chapter 27 - medical physics Flashcards

1
Q

X-ray properties

A
  • short wavelenght
  • EM waves
  • can be polarised and diffracted
  • high intensity can be harmful to living cells
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2
Q

production of X-rays in an X-ray tube

A
  • use can evacuated tube containing 2 electrodes
  • large pd between electrodes
  • cathode is a heater which produces electrons by thermionic emissions
  • electrons are accelerated towards the anode (target metal) eg tungsten - high mtp
  • X-rays produced when electrons decelerate by hitting anode
  • anode is shaped so rays are emitted in the desired direction
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3
Q

how to prevent X-ray tubes heating up too much

A
  • cooling fins help dissipate heat from the tube
  • water and oil cooling systems
  • target is rotated
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4
Q

shortest wavlentg of X-rays produced in an X-ray tube

A

eV = hf
eV = hc/λ
λ = hc/eV
so λ prop to 1/V
increasing current just increases intensity (as more electrons emitted)

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5
Q

X- ray spectra

A
  • range of decelerations of electrons inside the x-ray tube result in Bremsstrahlung (overall curve)
  • narrow intense lines (K-lines) are due to incident electrons removing electrons from the atom and these are filled by electrons dropping down energy levels and releasing photons of specific energies
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6
Q

how x-ray spectra is effected by increasing pd

A

intensity increases - graph shifts up and lowest wavelength shifts left (decreases)

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7
Q

attenuation

A

gradual decrease in intensity of the x-ray beam as it travels through a medium - bone attenuates more than soft tissue

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8
Q

energy range of x-rays used to diagnose bones

A

100eV - 100keV

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9
Q

4 attenuation mechanisms

A
  • simple scatter
  • photoelectric effect
  • compton scattering
  • pair production
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10
Q

simple scatter

A

1-20keV
- photon changes direction
- energy unchanged

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11
Q

photoelectric effect

A

<100keV
- X-ray photon absorbed
- electron emitted
- used in X-ray imaging

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12
Q

compton scattering

A

0.5-5MeV
- in high energy x-rays (radiotherapy) - used to kill cancerous cells
- elastic scattering of X-rays by orbital electron
- X-ray incident - low energy photon + electron released

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13
Q

pair production

A

1.02MeV
- X-ray photon -> electron-positron pair

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14
Q

attenuation coefficient

A
  • μ
  • interaction of x-ray photons with matter reduces intensity of the beam
  • transmitted intensity of x-rays depends on energy of photons + thickness/ type of substance
    I = I0 e^-μx
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15
Q

contrast medium

A
  • soft tissue have low absorption coefficients but adding a contrast medium allows visibility (larger absorption coefficient)
  • eg iodine and barium - have large atomic number which is related to absorption
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16
Q

CAT scan

A
  • patient lies on table that can slide in and out of large vertical ring
  • x-ray tube on one side and an array of detectors on the other
  • x-ray tube and detectors rotate
  • x-ray tube produces a then beam of x-rays which are attenuated by different amounts by different tissues
  • each time the tube rotates a 2D slice is formed - slices are turned into a 3D image by computer
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16
Q
A
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16
Q
A
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17
Q

+ CAT

A
  • 3D image
  • more detailed
  • can distinguish between soft tissues of similar attenuation coefficients
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17
Q
A
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18
Q
  • CAT
A
  • takes longer
  • patients receive a higher dose of ionising radiation vs an x-ray
  • have to lay still
18
Q

medical tracers used

A
  • need to target desired tissures
  • radioisotopes combined with elements to achieve this
19
gamma camera
- imaging tecnique to scan functions of organs - images radiation from a tracer in the patients body
20
gamma knife
- can be used to kill tumour cells - gamma emitted from multiple sources and concentrated to the target - try to minimise damage to healthy cells while providing a high enough does to kill tumour cells
21
gamma diagnosis + therapy
- diagnosis - gamma camera - therapy - gamma knife
22
chosing radioisotopes
imaging - isotopes have to be placed inside and detected outside - gamma used as least ionising and most penetrating - short half life- ensures patient doesnt remain radioactive for too long after and high enough activity from source so only small does required
23
gamma isotope used
Technetium - 99m Tc - 99m
24
gamma camera parts
- collimator - scintillator - photomultiplier - computer - outputs connected to a comp and use software to build image
25
collimator
lead tubes - only gamma photons that travel along axes of lead tubes are detected
26
scinillator
- gamma ray photon produces many vissible light photons
27
photomultiplier
- electrical pulse produced from each photon of visible light entering a photomultiplier tube - one visible light photon incident producing a photoelectron - electron accelerated to first electrode - high speed impact produces about 4 secondary electrons which are accelerated to the next higher V dynode - repeats and number of electrons grows exponentially
28
positron emission tomography (PET) scans
- like CAT scans, PET scans produces slices through the body to build a 3D image but uses gamma not x-rays - ring of gamma cameras around the patient
29
PET scan tracer
uses Fluorine-18 - positron emitter - short half life
30
PET scan steps
- pair of gamma photons produced from electron positron annihilation, emitted in opposite directions (obey conservation of momentum) - each photon detected at opposite detectors - arrival times recorded - as know speed can find location of annihilation based on arrival times - repeated until a 3D model can be produced - tracer density determined from rate of photons emitted in each region
31
PET +
- non invasive - diagnosis of cancer/ observes functionality of organs - used to assess effects of new medcines on organs
32
PET -
- expensive due to facilities required for on site tracer production - only found in main hospitals - only used for patients with complex problems
33
ultrasound
- longitudinal - >20kHz - non ionising - non invasive - high freqs mean wavelength is small and smaller details can be detected (2-15MHz)
34
piezoelectric effect
a piezoelectric material expands/ contracts when a pd is applied across opposite faces and vice versa
35
ultrasound transducer - emitting
- high freq alternating pd applied across the crystals - the crystal resonates producing an intense ultrasound signal
36
ultrasound transducer - detecting
- incident ultrasound makes crystal vibrate (compress and expand) - this generates an alternation emf across the ends of the crystal - detected by a ciruit
37
A scan
- simplest ultrasound scan - single transducer - used to determine thickness of bone / distance between lens and retina in eye
38
A scan - eye scan
- voltage pulse sent into the eye - reflections at each boundary between tissues - partly reflected and partly transmitted - the reflected pulse received by the transducer has less energy than original pulse - pulse voltage seen on a screen
39
B scan
- provide a 2D image - multiple A scans in different directions - transducer moved over skin - output connected to cop which produces a collection of dots on the screen - each dot corresponds to the boundary between tissues - brightness of dot prop to intensity of the reflected pulse
40
acoustic impedance
fraction of ultrasound intensity reflected at the boundary depends on acoustic impedance of both media Z = pc (density * speed of ultrasound in substance) prop of signal reflected Ir/I0 = (Z2-Z1)^2/(Z2+Z1)^2 more reflection when acoustic impedance is different - if the same not reflected
41
acoustic matching - coupling gel
- acoustic impedance of air is very different to body - air packets get trapped between transducer and body - gel stops air pockets and has a acoustic impedance similar to the body - means more ultrasound waves are transmitted and less reflected
42
doppler imaging
freq of ultrasound changes when it is reflected off a moving object - Doppler effect - can monitor flow of blood through vessel
43
colour doppler scans
- when ultrasound detected from moving blood cells - freq of detected pulse changes - moving towards - freq ^ - moving away - decreases - freq shift is prop to the speed of blood - comp can colour code image to show blood moving away/towards
44
speed of blood flow
Δf = 2fv cosθ/c