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RADIODIAGNOSTIC AND
RADIOTERAPHY
DEAPARTMENT OF
CT Training for Radiographers
Dr. Nursama Heru Apriantoro,
BASIC PHYSICS OF CT Scan
CT Training for Radiographers.
SECTION I
2
CT Training for Radiographers.
• Computerized Axial Tomography (CAT)
• Computer Aided Tomography (CAT)
• Computer Assisted Tomography (CAT)
• Computerized Transverse Axial
Tomography (CTAT)
• Computerized Transaxial Transmission
Reconstructive Tomography (CTT)
• Reconstructive Tomography (RT)
• Computerized Digital Tomography (CDT)
• Computerized Tomography (CT)
POPULAR NAME OF CT
3
CT Training for Radiographers.
8 NOVEMBER 1895 SINAR X DITEMUKAN
FISIKAWAN BERKEBANGSAAN JERMAN
WILHELM CONRAD RONTGEN
March 27, 1845
MERUPAKAN GEM DENGAN PANJANG
GELOMBANG BERKISAR 0,01 nm – 10 nm
(3 x 1016 Hz – 3 x 1019 Hz)
KARAKTERISTIK SINAR X
4
CT Training for Radiographers.
Memiliki daya tembus yang besar.
ƒDapat diserap oleh materi
(tergantung dari nomor atomnya)
ƒƒDapat dihamburkan (difraksi sinar-
x)
ƒMenimbulkan ionisasi.
Memiliki efek fotografi /
menimbulkan fluoresen.
KARAKTERISTIK SINAR X
5
CT Training for Radiographers.
RADIOGRAFI
KONVENSIONAL
.
PEMANFAATAN SINAR X
6
RADIOGRAFI
TOMOGRAPHY
CT Training for Radiographers.
 X-ray based
 Multiple Projections (each from different Angle)
 X-ray tube motions around the patient
 Detector motions around the patient opposite the tube
 In special technique :The patient's body is move
continuously as the x-ray beam is scanned around the
body
 Detector output and angular position fed into a
computer
 Computer perform calculation to estimate density of
tissues in each square of a slice
 Mathematically reconstruct image
 Create Voxel to Hounsfield Unit Value (CTNs)
 CTNs represent linear attenuation coefficient
CT SCAN
7
CT Training for Radiographers.
TAHUN 1971 GENERASI PERTAMA CT SCAN
DIPUBLIKASIKAN
Godfrey Newbold Hounsfield
28 August 1919 – 12 August 2004
Allan M. Cormack
23 Februari 1924 – 7 Mei 1998
CT SCAN
8
CT Training for Radiographers.
CT DEVELOPMENET
9
1970 1972
1976
1978
1990
CT Training for Radiographers.
ELECTRON BEAM OF CT
10
 Electron beam scanner
 Primarily for cardiologist, 50 msec scan times
 Tungsten target and high energy electron beam
https://www.youtube.com/watch?v=E9vLclEQRtc
CT Training for Radiographers.
CT DEVELOPMENT
11
HELICAL, 1990
Slip ring technology
Acquired data while table is
moving
Typical pitch ratio 0.5 - 2
on)(collimatithicknessslice
rotationpermovementtable
pitch 
MULTI DETECTOR, Late1990’s-
2000
Multiple detector array
Cone beam
MSCT
CT Training for Radiographers.
CT DEVELOPMENT
12
DUAL SOURCE, 2005
A Scanner using two x-ray source
and two detectors at the same time
Enables scanning a heart at any
heart rate and at the lowest radiation
dose possible
Dynamic Focal Spot,
Flying focal spot
Double ray density
Double spatial resolution
CT Training for Radiographers.
CT DEVELOPMENT
13
MULTI ENERGY DETECTOR
Consist of upper and bottom
detector
Upper detector to detects lower
energy
Bottom detector to detects higher
energy
Signal from both can be combine as
well
CT Training for Radiographers.
CT SCANNER DEVELOPMENT
14
CT Training for Radiographers.
SECTION II
15
CT Training for Radiographers.
Conventional Radiography Vs Tomography
16
a
t
ta
ba
SBm
)(
)(



)(
1
22
ba
a
Bmt



S
2t
CT Training for Radiographers. 17
BASICS PHYSICS of CT
CT Training for Radiographers. 18
BASICS PHYSICS of CT
CT Training for Radiographers. 19
CT Collimator
To decrease
scatter radiation
To reduce patien
dose
To Improve image
quaility
To determine slice
thickness
CT Training for Radiographers. 20
DETECTORS
• Scintillation Cristal + photodioda+ PMT
Sodium Iodide (Na I + Tl)
Calcium Fluoride (Ca F2)
cadmium tungstate (CdWO)
Bismuth germinate oxide (BGO)
Lutetium Terbium Aluminum Garnet (LuTAG)
Yttrium Gadolinium Oxide (YGO)
• Gas
Xenon Gas
Krypton
CT Training for Radiographers.
XENON GASES
21
CT Training for Radiographers.
SCINTILLATION DETECTOR
22
CT Training for Radiographers. 23
CT DETECTOR
 High efficiency; Kemampuan untuk
menyerap & mengubah foton x-ray
menjadi sinyal listrik
 Quick response time, waktu yang
dibutukan untuk menghasilkan data dari
setiap scanning
 High dynamic range, Kemampuan
untuk mendeteksi rasio berbagai
intensitas sinar x
 Stability, sinyal detektor dari waktu ke
waktu bersifat konsisten
CT Training for Radiographers.
CT Training for Radiographers.
It = Io exp (-μx)
Absorption and Attenuation
25
Io It
x







t
o
I
I
x
ln
1

μ1 μ2 μ3 μ4 μn
x x
Io
It

















t
o
i
i
t
o
n
xxxx
I
I
x
I
I
x
eIIeIIeIIeII
ln
1
ln
1
...
,,,
1
4321
4
34
3
23
2
12
1
01



CT Training for Radiographers.
BASIC CT RECON’S
26
1 2
3 4
4 6
4 6
5 11
9 10
8 14
16 17
13 16
19 22
3 6
9 12
1 2
3 4
X-RAY
CT Training for Radiographers. 27
Reconstruction process
0 0 0
0 0 1
0 1 0
0 1 1
1 0 0
1 0 1
1 1 0
1 1 1
Gray ScaleDIGITALANALOG
7 5 5
1 3 6
2 0 1
CT Training for Radiographers.
GRAY SCALE IMAGE
28
CT Training for Radiographers.
VOXEL, PIXEL, MATRIX SIZE
• Voxel (volume element) - for each image
slice, there is an x, y and z dimension.
These are coming close to isotropic (the
same in each dimension). A typical
voxel would be created from a 35 cm
FOV, 512 x 512 matrix and 0.6 -10.0
mm thick slice.
10 mm
.68 mm
.68 mm6 mm
.68 mm
.68 mm
CT Training for Radiographers.
VOXEL, PIXEL, MATRIX SIZE
Pixels
and
Voxels
CT Training for Radiographers.
VOXEL, PIXEL, MATRIX SIZE
31
VOXEL PIXEL
MATRIX SIZE, 16 x 16
PIXEL = SFOV / MATRIX SIZE
µ
(x,y,z)
p
(x,z)
CT Training for Radiographers.
CT NUMBER
32
• Hounsfield Units (HU), normalize to water.
 HU1000x
-)(
),('
water
water

 x,y
yxsCTN 
 HU1000x
-)(
),('
water
water

 x,y
yxsCTN 
• CTN Water = 0 HU (all energies)
• CTN range = -1024 to +3072
• 12 bit, 212
= 4096
CT Training for Radiographers.
CT NUMBER
Find the CTN of some tissues bellow :
• Bone = 0.528
• Blood = 0.208
• Gray Matter = 0.212
• White Matter = 0.213
• CSF = 0.207
• Water = 0.206
• Fat = 0.185
• Air = 0.0004
CT Training for Radiographers. 34
CT Training for Radiographers.
CT NUMBER
CT Training for Radiographers.
WL sama dan WW berbeda
CT Training for Radiographers.
WL beda dan WW sama
CT Training for Radiographers.
IMAGE FORMATION CT NUMBER
Some Preset Window and Levels
• Tissue Level Window
• Lung -550 HU 1600
• Soft Tissue 100 400
• Bone 800 1000
0
-1000 HU
Output gray levels
256
0 (black)
1000
0 HU
2000
1000 HU
CT Training for Radiographers.
CT RECONSTUCTIONS
39
Io It(y)
x
y
Io
It(d,Ө) x
y
d


dxyxyII
IdxyxyI
t
t
),())(/ln(
)),(exp()(
0
0


  dlldldtII )cossin,sincos()),(/ln( 10 
  dlldldfdg )cossin,sincos(),( 
F(x,y)
g(d,Ө)
Radon Transform
CT Training for Radiographers. 40
Fourier Transform
)()(
~
~
 

tetfF tj

The fourier transform changes SIGNAL from TIME
DOMAIN to FREQUENCY DOMAIN back again
F(ω) can be represented as :
Real + Imaginer
or
Magnitude + Phase
)()()()()(
~
~
~
~
 
 
dttjSintfdttCostfF 
CT Training for Radiographers. 41
Reconstruction process
intensityattenuated:)(intensity,incident:)(
[Np/m]ted)reconstrucbe(totcoefficienabsorption:),(
0 xIxI
yxf

















0
0
),(
0
),sincos(),(:projectionBack
),(ofFFT1Dis),(ewher
),(
2
1
),(:dataFiltered
)(
)(
ln),(),(:dataprojection
)()(:intensityattenuated
dyxpyxf
XpUP
dXeUUPXp
XI
XI
dYyxfXp
eXIXI
f
jUX
f
dYyxf
CT Training for Radiographers.
Back Projection
42
Backprojection at 4, 16, and 100 angles
-1
0
1
-1
0
1
-0.5
0
0.5
1
1.5
-1
0
1
-1
0
1
-0.5
0
0.5
1
1.5
-1
0
1
-1
0
1
-0.5
0
0.5
1
One, two, and four angles of backprojection
CT Training for Radiographers.
Attenuation Correction Factor
43
(a) Can be determined from attenuation coefficient measurements
determined from CT scan; (b) Array of attenuation correction
factors; (c) to provide final attenuation-corrected CT scan
CT Training for Radiographers.
Back Projection
44
Sample Back Projection Filtered Back Projection
FILTER
CT Training for Radiographers.
BASIC III
45
CT Training for Radiographers. 46
SSCT vs MSCT
CT Training for Radiographers. 47
SSCT MSCT
SSCT vs MSCT
CT Training for Radiographers.
SSCT vs MSCT
48
CT Training for Radiographers.
SSCT vs MSCT
49
SSCT COBRA
(Philips)
CT Training for Radiographers.
SSCT vs MSCT
50
COBRA
(Philips)
SSCT
CT Training for Radiographers.
SSCT vs MSCT
51
CT Training for Radiographers.
SSCT vs MSCT
52
PENUMBRA EFFECT
CT Training for Radiographers.
SSCT vs MSCT
53
CT Training for Radiographers. 54
SSCT vs MSCT
CT Training for Radiographers.
MSCT DETECTORS
55
CT Training for Radiographers.
DETECTOR CONFIGURATIONS
X-ray Tube Focal Spot
X-ray Beam Collimator
4 x 2.5 mm Detector Configuration
16-row Mosaic Detector
Diode FET Switching Array
Flex Connector A Flex Connector B
CT Training for Radiographers.
X-ray Tube Focal Spot
X-ray Beam Collimator
4 x 3.75 mm Detector Configuration
DETECTOR CONFIGURATIONS
16-row Mosaic Detector
Diode FET Switching Array
Flex Connector A Flex Connector B
CT Training for Radiographers.
DETECTOR CONFIGURATIONS
X-ray Tube Focal Spot
X-ray Beam Collimator
4 x 5.0 mm Detector Configuration
16-row Mosaic Detector
Diode FET Switching Array
Flex Connector A Flex Connector B
CT Training for Radiographers.
MSCT DETECTORS
CT Training for Radiographers.
Wide Area Coverage
60
Philips Brilliance 40Philips Brilliance 64
Over 525
40-mm
systems
installed
worldwide
as of
December
2005
Philips-Expertise in Detectors
Tomorrow- 256 Nano-panel
Working 256 Nano-panel detector array
CT Training for Radiographers.
MSCT DETECTOR CONFIGURATIONS
61
CT Training for Radiographers.
Flying Focal Spot
62
CT Training for Radiographers.
DFSTM
X-Ray Tube Design
63
Dynamic Focal Spot
X-ray Tube Design
Doubles
Ray Density and thus
Doubles
Spatial Resolution
with the same number
of detectors
CT Training for Radiographers.
PHILIPS : DFSTM
X-Ray Tube Design
64
WithWithout
CT Training for Radiographers.
PITCH
65
• Pitch = table travel per gantry
rotation (mm) / total nominal beam
width
• Pitch = table travel per gantry
rotation (mm) / (slice width ×
number of slices).
• Pitch = 0,13 -1,5, disarankan > 1
• mAs eff = mAs / pitch.
CT Training for Radiographers.
PITCH
66
• 16 Slice MSCT dengan 0,625 mm
slice thickness dan pergerakan
meja 15 mm per rotasi x ray tube.
• Tentukan Beam Pitch ?
pitch1.5
)625.0)(16(
15


mm
mm
BP
CT Training for Radiographers.
MSCT FASTER SCANNING
67
Detector Beam Thick
(mm)
# Rotation Total scan
time (sec)
1 x 1.25 1.25 160 128
4 x 1.25 5 40 32
8 x 1.25 10 20 16
16 x 1.25 20 10 8
64 x 0.625 40 5 4
1.25 mm images and 20 cm scan length at 0.8 sec
rotation and 1.0 pitch
CT Training for Radiographers.
Metode ABC/2 didasarkan pada penghitungan
volume ellipse, dengan menggunakan
persamaan :
V = 4/3 π r3 atau V= 4/3 x π x r1 x r2 x r3
Dengan penyederhanakan diameter d, , maka
diperoleh
V = ½ (d1 x d2 x d3)
Shg dapat ditulis menjadi
VOLUME IN CT SCAN
68
V = ABC / 2
CT Training for Radiographers.
The Total volume (V) was calculated by equation
• HU min adalah range HU minimum pada cairan
yang terdeteksi ROI
• HU max adalah range HU maksimum pada
cairan yang terdeteksi ROI
• from CAVA (Computer Assited Volumetric
Analysis)
VOLUME SUBJEK PADA CT SCAN
69
CT Training for Radiographers.
BASIC IV
70
Multiple-scan average dose
CT DOSIMETRY
CT Training for Radiographers.
CT DOSIMETRY
• MSAD = Multy Sice Average Dose
• CTDIw
• CTDIvol
• DLP
CTDI100
MSAD
Effective
Dose
CT Training for Radiographers.
CT DOSIMETRY
• CTDI menggunakan CTDI phantom dan
Ionization chambar
• CTDIw adalah CTDI weighted average
ditentukan berdasarkan :
CTDIw = (2*CTDIperiphery+CTDIcenter)/3
CTDIvol = CTDIw/Pitch
DLP = CTDIvol * L
L is the Z-length of the scan
CT Training for Radiographers.
DLP DAN DOSE EFEKTIF
DLP = CTDIvol * L
L is the Z-length of the scan
DOSE EFEKTIF = DLP * WT
WT adalah faktor bobot jaringan diperoleh
dari ICRP
CT Training for Radiographers.
CT DOSIMETRY
CT Training for Radiographers.
CTDIw: Dose for a “Procedure”
CT Training for Radiographers.
Present Calculation CT Dose
))((
2
LAT
2
AP
22
DiameterEffective
,
2
;
2
21
2
21
LATviewAPviewDEff
A
DEff
rrrALUASAN
ViewLAT
r
ViewAP
r




















CT Training for Radiographers.
)(DefffCTDISSDE vol 
SSDE (Size Specific Dose Estimate)
f (Deff) = Konversion factor pada diameter efektif
diperoleh dari AAPM Report 204
CT Training for Radiographers.
Doses From CT
BERT*Eff Dose (mSv)Exam
2.4 days0.02Chest x ray (PA film)
8.5 days0.07Skull x ray
158 days1.3Lumbar spine
304 days2.5I.V. urogram
1.0 year3Upper G.I. exam
2.3 years7Barium enema
243 days2CT head
3.3 years10CT abdomen
1.3 years3.9PET FDG Exam (10 mCi)
158 days1.3NM Bone Scan (20 mCi)
* Time to receive equivalent effective dose from
natural background radiation
CT Training for Radiographers.
Typical doses in mGy during CT in adults
(Shrimpton et al. 1991)
Exam Eyes Thyroid Breast Uterus Ovaries Testes
Head 50 1.9 0.03 * * *
Cervical
spine
0.62 44 0.09 * * *
Thoracic
spine
0.04 0.46 28 0.02 0.02 *
Chest 0.14 2.3 21 0.06 0.08 *
Abdomen * 0.05 0.72 8.0 8.0 0.7
L. spine * 0.01 0.13 2.4 2.7 0.06
Pelvis * * 0.03 26 23 1.7
The symbol * indicates that dose is < 0.005 mGy
CT Training for Radiographers. 80
Patient Dose Path
CT Training for Radiographers. 81
CT Training for Radiographers. 82
CT Training for Radiographers. 83
REFFERENCES
Edward M. Hsiao, Frank J. Rybicki, and Michael Steigner.
(2010) CT Coronary Angiography: 256-Slice and 320-
Detector Row Scanners. Curr Cardiol Rep. 12(1): 68–75.
Hameed T, Teague S, Vembar M, et al. Low radiation dose
ECG-gated chest CT angiography on a 256-slice
multidetector CT scanner. Int J Cardiovasc Imaging.
2009;25:267–278.
Kalendar, W.A. (2005) Computed Tomography.2nd Ed.
Mahesh, 2002. Physics Tutorial for Residents. Radiographics
22: 249-962
Nagel, H.D. (2004). MSCT Technology. Philips Medical
system Germany. www.multislice-ct.com
Philips. MSCT 256 Slices. PT BERCA NIAGA MEDIKA
Seeram, E. (2009). COMPUTED TOMOGRAPHY. Physical
Principles, Clinical Applications, and Quality Control. 3rd
Ed. St Louis: Saunders.
Walker M, Olszewski M, Desai M, et al. New radiation dose
saving technologies for 256-slice cardiac computed
tomography angiography. Int J Cardiovasc Imaging.
2009;25:189–199.
CT Training for Radiographers.
TERIMA KASIH
• ‫شكرا‬
• THANKS YOU
• ありがとう
• 감사합니다
• Спасибо
• Merci
• Danke
• igracias
• Matur nuwun
84

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PHYSICS of COMPUTED TOMOGRAPHY

  • 1. RADIODIAGNOSTIC AND RADIOTERAPHY DEAPARTMENT OF CT Training for Radiographers Dr. Nursama Heru Apriantoro, BASIC PHYSICS OF CT Scan
  • 2. CT Training for Radiographers. SECTION I 2
  • 3. CT Training for Radiographers. • Computerized Axial Tomography (CAT) • Computer Aided Tomography (CAT) • Computer Assisted Tomography (CAT) • Computerized Transverse Axial Tomography (CTAT) • Computerized Transaxial Transmission Reconstructive Tomography (CTT) • Reconstructive Tomography (RT) • Computerized Digital Tomography (CDT) • Computerized Tomography (CT) POPULAR NAME OF CT 3
  • 4. CT Training for Radiographers. 8 NOVEMBER 1895 SINAR X DITEMUKAN FISIKAWAN BERKEBANGSAAN JERMAN WILHELM CONRAD RONTGEN March 27, 1845 MERUPAKAN GEM DENGAN PANJANG GELOMBANG BERKISAR 0,01 nm – 10 nm (3 x 1016 Hz – 3 x 1019 Hz) KARAKTERISTIK SINAR X 4
  • 5. CT Training for Radiographers. Memiliki daya tembus yang besar. ƒDapat diserap oleh materi (tergantung dari nomor atomnya) ƒƒDapat dihamburkan (difraksi sinar- x) ƒMenimbulkan ionisasi. Memiliki efek fotografi / menimbulkan fluoresen. KARAKTERISTIK SINAR X 5
  • 6. CT Training for Radiographers. RADIOGRAFI KONVENSIONAL . PEMANFAATAN SINAR X 6 RADIOGRAFI TOMOGRAPHY
  • 7. CT Training for Radiographers.  X-ray based  Multiple Projections (each from different Angle)  X-ray tube motions around the patient  Detector motions around the patient opposite the tube  In special technique :The patient's body is move continuously as the x-ray beam is scanned around the body  Detector output and angular position fed into a computer  Computer perform calculation to estimate density of tissues in each square of a slice  Mathematically reconstruct image  Create Voxel to Hounsfield Unit Value (CTNs)  CTNs represent linear attenuation coefficient CT SCAN 7
  • 8. CT Training for Radiographers. TAHUN 1971 GENERASI PERTAMA CT SCAN DIPUBLIKASIKAN Godfrey Newbold Hounsfield 28 August 1919 – 12 August 2004 Allan M. Cormack 23 Februari 1924 – 7 Mei 1998 CT SCAN 8
  • 9. CT Training for Radiographers. CT DEVELOPMENET 9 1970 1972 1976 1978 1990
  • 10. CT Training for Radiographers. ELECTRON BEAM OF CT 10  Electron beam scanner  Primarily for cardiologist, 50 msec scan times  Tungsten target and high energy electron beam https://www.youtube.com/watch?v=E9vLclEQRtc
  • 11. CT Training for Radiographers. CT DEVELOPMENT 11 HELICAL, 1990 Slip ring technology Acquired data while table is moving Typical pitch ratio 0.5 - 2 on)(collimatithicknessslice rotationpermovementtable pitch  MULTI DETECTOR, Late1990’s- 2000 Multiple detector array Cone beam MSCT
  • 12. CT Training for Radiographers. CT DEVELOPMENT 12 DUAL SOURCE, 2005 A Scanner using two x-ray source and two detectors at the same time Enables scanning a heart at any heart rate and at the lowest radiation dose possible Dynamic Focal Spot, Flying focal spot Double ray density Double spatial resolution
  • 13. CT Training for Radiographers. CT DEVELOPMENT 13 MULTI ENERGY DETECTOR Consist of upper and bottom detector Upper detector to detects lower energy Bottom detector to detects higher energy Signal from both can be combine as well
  • 14. CT Training for Radiographers. CT SCANNER DEVELOPMENT 14
  • 15. CT Training for Radiographers. SECTION II 15
  • 16. CT Training for Radiographers. Conventional Radiography Vs Tomography 16 a t ta ba SBm )( )(    )( 1 22 ba a Bmt    S 2t
  • 17. CT Training for Radiographers. 17 BASICS PHYSICS of CT
  • 18. CT Training for Radiographers. 18 BASICS PHYSICS of CT
  • 19. CT Training for Radiographers. 19 CT Collimator To decrease scatter radiation To reduce patien dose To Improve image quaility To determine slice thickness
  • 20. CT Training for Radiographers. 20 DETECTORS • Scintillation Cristal + photodioda+ PMT Sodium Iodide (Na I + Tl) Calcium Fluoride (Ca F2) cadmium tungstate (CdWO) Bismuth germinate oxide (BGO) Lutetium Terbium Aluminum Garnet (LuTAG) Yttrium Gadolinium Oxide (YGO) • Gas Xenon Gas Krypton
  • 21. CT Training for Radiographers. XENON GASES 21
  • 22. CT Training for Radiographers. SCINTILLATION DETECTOR 22
  • 23. CT Training for Radiographers. 23 CT DETECTOR  High efficiency; Kemampuan untuk menyerap & mengubah foton x-ray menjadi sinyal listrik  Quick response time, waktu yang dibutukan untuk menghasilkan data dari setiap scanning  High dynamic range, Kemampuan untuk mendeteksi rasio berbagai intensitas sinar x  Stability, sinyal detektor dari waktu ke waktu bersifat konsisten
  • 24. CT Training for Radiographers.
  • 25. CT Training for Radiographers. It = Io exp (-μx) Absorption and Attenuation 25 Io It x        t o I I x ln 1  μ1 μ2 μ3 μ4 μn x x Io It                  t o i i t o n xxxx I I x I I x eIIeIIeIIeII ln 1 ln 1 ... ,,, 1 4321 4 34 3 23 2 12 1 01   
  • 26. CT Training for Radiographers. BASIC CT RECON’S 26 1 2 3 4 4 6 4 6 5 11 9 10 8 14 16 17 13 16 19 22 3 6 9 12 1 2 3 4 X-RAY
  • 27. CT Training for Radiographers. 27 Reconstruction process 0 0 0 0 0 1 0 1 0 0 1 1 1 0 0 1 0 1 1 1 0 1 1 1 Gray ScaleDIGITALANALOG 7 5 5 1 3 6 2 0 1
  • 28. CT Training for Radiographers. GRAY SCALE IMAGE 28
  • 29. CT Training for Radiographers. VOXEL, PIXEL, MATRIX SIZE • Voxel (volume element) - for each image slice, there is an x, y and z dimension. These are coming close to isotropic (the same in each dimension). A typical voxel would be created from a 35 cm FOV, 512 x 512 matrix and 0.6 -10.0 mm thick slice. 10 mm .68 mm .68 mm6 mm .68 mm .68 mm
  • 30. CT Training for Radiographers. VOXEL, PIXEL, MATRIX SIZE Pixels and Voxels
  • 31. CT Training for Radiographers. VOXEL, PIXEL, MATRIX SIZE 31 VOXEL PIXEL MATRIX SIZE, 16 x 16 PIXEL = SFOV / MATRIX SIZE µ (x,y,z) p (x,z)
  • 32. CT Training for Radiographers. CT NUMBER 32 • Hounsfield Units (HU), normalize to water.  HU1000x -)( ),(' water water   x,y yxsCTN   HU1000x -)( ),(' water water   x,y yxsCTN  • CTN Water = 0 HU (all energies) • CTN range = -1024 to +3072 • 12 bit, 212 = 4096
  • 33. CT Training for Radiographers. CT NUMBER Find the CTN of some tissues bellow : • Bone = 0.528 • Blood = 0.208 • Gray Matter = 0.212 • White Matter = 0.213 • CSF = 0.207 • Water = 0.206 • Fat = 0.185 • Air = 0.0004
  • 34. CT Training for Radiographers. 34
  • 35. CT Training for Radiographers. CT NUMBER
  • 36. CT Training for Radiographers. WL sama dan WW berbeda
  • 37. CT Training for Radiographers. WL beda dan WW sama
  • 38. CT Training for Radiographers. IMAGE FORMATION CT NUMBER Some Preset Window and Levels • Tissue Level Window • Lung -550 HU 1600 • Soft Tissue 100 400 • Bone 800 1000 0 -1000 HU Output gray levels 256 0 (black) 1000 0 HU 2000 1000 HU
  • 39. CT Training for Radiographers. CT RECONSTUCTIONS 39 Io It(y) x y Io It(d,Ө) x y d   dxyxyII IdxyxyI t t ),())(/ln( )),(exp()( 0 0     dlldldtII )cossin,sincos()),(/ln( 10    dlldldfdg )cossin,sincos(),(  F(x,y) g(d,Ө) Radon Transform
  • 40. CT Training for Radiographers. 40 Fourier Transform )()( ~ ~    tetfF tj  The fourier transform changes SIGNAL from TIME DOMAIN to FREQUENCY DOMAIN back again F(ω) can be represented as : Real + Imaginer or Magnitude + Phase )()()()()( ~ ~ ~ ~     dttjSintfdttCostfF 
  • 41. CT Training for Radiographers. 41 Reconstruction process intensityattenuated:)(intensity,incident:)( [Np/m]ted)reconstrucbe(totcoefficienabsorption:),( 0 xIxI yxf                  0 0 ),( 0 ),sincos(),(:projectionBack ),(ofFFT1Dis),(ewher ),( 2 1 ),(:dataFiltered )( )( ln),(),(:dataprojection )()(:intensityattenuated dyxpyxf XpUP dXeUUPXp XI XI dYyxfXp eXIXI f jUX f dYyxf
  • 42. CT Training for Radiographers. Back Projection 42 Backprojection at 4, 16, and 100 angles -1 0 1 -1 0 1 -0.5 0 0.5 1 1.5 -1 0 1 -1 0 1 -0.5 0 0.5 1 1.5 -1 0 1 -1 0 1 -0.5 0 0.5 1 One, two, and four angles of backprojection
  • 43. CT Training for Radiographers. Attenuation Correction Factor 43 (a) Can be determined from attenuation coefficient measurements determined from CT scan; (b) Array of attenuation correction factors; (c) to provide final attenuation-corrected CT scan
  • 44. CT Training for Radiographers. Back Projection 44 Sample Back Projection Filtered Back Projection FILTER
  • 45. CT Training for Radiographers. BASIC III 45
  • 46. CT Training for Radiographers. 46 SSCT vs MSCT
  • 47. CT Training for Radiographers. 47 SSCT MSCT SSCT vs MSCT
  • 48. CT Training for Radiographers. SSCT vs MSCT 48
  • 49. CT Training for Radiographers. SSCT vs MSCT 49 SSCT COBRA (Philips)
  • 50. CT Training for Radiographers. SSCT vs MSCT 50 COBRA (Philips) SSCT
  • 51. CT Training for Radiographers. SSCT vs MSCT 51
  • 52. CT Training for Radiographers. SSCT vs MSCT 52 PENUMBRA EFFECT
  • 53. CT Training for Radiographers. SSCT vs MSCT 53
  • 54. CT Training for Radiographers. 54 SSCT vs MSCT
  • 55. CT Training for Radiographers. MSCT DETECTORS 55
  • 56. CT Training for Radiographers. DETECTOR CONFIGURATIONS X-ray Tube Focal Spot X-ray Beam Collimator 4 x 2.5 mm Detector Configuration 16-row Mosaic Detector Diode FET Switching Array Flex Connector A Flex Connector B
  • 57. CT Training for Radiographers. X-ray Tube Focal Spot X-ray Beam Collimator 4 x 3.75 mm Detector Configuration DETECTOR CONFIGURATIONS 16-row Mosaic Detector Diode FET Switching Array Flex Connector A Flex Connector B
  • 58. CT Training for Radiographers. DETECTOR CONFIGURATIONS X-ray Tube Focal Spot X-ray Beam Collimator 4 x 5.0 mm Detector Configuration 16-row Mosaic Detector Diode FET Switching Array Flex Connector A Flex Connector B
  • 59. CT Training for Radiographers. MSCT DETECTORS
  • 60. CT Training for Radiographers. Wide Area Coverage 60 Philips Brilliance 40Philips Brilliance 64 Over 525 40-mm systems installed worldwide as of December 2005 Philips-Expertise in Detectors Tomorrow- 256 Nano-panel Working 256 Nano-panel detector array
  • 61. CT Training for Radiographers. MSCT DETECTOR CONFIGURATIONS 61
  • 62. CT Training for Radiographers. Flying Focal Spot 62
  • 63. CT Training for Radiographers. DFSTM X-Ray Tube Design 63 Dynamic Focal Spot X-ray Tube Design Doubles Ray Density and thus Doubles Spatial Resolution with the same number of detectors
  • 64. CT Training for Radiographers. PHILIPS : DFSTM X-Ray Tube Design 64 WithWithout
  • 65. CT Training for Radiographers. PITCH 65 • Pitch = table travel per gantry rotation (mm) / total nominal beam width • Pitch = table travel per gantry rotation (mm) / (slice width × number of slices). • Pitch = 0,13 -1,5, disarankan > 1 • mAs eff = mAs / pitch.
  • 66. CT Training for Radiographers. PITCH 66 • 16 Slice MSCT dengan 0,625 mm slice thickness dan pergerakan meja 15 mm per rotasi x ray tube. • Tentukan Beam Pitch ? pitch1.5 )625.0)(16( 15   mm mm BP
  • 67. CT Training for Radiographers. MSCT FASTER SCANNING 67 Detector Beam Thick (mm) # Rotation Total scan time (sec) 1 x 1.25 1.25 160 128 4 x 1.25 5 40 32 8 x 1.25 10 20 16 16 x 1.25 20 10 8 64 x 0.625 40 5 4 1.25 mm images and 20 cm scan length at 0.8 sec rotation and 1.0 pitch
  • 68. CT Training for Radiographers. Metode ABC/2 didasarkan pada penghitungan volume ellipse, dengan menggunakan persamaan : V = 4/3 π r3 atau V= 4/3 x π x r1 x r2 x r3 Dengan penyederhanakan diameter d, , maka diperoleh V = ½ (d1 x d2 x d3) Shg dapat ditulis menjadi VOLUME IN CT SCAN 68 V = ABC / 2
  • 69. CT Training for Radiographers. The Total volume (V) was calculated by equation • HU min adalah range HU minimum pada cairan yang terdeteksi ROI • HU max adalah range HU maksimum pada cairan yang terdeteksi ROI • from CAVA (Computer Assited Volumetric Analysis) VOLUME SUBJEK PADA CT SCAN 69
  • 70. CT Training for Radiographers. BASIC IV 70 Multiple-scan average dose CT DOSIMETRY
  • 71. CT Training for Radiographers. CT DOSIMETRY • MSAD = Multy Sice Average Dose • CTDIw • CTDIvol • DLP CTDI100 MSAD Effective Dose
  • 72. CT Training for Radiographers. CT DOSIMETRY • CTDI menggunakan CTDI phantom dan Ionization chambar • CTDIw adalah CTDI weighted average ditentukan berdasarkan : CTDIw = (2*CTDIperiphery+CTDIcenter)/3 CTDIvol = CTDIw/Pitch DLP = CTDIvol * L L is the Z-length of the scan
  • 73. CT Training for Radiographers. DLP DAN DOSE EFEKTIF DLP = CTDIvol * L L is the Z-length of the scan DOSE EFEKTIF = DLP * WT WT adalah faktor bobot jaringan diperoleh dari ICRP
  • 74. CT Training for Radiographers. CT DOSIMETRY
  • 75. CT Training for Radiographers. CTDIw: Dose for a “Procedure”
  • 76. CT Training for Radiographers. Present Calculation CT Dose ))(( 2 LAT 2 AP 22 DiameterEffective , 2 ; 2 21 2 21 LATviewAPviewDEff A DEff rrrALUASAN ViewLAT r ViewAP r                    
  • 77. CT Training for Radiographers. )(DefffCTDISSDE vol  SSDE (Size Specific Dose Estimate) f (Deff) = Konversion factor pada diameter efektif diperoleh dari AAPM Report 204
  • 78. CT Training for Radiographers. Doses From CT BERT*Eff Dose (mSv)Exam 2.4 days0.02Chest x ray (PA film) 8.5 days0.07Skull x ray 158 days1.3Lumbar spine 304 days2.5I.V. urogram 1.0 year3Upper G.I. exam 2.3 years7Barium enema 243 days2CT head 3.3 years10CT abdomen 1.3 years3.9PET FDG Exam (10 mCi) 158 days1.3NM Bone Scan (20 mCi) * Time to receive equivalent effective dose from natural background radiation
  • 79. CT Training for Radiographers. Typical doses in mGy during CT in adults (Shrimpton et al. 1991) Exam Eyes Thyroid Breast Uterus Ovaries Testes Head 50 1.9 0.03 * * * Cervical spine 0.62 44 0.09 * * * Thoracic spine 0.04 0.46 28 0.02 0.02 * Chest 0.14 2.3 21 0.06 0.08 * Abdomen * 0.05 0.72 8.0 8.0 0.7 L. spine * 0.01 0.13 2.4 2.7 0.06 Pelvis * * 0.03 26 23 1.7 The symbol * indicates that dose is < 0.005 mGy
  • 80. CT Training for Radiographers. 80 Patient Dose Path
  • 81. CT Training for Radiographers. 81
  • 82. CT Training for Radiographers. 82
  • 83. CT Training for Radiographers. 83 REFFERENCES Edward M. Hsiao, Frank J. Rybicki, and Michael Steigner. (2010) CT Coronary Angiography: 256-Slice and 320- Detector Row Scanners. Curr Cardiol Rep. 12(1): 68–75. Hameed T, Teague S, Vembar M, et al. Low radiation dose ECG-gated chest CT angiography on a 256-slice multidetector CT scanner. Int J Cardiovasc Imaging. 2009;25:267–278. Kalendar, W.A. (2005) Computed Tomography.2nd Ed. Mahesh, 2002. Physics Tutorial for Residents. Radiographics 22: 249-962 Nagel, H.D. (2004). MSCT Technology. Philips Medical system Germany. www.multislice-ct.com Philips. MSCT 256 Slices. PT BERCA NIAGA MEDIKA Seeram, E. (2009). COMPUTED TOMOGRAPHY. Physical Principles, Clinical Applications, and Quality Control. 3rd Ed. St Louis: Saunders. Walker M, Olszewski M, Desai M, et al. New radiation dose saving technologies for 256-slice cardiac computed tomography angiography. Int J Cardiovasc Imaging. 2009;25:189–199.
  • 84. CT Training for Radiographers. TERIMA KASIH • ‫شكرا‬ • THANKS YOU • ありがとう • 감사합니다 • Спасибо • Merci • Danke • igracias • Matur nuwun 84