy:9 Ca2 polyps in 15 ptsRemaining 12 patients normal

    Ultra-low-dose CT:

    Detected all carcinomas10 / 12 polyps (sens 83.3%).Missed 2/6 < 5mm polyps.

    Eur Rad 2003 Jun;13(6):1297-302

    Noise and Windowing

  • 8/13/2019 Dr. Gunn CT Lecture

    54/75

    WW 3000 WL550 WW 340 WL60

    Bone Plus Algorithm

    Reconstruction Kernel

  • 8/13/2019 Dr. Gunn CT Lecture

    55/75

    Standard Bone Plus

    Slice Reconstruction Thickness

  • 8/13/2019 Dr. Gunn CT Lecture

    56/75

    2.5 mm 0.625 mmDouble Image Noise

  • 8/13/2019 Dr. Gunn CT Lecture

    57/75

    Reduce Phases.

    Reduce phase overlap.Reduce scan range.

    Center the patient.Reduce Follow-up Exams.

  • 8/13/2019 Dr. Gunn CT Lecture

    58/75

    Reduce Phases: Adrenal Washout

  • 8/13/2019 Dr. Gunn CT Lecture

    59/75

    AJR 2000;175:14111415

    OR DO MRI!!

    Reducing the Scan Range

  • 8/13/2019 Dr. Gunn CT Lecture

    60/75

    Segmented approachSegmented approachPanPan--Scan ApproachScan Approach

    Overlap regions:Overlap regions:

    Wasted radiationWasted radiation

    Positioning:Body / Profile Size and Symmetry

  • 8/13/2019 Dr. Gunn CT Lecture

    61/75

    Noise increases with increasing

    phantom diameter.Also increases in humans, but slightly

    differently, due to a number of factors

    (asymmetry, tissue type, intrinsiccontrast of fat.

    X-ray attenuation increases

    exponentially with body diameter

    Noise level doubles every 4-8 cm

    increase in effective body diameter.

  • 8/13/2019 Dr. Gunn CT Lecture

    62/75

    Arms at side

  • 8/13/2019 Dr. Gunn CT Lecture

    63/75

    Arms up

    Arms at side

    Standard approachStandard approachTotal Body ApproachTotal Body ApproachmA

    Patient Size

  • 8/13/2019 Dr. Gunn CT Lecture

    64/75

    Iterative Reconstruction

  • 8/13/2019 Dr. Gunn CT Lecture

    65/75

    Original way to reconstruct CT data.Replaced by Filtered Back Projection

    Latest statistical iterativereconstruction techniques produce:

    Less noisy images with significantly lowerradiation dose.

    Less beam hardening artifact.

    Currently limited by computer power.

    Iterative Reconstruction

  • 8/13/2019 Dr. Gunn CT Lecture

    66/75

    2.5 mmImages courtesy of GE Healthcare

  • 8/13/2019 Dr. Gunn CT Lecture

    67/75

    Quality Improvement

    How to Approximate Effective Dose

  • 8/13/2019 Dr. Gunn CT Lecture

    68/75

    eDLP FactorRegion

    0.019Pelvis

    0.015Abdomen

    0.017Chest

    0.0054Neck

    0.0023Head

    EUR 16262 EN-European Guidelines on Quality Criteria for Computed Tomography May 1999).

    = DLP x k = 0.017x 547.37

    = 9.3 mSv

    http://faculty.washington.edu/aalessio/doserisk/index.html

  • 8/13/2019 Dr. Gunn CT Lecture

    69/75

    Repeat CT for Renal Colic

  • 8/13/2019 Dr. Gunn CT Lecture

    70/75

    5,564 examinations performed on 4,562patients. 61% women (mean age, 45.5 y)

    38% men (mean age, 44.7 y) 3% (44) patients of pediatric age (

  • 8/13/2019 Dr. Gunn CT Lecture

    71/75

    * Does not include examinations performed at other sites

    AJR 2006; 186:1120-1124Other examinations have a proven efficacy

    Quality Control

  • 8/13/2019 Dr. Gunn CT Lecture

    72/75

    Collect Dose Data on All Scans

  • 8/13/2019 Dr. Gunn CT Lecture

    73/75

    Effective Dose (mSV) = 0.016 x DLP

    0.017 x 1710.95 = 29.08 mSv

    Head 0.0023, Neck 0.0054, Chest 0.017, Abdomen 0.015, Pelvis 0.019

    Other ways to reduce dose

  • 8/13/2019 Dr. Gunn CT Lecture

    74/75

    Not doing a CT!Ultrasound, MRI, x-ray, or no imaging.

    Using prediction rules to determinethe need for imaging.

    Wells criteria for CT PA for PE, NewOrleans criteria for minor head injury,

    Mann-Wilson C Spine CT rules.

  • 8/13/2019 Dr. Gunn CT Lecture

    75/75