Week1 Flashcards

1
Q

What is the only harmful radiation?

A

ionizing radiation

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2
Q

Classification of radiation (3):

A
  1. Electromagnetic radiation
  2. Particulate radiation
  3. Ionising and non-ionising radiation
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3
Q

Characteristics of electromagnetic waves (4):

A
  1. amplitude (trough/crest from straight line)
  2. wavelength (b/w 2 crests/troughs) λ
  3. frequency f
  4. speed v
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4
Q

For X-rays, λ and f are expressed:

A

λ - nm
f - Hz (1 Hz = 1 cycle/s = 1s-1)

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5
Q

γ-rays:

A
  • commonly referred as photons
  • bundle or particle of radiation
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6
Q

diff b/w light photons and γ-ray photons?

A

their energy (E) and f

E = hf = hc/λ

where h - Planck’s constant = 6.626*10-34 Js

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7
Q

unit f/ denotation of photon E -

A

eV - electronvolt
1 J = 6.241509*1018 eV

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8
Q

particulate radiation in diagnostic radiology and its rest m and E:

A

electron particulate radiation
rest m = 9.109*10-31 kg
rest E = 511 keV

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9
Q

Radiation is classified as ionizing/non-ionizing depending on:

A

its ability to ionize matter:
- EM radiation of frequency higher than near-UV region of EM spectrum - ionizing
- EM radiation w/ E below the far-UV region (visible light, infrared, radiofrequency) - non-ionizing

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10
Q

Interactions of photons w/ matter (3):

A
  • photoelectric absorption
  • Compton scattering
  • pair production
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11
Q

characteristic photon has E

A

characteristic of the absorbing material

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12
Q

Photoelectric absorption:

A
  • photon is absorbed by transferring all of its E to an inner orbital electron => electron is ejected & photon disappears => atom fills vacant orbit w/ outer electrons => atom releases a characteristic X-ray photon
  • the most likely form of absorption f/ incident photons w/ lower E (especially below 25 keV)
  • likelihood of photoelectric absorption increases as the cube of the atomic # Z3 => heavy metals like lead (Z=82) are good absorbers of X-ray photons
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13
Q

All interactions b/w photons & matter are probabilistic:

A

odds that a proton is absorbed by photoelectric absorption depend on chem elements in the absorbing material

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14
Q

Attenuation of an X ray beam in the air:

A

negligible

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15
Q

Attenuation of an X ray beam in the bone:

A

significant due to relatively high density (atom mass number of Ca)

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16
Q

Attenuation of an X ray beam in the soft tissue (muscle, …):

A

similar to water

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17
Q

Attenuation of an X ray beam in the fat tissue:

A

less than in water

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18
Q

Attenuation of an X ray beam in the lungs:

A

weak due to density

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19
Q

Compton effect:

A
  • interaction w/ the outer e that isn’t tightly bound to an atom: photon collides w/ an e and gives some of its E to it
  • in the “head-on” collision, photon has its direction of travelling reversed and loses max E
  • in the glancing collision, E given to the recoil e is much less
  • the Compton eff is dominant f/ photon E above 200 keV up to 2 MeV
  • a single photon may undergo several collisions, loosing some E and eventually be absorbed by the photoelectric eff
20
Q

the actual loss of E as a result of Compton scattering depends upon

A

the angle through which the photon is scattered

21
Q

depending on E of photon, what is the most dominant effect:

A
  • <25 keV - photoelectric effect
  • 60-90 keV - both photoelectric & Compton effects can occur
  • 200 keV up to 2 MeV - Compton effect
  • above 5 MeV - pair production
22
Q

why is the Compton effect relatively insensitive to variations in anatomy, compared to photoelectric effect?

A

most soft tissues have similar densities

23
Q

Compton effect depends on - ?

A

photons interact w/ electrons as though they are not bound to an atom => only total # of electrons in a block of material matters => only thickness of an absorber & its density are important f/ photon absorption

24
Q

What contributes to contrast in x-ray imaging?

A

diff in density & thickness of a tissue

25
What effect plays the dominant role in x-ray imaging?
photoelectric absorption effect plays a dominant role => contrast is affected more by chemical composition of materials and photon E
26
Pair production:
- only happens f/ very high-E protons: photon can be absorbed by an atomic nucleus in the absorber => **electron + positron** - **E is being converted to m!!!**
27
how much E is needed to produce the pair of particles, based on mass of electron and positron?
1.02 MeV, if the incident photon has more E, the excess increases the velocity of electron & positron
28
does positron live long?
no, it will not live very long, b/c if it meets an electron it can combine with it to produce 2 photons of 0.51 MeV - ***annihilation radiation***
29
PET (positron emission tomography) basis:
synchronous detection of the two 0.51 MeV γ photons to localize the emitter
30
ABSORPTION OF PHOTONS AS A FUNCTION OF ENERGY
31
Absorption processes are **NOT** the only processes that reduce the intensity of a beam of photons:
*point source*: intensity falls off as you move away from the source *if radiation from the source can spread in all directions*: its intensity will fall off in **INVERSR PROPORTION TO THE DISTANCE SQUARED**
32
The inverse square law states that:
the energy twice as far from the source is spread over four times the area thus we have one-fourth of the intensity
33
In measuring radiation, we:
can't detect it directly. Thus, we rely on it to interact w/ smth else that allows it to be detected
34
dosimeter -
instrument that measures ionizing radiation; comprises of a measuring assembly and one or more detector assemblies (may or may not be an integral part of measuring assembly)
35
examples of dosimeters:
- low levels of dose rate: **Geiger-Muller (G-M) tubes** / **scintillation counters** - high dose rate: **ionisation chambers** are more accurate & less affected by radiation E
36
Film dosimeters' advantages (5):
- not expensive - provides a permanent record - very reliable - very simple personal device - used to measure and record radiation exposure due to **γ rays, X-rays, beta particles**
37
Film dosimeters' disadvantages (3):
- can't be read on site, need to be sent for developing - not reusable - exposures of less than 0.2 mSv (millirem) can't be accurately measured
38
TLDs dosimeters' advantages (3):
- measure a great range of doses, compared to film dosimeters - doses can easily be obtained, b/c can be read on site - reusable
39
TLDs dosimeters' disadvantages (2):
- each dose can't be read out more than once - readout process "zeroes" the TLD
40
Electronic personal dosimeter:
- high range - alarming - designed to be worn by occupational radiation workers in **planned exposure situations** f/ regulatory compliance (industrial, medical) - displays dose & rate - high level of radiation sensitivity
41
Electric current is simply a flow of electrons / ions, BUT
if some of the atoms in the air are ionised, then free electrons are produced => electric current can flow *ex: flash of lightning - high potential gradient b/w cloud & ground is sufficient to ionise the air => electric current*
42
Ionisation chamber's principle of work:
ionising radiation frees electrons in the air => electrons fill the chamber => electric current when the chamber is exposed to ionising radiation, positive or negative ions are produced => they are attracted to either negative or positive plate => current flows through the chamber => current is measured by a sensitive ammeter (often of 10-9 A, which **corresponds to 6*109 electrons per second**)
43
Where are ionization chambers used?
- to measure the ionising radiation output of therapeutic & diagnostic ionising radiation generators - to make accurate measurements of patient radiation dose
44
G-M counter picture
45
G-M counters what it is and principle of work:
- very sensitive form of ionisation chamber: can detect single ionising particles which enter the tube - construction is similar to ionisation chambers: central wire electrode inside a hollow metal tube; **difference**: tube is filled w/ gas (Ar, Ne), which is at 1/5 atmospheric P => incident ionising radiation will produce free electrons within the tube => they are attracted to the central electrode (held at positive potential) => electrons are accelerated by potential => gain sufficient E => further ionisation => chain reaction => all electrons hitting the central anode can cause photons to be emitted => visible light / UV radiation => more ionisation
46
what is G-M used for?
- detection & measurements of all types of radiation: α , β, γ - NOT recommended f/ diagnostic radiology, typically designed to detect isotope emissions
47
2 main difficculties in diagnostic radiology for G-M counters:
- response time of several s - strong E dependence at low photon levels