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Radiation Fundamentals & Detection Flashcards

7 cards from real NRRPT practice questions. Tap to flip, then mark Knew It or Still Learning — missed cards come back until you master them.

Read the first 7 Radiation Fundamentals & Detection flashcards as text
  1. A sealed radioactive source contains 10 mCi of Cs-137 (T½ = 30 years). Approximately how much activity remains after 90 years?

    Answer: 1.25 mCi

    90 years = 3 half-lives; 10 × (1/2)³ = 10/8 = 1.25 mCi remaining.

  2. In a proportional counter, what is the primary advantage over an ionization chamber?

    Answer: Gas multiplication amplifying the primary ion signal

    Proportional counters operate in the gas multiplication region where avalanche ionization amplifies the primary signal by factors of 10³–10⁵.

  3. The photoelectric effect is the dominant photon interaction in tissue at energies:

    Answer: Below about 100 keV

    Photoelectric absorption dominates at low photon energies (below ~100 keV in tissue) and is highly dependent on atomic number (Z³).

  4. Which detector is best suited for measuring low-energy beta emitters like tritium (H-3)?

    Answer: Liquid scintillation counter

    Liquid scintillation counting dissolves the sample in scintillant fluid, allowing nearly 100% geometric efficiency for weak beta emitters like tritium.

  5. What is the significance of the 'dead time' in a radiation detector?

    Answer: The period after each pulse during which new events cannot be recorded

    Dead time is the minimum time that must separate two events for both to be detected; counts are lost during this interval at high count rates.

  6. Which nuclear decay mode is characterized by emission of radiation from nuclear isomers (metastable states)?

    Answer: Isomeric transition (IT)

    Isomeric transition occurs when a metastable nuclear isomer (indicated by 'm') decays to a lower energy state, typically emitting a gamma ray.

  7. The Compton edge in a gamma-ray spectrum represents:

    Answer: The maximum energy transferred to the recoil electron in Compton scattering

    The Compton edge is the maximum recoil electron energy, occurring when the photon is backscattered 180° and transfers maximum energy to the electron.