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COMPUTED TOMOGRAPHY
INSTRUMENTATION AND
OPERATION
Nchanji NKEH Kenneth
kennchanji@yahoo.com/nkeh92@gmail.com
671459765/662695118
B.TECH/HPD, MDIRT
CHM Virtued Academy India (Ongoing)
Leader
Radiology Department
Level 300 MDI
2016/2017 Academic Year
ST. Louis UNIHEBS mile 3 Nkwen ,Bamenda- Cameroon
1
COMPUTED TOMOGRAPHY
INSTRUMENTATION AND OPERATION
2
3
4
5
6
7
8
9
10
11
12
13
14
15
OUTLINE
 CT SYSTEM COMPONENTS – DEFINITION OF A
SCANNER
 SCANNER COORDINATE SYSTEM – XYZ,
ISOCENTER
 IMAGING SYSTEM
 COMPUTER SYSTEM
 DISPLAY, RECORDING, AND STORAGE
SYSTEMS
16
CT MAIN SYSTEMS
 IMAGING SYSTEM
 COMPUTER SYSTEM
 DISPLAY, RECORDING, STORAGE SYSTEM
 DATA ACQUISITION SYSTEM
17
CT SYSTEM
GANTRY
DETECTORS
SAMPLE HOLD UNIT
ADC
ARRAY PROCESSOR
HOST
COMPUTER
STORAGE
CONSOLE
SCAN CONTROLLER
DAC
GANTRY CONTROL
HIGH VOLTAGE
GENERATOR
X-RAY TUBE
18
SCANNER 19
Some CT hardware 20
SCANNER
 GANTRY
 PATIENT COUCH
21
22
23
24
GANTRY HOUSES:
 X-RAY TUBE
 GENERATOR (LOW VOLTAGE DESIGN)
 COLLIMATORS
 DETECTORS
25
GANTRY
CHARACTERISTICS
 APERTURE
 TILTING RANGE
26
MOST OF THE SCANNERS HAVE
70CM APERTURE
27
70 CM
28
COORDINATE SYSTEM
X
29
COORDINATE SYSTEM
Y
30
COORDINATE SYSTEM
Z
31
ISOCENTER 32
TILTING RANGE OF MOST
SCANNERS- +30 TO -30
DEGREES
33
PATIENT COUCH :
450 LBS (204 KG) DISTRIBUTED
WEIGHT LIMIT
34
SCANNABLE RANGE:
COVERAGE FROM HEAD TO
THIGH (162CM)
35
MAX. SCANNABLE RANGE 36
IMAGING SYSTEM
 PRODUCTION OF X-RAYS
 SHAPING OF X-RAY BEAM ENERGY
 FILTERING X-RAY BEAM
37
IMAGING SYSTEM
COMPONENTS
 X-RAY TUBE
 GENERATOR –HIGH VOLTAGEHIGH VOLTAGE
 COLLIMATORS
 FILTER
 DETECTORS
 DETECTOR ELECTRONICS
38
X-RAY TUBE AND X-RAY
PRODUCTION
39
40
CATHODE --------
MADE OF TUNGSTEN
IN CT – STILL SMALL AND LARGE
41
THERMIONIC EMISSION
CATHODE HEATED UP TO AT LEAST 2,200 DEG. CELSIUS
TO LIBERATE ELECTRONS FOR TRANSIT TO ANODE
42
FOCAL SPOT- CT UTILIZES
DIFFERENT FOCAL SPOTS
 THE FILAMENT SIZE – LENGTH – FOCAL SPOTFOCAL SPOT
SMALLER FOCAL SPOT - Low mA
SMALLER FOCAL SPOT – sharper image
43
ANODE +++++ MADE OF
TUNGSTEN AND
MOLYBDENUM
TUNGSTEN
TARGET
TARGET MADE OF TUNGSTEN
AND
RHENIUM
44
mA – tube current
 The number of electrons flowing from cathode to
anode
45
kVp
 Potential difference between cathode and
anode (Volts) kilo means 1,000 x.
46
S –time of exposure
mAs tube current for certain
length of time
47
X-RAY PRODUCTION
RESULTS IN A LOT OF HEAT
AND VERY LITTLE
X-RAYS BEING GENERATED
HEAT UNITS CALCULATION
HU= kVp X mA x time
MOST CT TUBES HEAT CAPACITY
3-5 MILLION HU
48
REDUCTION OF HEAT UNITS –
TECHNIQUE
COMPENSATION kVp
 mA
 Time
INCREASED NOISE
49
TOO LOW OF kVp:
 NOISE !!!!NOISE !!!!
50
X-RAY EMISSION 51
TUBE CURRENT CHANGE
CURRENT
INTENSITY
ENERGY – NO CHANGE
2 * mA = 2 * number of photons
4 * mA = 4 * number of photons
52
Why changing
mA or time
 Avoiding motion – mA time
 Pediatric technique modification
 Reducing noise - mAs
NOISE
MOTION
53
Tube voltage (kVp)
CHANGE
kVp
INTENSITY -
ENERGY –
15% INCREASE OF KVP = 2 * mAs
54
kVp IN CT
 80-140
 TOO LOW – NOISE
(NOT ENOUGH PENETRATION OF THE PATIENT )
PHOTON STARVATION - NOISE!!!!!PHOTON STARVATION - NOISE!!!!!
55
HIGH VOLTAGE
GENERATOR –(HVG)
 GENERATES HIGH VOLTAGE POTENTIAL BETWEEN
CATHODE AND ANODE OF AN X-RAY TUBE
56
CT GENERATOR
 5-50 kHz
 30-60 kW
KVP SELECTION:
80, 100, 120, 130,140
mA selection:
30, 50, 65, 100, 125, 150, 175, 200, 400
57
COLLIMATION IN CT
ADC
PRE-PATIENT COLLIMATION
POST-PATIENT COLLIMATION
58
BASIC DATA AQUSITION SCHEME IN CT
ADC
FILTRATION
59
FILTRATION CHANGE
FILTRATION
INTENSITY
ENERGY –
60
FILTRATION MATERIAL
 ALUMINIUM ( SPECIAL FILTER IN CT)
BOWTIE
TO MAKE THE BEAM HARDER AND
MORE MONOENERGETIC
61
Filter
Patient
DEFINES SLICE
THICKNESS
REDUCES SCATTER
RECHING THE PATIENT
Detector
62
CT DETECTORS 63
CONCEPT OF MDCT 64
SDTCT AND MDCT 65
DETECTOR TYPES: SCINTILLATION
PM TUBE
S. CRYSTAL
S. CRYSTAL
PHOTODIODE
66
SCINTILLATION CRYSTALS
USED WITH PM TUBES:
 SODIUM IODIDE –AFTERGLOW + LOW DYNAMICAFTERGLOW + LOW DYNAMIC
RANGERANGE ( USED IN THE PAST)( USED IN THE PAST)
 CALCIUM FLUORIDE
 BISMUTH GERMANATE
67
S. CRYSTAL USED WITH
PHOTODIODE
 CALCIUM TUNGSTATE
 RARE EARTH OXIDES - CERAMIC
68
DETECTOR TYPE: GAS IONIZATION
XENON GAS
30 ATM
69
EFFICIENCY OF
DETECTORS- QDE
 SCINTILLATION – 95% - 100%- COMMONLY USED INCOMMONLY USED IN
III & IV GENERATION SCANNERSIII & IV GENERATION SCANNERS
 GAS – 50% - 60%
70
COMPUTER SYSTEM
 RECONSTRUCTION AND POSTPROCESSING
 CONTROL OF ALL SCANNER COMPONENTS
 CONTROL OF DATA ACQUSITION, PROCESSING,
DISPLAY.
 DATA FLOW DIRECTION
71
COMPUTER SYSTEM IN CT
 MINICOMPUTERS
72
COMPUTER SYSTEM
COMPOSED OF:
 HARDWARE
 SOFTWARE
73
COMPUTER PROCESSING
IN CT
 SEQUENTIAL PROCESSING
 MULTITASKING
 MULTIPROCESSING
74
SOFTWARE –PROGRAM (S)
HELPING CT USER TO
COMMUNICATE WITH THE CT
SYSTEM
75
CT OPERATING SYSTEM-
PROGRAMS THAT CONTROL
THE HARDWARE COMPONENTS
AND THE OVERALL OPERATION
OF THE CT COMPUTER
76
CT OPERATING SYSTEM
 UNIX
 WINDOWS
77
HOST COMPUTER
 CONTROL OF ALL COMPONENTS
 CONTROL OF DATA ACQUSITION, PROCESSING,
DISPLAY.
 DATA FLOW DIRECTION
78
ARRAY PROCESSOR
 TAKES DETECTOR MEASUREMENTS FROM HUNDREDS OF
PROJECTIONS. RESPONSIBLE FOR RETROSPECTIVE
RECONSTRUCTION AND POSTPROCESSING OF DATA.
THE MORE PROCESSORS IN THE COMPUTER
THE SHORTER THE RECONSTRUCTION TIME
79
DATA ACQUISITION
SYSTEM (DAS)
 SET OF ELECTRONICS BETWEEN DETECTORS AND
HOST COMPUTER.
 IT CONTAINS: AMPLIFIER, ADC, DAC, GENERATOR,
S/H.
80
AMPLIFIER
 SIGNAL FROM DETECTORS GOES TO AMPLIFIERS
FOR SIGNAL MAGNIFICATION AND THEN IS SENT
TO SAMPLE/HOLD UNIT
81
ADC
 CONVERTS ANALOG SIGNAL OUTPUT FROM THE
SCANNING EQUIPMENT TO A DIGITAL SIGNAL SO IT
CAN BE PROCESSED BY A COMPUTER.
82
SAMPLE/HOLD UNIT (S/H)
 LOCATED BETWEEN AMPLIFIERAMPLIFIER AND ADCADC PERFORMS SAMPLING
AND ASSIGNS SHADES OF GRAY TO THE PIXELS IN THE DIGITAL
MATRIX CORRESPONDING TO THE STRUCTURES
83
DAS
GANTRY
DETECTORS
S/H
ADC
ARRAY PROCESSOR
HOST
COMPUTER
STORAGE
CONSOLE
SCAN CONTROLLER
DAC
GANTRY CONTROL
HIGH VOLTAGE
GENERATOR
X-RAY TUBE
84
IMAGE DISPLAY,
RECORDING, STORAGE
 DISPLAYS IMAGE ( OUTPUT FROM COMPUTER)
 PROVIDES HARD COPY OF THE IMAGE
 FACILITATES THE STORAGE AND RETRIEVAL OF
DIGITAL DATA
 COMMUNICATES IMAGES IN THE NETWORK
85
IMAGE
DISPLAY
86
IMAGE RECORDING SYSTEMS
(LASER PRINTERS)
 SOLID STATE LASER
PRINTERS
 GAS LASER PRINTERS
87
HARD COPY 88
IMAGE STORAGE MEDIA
 MAGNETIC TAPES
 MAGNETO-OPTICAL DISK (MOD)
 CD
89
COMMUNICATION
 PACS
90
NETWORK
WHILE MOST TELERADIOLOGY SYSTEMS
PURCHASED OVER THE LAST DECADE WERE
INTENDED FOR ON-CALL PURPOSES, THE PAST
TWO YEARS HAVE SEEN A RAPID INCREASE IN
THE USE OF TELERADIOLOGY TO LINK
HOSPITALS AND AFFILIATED SATELLITE
FACILITIES, OTHER PRIMARY HOSPITALS, AND
IMAGING CENTERS. A NUMBER OF THE
ENABLING TECHNOLOGIES NEEDED FOR
EFFECTIVE OVERREAD NETWORKS, SUCH AS
MORE AFFORDABLE HIGH-SPEED
TELECOMMUNICATIONS NETWORKS AND
IMPROVED DATA COMPRESSION TECHNIQUES,
HAVE MATURED IN RECENT YEARS.
91
NightHawk Radiology Services has developed
an innovative approach to the delivery of
radiology services by operating centralized,
state-of-the-art reading centers in Sydney,
Australia and Zurich, Switzerland. Staffing
U.S.-trained, board-certified radiologists
specializing in emergency radiology, these
locations are ideally situated for U.S. care
because when it’s the middle of the night in
Boston, it’s daytime “Down Under.” When it’s
early morning in Los Angeles, it’s daytime in
the Alps. From the centralized reading centers,
NightHawk radiologists interpret exams and
report the results to attending physicians in
real-time, usually less than 20 minutes.
92
CT ROOM LAYOUT 93
How much does a CT
scanner cost?
94
How much ??
4-slice scanner: $85,000 - $115,000
16-slice scanner: $145,000 - $225,000
64-slice scanner: $250,000 - $450,000
Service contracts: $100,000 - $135,000
95
96
97
Lecture delivered with use of
resources from ICRP, IAEA,
AAPM and GE
98
NEXT LECTURE:
1. ULTRASONOGRAPHIC INSTRUMENTATION
2. MAMMORAPHIC INSTRUMENTATION
3. FLUOROSCOPIC INSTRUMENTATION
4. MRI INSTRUMENTATION
99
100
101
102

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