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(1)

Remote sensing

(Health Physics)

Cambridge IA2 Physics

(2)

Syllabus Section VII.29

X-Rays

(a)

explain in simple terms the need for remote sensing

(non-invasive techniques of diagnosis) in medicine.

(b)

explain the principles of the production of X-rays by

electron bombardment of a metal target.

(c) describe the main features of a modern X-ray tube, including

control of the intensity and hardness of the X-ray beam.

(d)

show an understanding of the use of X-rays in imaging

internal body structures, including a simple analysis of the

causes of sharpness and contrast in X-ray imaging.

(e)

recall and solve problems by using the equation I =

I

0

e

-μx

for the attenuation of X-rays in matter.

(3)

X-Rays

• Production

• Spectrum

• Attenuation

• Imaging

(4)

The Electromagnetic Spectrum

electromagneticspectrum.swf

(5)
(6)
(7)

X-Ray Production

• Heater cathode

Thermionic emission

• Accelerating p.d.

• Anode target (often Tungsten, W)

High m.pt,

water cooled to remove heat

• X-rays are produced as electrons are

(8)
(9)

X-Ray

Spectrum

Background

spectrum

Characteristic

lines

Threshold

(10)

X-Ray Spectrum

(11)

X-Ray Spectrum

Background

• Bremsstrahlung (‘braking’) radiation

emitted by electrons as they slow down and

rapidly lose energy inside the target

Characteristic lines

(12)

Characteristic X-Rays

http://hyperphysics.phy-astr.gsu.edu/hbase/quantum/xrayc.html

Characteristic lines

produced by electron

transitions of fixed

energy within the

target atoms.

(13)

X-Ray Spectrum

Electron KE

X-ray photon energy:

E

k

= eV = h

max

= hc/

min

Threshold wavelength,

(14)

Threshold Wavelength

= hc/eV

=

(6.6 x 10

-34

x 3 x 10

8

)

/(1.6 x 10

-19

x 3.5 x 10

4

)

= 3.5 x 10

-11

m

(15)

X-Ray Spectrum

Intensity

• Intensity

tube current (heater current)

Hardness

• Hardness = penetration of the X-rays

electron energy

accelerating voltage

(16)
(17)

X-Rays – Attenuation

I = I

0

e

-

x

I

0

= incident intensity

(Wm

-2

)

= linear attenuation coefficient

(m

-1

)

x = thickness of medium

(m)

Incident Intensity, I

0

Transmitted intensity, I

(18)

X-Rays – Attenuation

Worked Example (Page 37 – Health Physics)

For 1MeV radiation incident on tissue, the linear

attenuation coefficient is 7m

-1

. Calculate the

thickness of tissue required to reduce the intensity

of the beam by half.

0.5 = e

-

x

x = ln0.5

x = ln2 / 7

(19)

XRayInteract.swf

(20)
(21)

X-Ray Imaging

Sharpness

• Size of anode

• Size of aperture

• Removal of scattered X-rays by Pb collimator grid

Contrast

• Densities of tissue/bone

(22)

X-Ray Imaging - Sharpness

Depends on area of target anode

(23)

X-Ray Imaging - Sharpness

Pb collimator grid removes scattered X-rays

Film or

detector

Unexposed

area

(24)
(25)

1. Object Contrast

Dependent on the object under study:

Density

• Atomic number

• Thickness

(26)

Barium meal

(27)
(28)

Barium meal (contrast agent)

Investigating swallowing

(29)

2. Subject Contrast

Dependent on:

Object contrast

and on

• The

energy characteristics of the beam

(30)

3. Display Contrast

Dependent upon

• The detection devices

• The display devices

(31)

Image Resolution

Image resolution is affected

by

• The design of the X-ray

tube

• The design of the detector

• The nature of the display

(32)
(33)

X-Rays – Questions

(34)

Let’s look at

how X-rays

are used in

Computerise

d Axial

Tomography

(35)

Syllabus Section VII.29

CT (Computed Tomography) Scanning

(f) Show an understanding of the purpose of

computed tomography or CT scanning.

(g) Show an understanding of the principles of CT

scanning.

(h) Show an understanding of how the image of an

8-voxel cube can be developed using CT

scanning.

(i) – (k) Ultrasound

(36)

www.impactscan.org/rsna99.htm

www.chadwickmedical.com/svc_ctangio.htm

(37)
(38)
(39)
(40)

3D Image divided into

voxels

(

Pixel

= 2D)

(41)

CAT Imaging

• 3D X-ray scanning of the whole body or

region of a body

(42)

P. Lovatt & Hari.R 42/122

This image was

produced with a

window of

1000HU at level

–700HU

(HU<+300)

CAT Imaging

http://cal.man.ac.uk/student_projects/2000/mmmr7gjw/technique9.htm

(43)

CAT Imaging

This image was

produced with a

window of

500HU at level

+50HU.

(–450<HU<+550)

(44)

Computerised Tomography

(45)

CAT Imaging

Rotating the

scanner provides

more information

about the

(46)

Physics 2000 website (Colorado)

Physics 2000\tomography\auto_rib_cage.html

(47)
(48)
(49)

Image Planes

Image planes

A Axial

(50)

Creating a CAT Image

4 1

2 7

? ?

? ?

Imagine just 4 voxels of tissue (small 3D cubes) to be

imaged using a rotating CAT scanner

X-ray

production

Tissue to

(51)

First Image 0

0

4 1

2 7

Image

Angle 0

0

+5

+9

(52)

4 1

2 7

Angle 45

0

Second Image 45

0

(53)

Third Image

90

0

4 1

2 7

Angle 90

0

+6 +8

22 14

16 6

11 20

(54)

4 1

2 7

Angle 135

0

Fourth Image 135

0

(55)

Image Processing

1. Subtract ‘background’ (4 + 1 + 2 + 7 = 14)

2. Divide by 3 to remove duplication

Scan

Result

26 17

20 35

12 3

6 21

Final

Image

4 1

2 7

– 14

3

(56)

Consider

one voxel

1. Subtract the

unwanted

contribution to

each voxel

(background)

4

Scan 1

4 4

0 0

8 4

0 4

Sca

n 2

Sc

an

4

Sc

an

3

12 4

4 4

16 4

4 4

12 0

0 0

Image

4 0

0 0

– 4

3

2. Divide by 3 to

remove the

(57)

3D Imaging

• Based on the 8-voxel cube in 3D

• Many scans at different angles

• Linear and angular motion

• Millions of computations per voxel

• Intensity and contrast can be varied

(58)

P. Lovatt & Hari.R 58/122

Clockwise from top-left: Volume rendering overview, axial slices, coronal slices, sagittal slices.

Although visually very appealing, the volume rendering is often of limited diagnostic value, and requires substantial computer resources. Qualitative and quantitative information tends to be more accessible on the cross-sectional images, and many operators prefer to forgo the volume rendering for

www.answers.com/topic/ct-workstation-neck-jpg

(59)
(60)

CAT Images

(61)

Stroke diagnosis (brain)

Abdomen

(62)

CAT Images

(63)

CAT

Images

Sliced CAT

sections

(axial) can be

combined to

produce 3D

or moving

images

(64)

P. Lovatt & Hari.R 64/122

CAT Mummies

Another mummy:touregypt.net/featurestories/mummification.htm

(65)

CAT Advantages

Can image calcium

More useful than MRI for investigating cortical bone

fractures and calcification of organs.

Rapid imaging

Modern machines can produce images in a matter of a few

seconds, depending on the type of scan.

Good for obese patients

Fat separates the abdominal organs and good CT images can be generated. Ultrasound is difficult in obese patients.

Good contrast between

different tissues

Good contrast is seen between tissues which are mainly bone, fat, water, and air. Use of a narrow X-ray beam and windowing can produce detailed images. However CT cannot differentiate well between different parts of the same organ.

Cancer Treatment

CT is particularly useful for staging and treating tumours.

Three-dimensional Imaging

(66)

CAT Disadvantages

High ionizing dose

A thoracic CT scan may expose the patient to as much

radiation as 40 chest X-rays.

Bony artefacts

Brain scans may be distorted by bony artefacts

Imaging in the transverse (axial)

plane only

Sagittal

and

coronal

images are generally difficult,

although possible if the patient can be positioned

appropriately within the scanner.

High cost of equipment and

procedure

CT scanners are fairly expensive to purchase and the

number of personnel involved means that each scan is

considerably more expensive than an X-ray.

(67)

CAT - Questions

SAQ 5.2 (Page 49,

Health Physics

)

(68)

Syllabus Section VII.29

Ultrasound

(i) explain the principles of the generation and detection of

ultrasonic waves using piezo-electric transducers.

(j)

explain the main principles behind the use of

ultrasound to obtain diagnosticinformation about

internal structures.

(k)

show an understanding of the meaning of

acoustic impedance and its importance to the intensity

reflection coefficient at a boundary.

(69)
(70)

Ultrasound is used for the

diagnosis (finding) and treatment

(destruction) of kidney stones

(71)

Ultrasound Imaging

• Ultrasound >20kHz

Ultrasound transducer

generates sound

pulses using the

piezo-electric

effect

• Pulses are

reflected

where they meet a

boundary between regions of different

density

(72)

Piezo-electric Effect

www.physikinstrumente.com/tutorial/4_15.html

(73)
(74)

Piezo-electric Effect

piezocompressMS.avi

Change in the dimensions of a

crystal when a p.d. is applied

(75)

Piezo-electric ‘Poling’

An electric field of 2000Vmm

-1

is applied to a

heated crystal (above the Curie temperature)

(76)

Piezo-electric Effect

(77)

Ultrasound

- transducer

Frequency range <600MHz

Earthed case

Co-axial cable

Piezo-electric crystal

Plastic

cover

Silver electrodes

Backing material

Input/output

p.d.

Pulse of high frequency p.d.

Ultrasound pulse

Reflected pulse

(78)

Acoustic Impedance

• Intensity of a reflected pulse depends on

differences in density

across a boundary

• Acoustic impedance,

Z =

c

where:

= density

(kgm

-3

)

(79)

Acoustic Impedance

Intensity of the reflected pulse:

I

R

= I

0

(Z

2

– Z

1

)

2

(Z

2

+ Z

1

)

2

Medium 1 (

1

, Z

1

) Medium 2

(

2

, Z

2

)

I

0

I

T

Transmission

(80)

Acoustic Impedance

Medium

Z =

c / kgm

-2

s

-1

Air

430

Quartz

1.52 x 10

7

Water

1.50 x 10

6

Blood

1.59 x 10

6

Fat

1.38 x 10

6

Muscle

1.70 x 10

6

Soft tissue

1.63 x 10

6

Bone

5.6 – 7.8 x 10

6

See also

Table 7.1

(page 58,

(81)

Questions

SAQ 7.1 (Health Physics, Page 59)

Calculate the ratio of sound

reflected

at the boundary

between muscle and soft tissue, using the data from

table 7.1 (page 58).

Extension

Calculate the ratios across

(i) an air-tissue boundary

(ii) a bone-tissue boundary

Ratio = 0.000921

(Virtually ALL the energy is transmitted)

(82)

Coupling Gel

Air-tissue boundaries reflect

most of the ultrasound energy

A

coupling gel

is applied

(83)

Absorption Of Ultrasound

I = I

0

e

-kx

I

0

= incident intensity

(Wm

-2

)

k = absorption coefficient

(m

-1

)

x = thickness of medium

(m)

Incident Intensity, I

0

Transmitted intensity, I

(84)

Absorption Co-efficient

Medium

k at 1MHz / m

-1

Air

120

Water

0.02

Muscle

23

Bone

130

(85)

Transmission pulse

Ultrasound A-scan

• Similar to early RADAR

systems (radio waves)

Timebase

(calibrated to give distance)

Skull echoes

Mid-line echo

from median

fissure at centre

of brain

Scalp-air echo

Skull-tissue echo

Inner skull echo

(86)

Ultrasound

A-scan

(87)

Ultrasound B-scan

(88)

P. Lovatt & Hari.R 88/122

(89)
(90)
(91)
(92)

Doppler Ultrasound

Doppler image of umbilical cord artery & vein

www.centrus.com.br/.../chapter_01.htm

(93)
(94)

Doppler Ultrasound

Measuring blood flow

(95)

Ultrasound in use

• Essentially

Safe

– to

patient and operator

• Portable & low power

• Can obtain

images in 3D

and in

real-time

• Can analyse blood flow using

doppler effect

(96)

Ultrasound Therapy

(97)

Ultrasound Questions

Health Physics textbook

SAQ 7.2 (Page 61)

(ultrasound v X-rays)

SAQ 7.3

(Doppler effect)

Questions (Page 62)

(98)
(99)

RADAR

Imaging

Similar

(100)

SONAR

Imaging

http://surveying.wb.psu.edu/psu-surv/

SURIs/hydrographic_surveying.htm

(101)

Syllabus Section VII.29

Magnetic Resonance Imaging (MRI)

(l) explain the main principles behind the use of magnetic resonance

to obtain diagnostic information about internal structures.

(m)

show an understanding of the function of the non-uniform

magnetic field, superimposed on the large constant magnetic

field, in diagnosis using magnetic resonance.

Note:

The technology is called

Nuclear Magnetic Resonance

imaging (NMR)

. However, because of the negative associations

with the word

nuclear

, hospitals prefer to use the term

MRI

(102)
(103)
(104)

MRI

A brain scan showing a tumour

A hospital MRI scanner

(105)

MRI Scanner

• Powerful magnet 0.5-3.0T (60T in research)

• Non-linear (gradient) field

• RF generator coil

• RF received

(106)

MRI Theory

• The human body is 60% hydrogen

• Hydrogen (single proton) has a high

(107)

MRI Theory

All of the hydrogen protons

will align with a strong

magnetic field in one direction

or the other.

The vast majority cancel each

other out, but in any sample

there is not complete

(108)

No applied B-field

(random, no net

alignment)

With applied

magnetic field

(small net dipole)

(109)

MRI Theory

• An Radio Frequency (

RF

) pulse is

generated using a coil

• It causes the uncancelled aligned

proton spin axes

to

precess

around

the

field axis

at certain frequencies

• When the pulse turns off, the

protons ‘

decay

back to their

original state, releasing RF energy

• The returning RF energy is detected

(110)
(111)

Protons have random spin orientation

Protons align with the field

(112)

MRI Theory

Gradient magnets

vary the field (and

the return RF

frequencies detected)

allowing emissions

(113)

MRI Safety

• Non-invasive

• Safe, except for patients with

metal objects inside their bodies

e.g. pacemakers, metal implants, shrapnel, bullets,

surgical staples etc

(114)
(115)

Functional

MRI

(fMRI)

(116)
(117)
(118)

MRI Advantages

Non-ionizing radiation

Because MRI does not ionize tissue it is considered amongst the safest of radiological techniques. There are no known physiological side effects of being exposed to a magnetic field.

High soft-tissue contrast

MRI images provide very detailed information about soft tissues. They can differentiate between normal and abnormal tissues and may show damage missed on CT

Images can be produced in any plane This is of great value in studies of the Central Nervous System.

Visualisation of areas deep within bony structures

MRI is thus invaluable for the diagnosis and treatment of brainstem tumours.

Shows vasculature (veins and

arteries) without contrast media

Because the patient is not subject to any invasive procedure (i.e. the injection of contrast media) the technique is less unpleasant.

Good for angiography

MRI is excellent for imaging blood flow and studying heart

function. Functional MRI maps changes in blood flow in the brain during specific tasks. This provides valuable information about how the brain works.

(119)
(120)

MRI Disadvantages

High cost of equipment An MRI scanner can cost over GB£1,500,000 (US$ 3,000,000) to purchase.

Claustrophobia Up to 10% of patients experience claustrophobia during an MRI scan and 1% of scans have to be aborted because of it.

Long imaging time

A complete image may take up to 30mins and movement at the wrong time can cause artefacts in the image. New techniques have reduced imaging time.

Strong magnetic field

MRI imaging is unsuitable for many patients with metal implants (e.g. artificial joints) and is especially dangerous for patients with pacemakers, neural

stimulators, or cochleal implants. Loose metal objects must be removed before coming near to the scanner otherwise they may be attracted so strongly by the magnet that they fly through the air towards the patient like tiny missiles!

Unable to image calcium Because MRI detects water rather than molecular density, calcium is not well visualized. This means that tissue calcification, a feature of a number of disease processes, can not be detected. Bone is also less obvious than on a CT scan.

Acoustic noise

Switching on and off of the gradient coils causes repeated loud bangs. Noise levels may reach 95 dB for much of the scan. Ear plugs are advisable to reduce the risk of temporary or even permanent hearing loss.

Various minor biological effects

(121)

Time for

Lunch!

(122)

MRI Questions

Health Physics textbook

SAQ 8.1 (Page 65)

(Basic principles)

Question (Page 67)

(123)

Visible

Human

Project

www.dhpc.adelaide.edu.au

/projects/vishuman2/

www.magnet.fsu.edu/

education/tutorials/

(124)

MRI Game

References

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