Topic 2: ionising radiation measurements + standards Flashcards

1
Q

Who discovered X-rays?

A
  • Wilhelm Conrad
  • Father of radiography
  • Mechanica engineer + physicist
  • 1895
  • By accident
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2
Q

Who discovered radioactivity?

A
  • Henri Becquerel
  • In 1896
  • Accidentally detected radiation
  • Within a year of X-ray discovery = used film + electroscope to detect ionising radiation
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3
Q

Define dosimeter

A
  • Measures ionizing radiation
  • Measuring assembly = electrometer + detector
  • Monitoring equipment calibrated = f mrad/h or µGy/h
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4
Q

What are the 2 ways to measure the dose rate?

A

1) Geiger Muller tube = low level dose rate
2) Ionization chamber = more accurate + less effected by radiation = can measure high dose rate

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5
Q

What is the standard instrument for measuring dose rate?

A
  • Ionization chamber system
  • Solid state detector + scintillation counter not suitable for routine dose measurements
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6
Q

What is a TLD?

A
  • Cheapest + most common personal monitor
  • AKA thermoluminescent dosimetry
  • Getting replaced by ionization chamber dosimeters
  • Don’t offer protection/alert to exposure/not radioactive
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7
Q

Advantages of film dosimeters

A
  • Film badge = very simple personal monitor = inexpensive
  • Permanent record
  • Very reliable
  • Measure + record exposure = gamma + X-ray + beta particles
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8
Q

Disadvantages of film dosimeters

A
  • Cannot be read on site = have to be developed
  • 1 time use
  • Exposure > 0.2 mSv gamma = not accurately measured
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9
Q

Advantages of TLDs

A
  • Measure greater range of doses compared to film
  • Doses easily obtained
  • Read on site
  • Reusable
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10
Q

Disadvantages of TLDs

A
  • Each dose cannot be read more than once
  • Readout = zeros TLD
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11
Q

Describe electronic personal dosimeters

A
  • For occupational radiation workers in planned exposure situations = measure for regulatory compliance
  • High range
  • Alarming
  • Displays dose + dose rate
  • High level sensitivity
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12
Q

Explain lightning

A
  • Electricity cannot flow in air = no free e- + ions to carry current
  • If some atoms in air ionized = free e- produced = electric current can flow
  • High potential gradient between cloud + ground
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13
Q

What is the use of ionization chambers?

A
  • Measure ionizing radiation output of therapeutic + diagnostic radiation generators
  • Used to make accurate measurements of patient radiation dose
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14
Q

Describe ionization chambers

A
  • Ionizing radiation frees e- in air of chamber
  • e- fill up chamber = allow current to flow
  • Potential applied across metal plates
  • Chamber = sealed/open
  • When chamber exposed to radiation = +/- ions produced
  • +ve attracted to -ve plate and vise versa
  • This allows current to flow through chamber
  • Current measured by sensitive ammeter because currents = 10^-9 A > 6x10^9 e- per sec
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15
Q

What is the use of GM counters?

A
  • Detect + measure all types of radiation = alpha/beta/gamma
  • Not for diagnostic radiology
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16
Q

Describe GM counters

A
  • Very sensitive form of ionization chamber = can detect single ionizing particle entering tube
  • Structure = central wire electrode inside hollow metal tube
  • Difference from ionization chamber = filled with gas e.g. argon/neon instead of air
  • Gas 1/5th atm
  • Incident ionizing radiation = produce free e- in tube = attracted to central electrode = positive potential
  • e- attracted towards central anode = accelerated by potential = gain energy to further ionize = chain reaction
  • When all e- produced = hit central anode = photons emitted = cause more ionisation in chamber
17
Q

How many e- can the original ionizing radiation produce in GM tube?

A
  • 10^5
  • Measured as a pulse current = 1µs
18
Q

What is the disadvantage of the GM tube?

A
  • Positive ions = travel slowly compared to e-
  • Tube takes long to recover from recorded pulse
  • Causes dead time = limits number of events that can be recorded each second
19
Q

2 difficulties in diagnostic radiology with GM counter

A

1) Several-second response time
2) Strong energy dependence at low photon energy