Problem Solving in Preparation for the NRRPT Exam. David Waite, Ph.D. James Mayberry, Ph.D.
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1 Problem Solving in Preparation for the NRRPT Exam David Waite, Ph.D. James Mayberry, Ph.D. Latest Revision February 2013
2 Disclaimer The problems exhibited in this book are similar to the ones on the NRRPT examination. However, being able to successfully complete such problems does not guarantee successful results on the examination. Additional study should be performed based upon the references in the application package or as depicted on the NRRPT web site. ( History of Revisions to the Waite Book Date Made By Approved By Page Change 2013 Feb 8 D. Tucker R. Rasmussen 6.2 Corrected problem 6-1. Final answer changed from 18 mr to 180 mr. Reference to answer in discussion corrected and accompanying slight grammatical change ( An -> A ). Identified in from kenneth.j.moran@us.army.mil to NRRPT 2011 December Feb 8 D. Tucker R. Rasmussen 6.13 Reinserted Exhibit 6-4 from original. Adjusted pagination of remainder of chapter Feb 8 D. Tucker R. Rasmussen 3.1 Corrected Equation 3-1a per official Errata 2013 Feb 8 D. Tucker R. Rasmussen 7.12 Corrected equation in step 4 of problem 7-7. Answer unchanged Feb 15 D. Tucker R. Rasmussen 6.2 Equivalency sign changed to equal sign in step 5 of Problem 6-1 as identified during review of edits by R. Rasmussen.
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25 CHAPTER 3 PARTICULATE RANGE BEHAVIOR An important component of becoming competent in solving range/energy equations is that of dispelling the idea that all range/energy problems are the same; that is to say, given a type of radiation and an energy, what is the range? In this chapter it will be demonstrated that there are 5 or 6 ways that this type of problem can come up, only one of which is the given a type of radiation and energy, what is the range? The several ways will be illustrated in the example problems in this chapter, and the demonstration will begin in the context of alpha particles. Alpha Particles All of the alpha range problems presented in this chapter are doable through the use of algebra, which was summarized in the previous chapter. However, before we get to the solving of problems, perhaps a brief discussion of the physics of alpha interactions might be useful. Alpha particles are emitted from heavy radioactive nuclei monoenergetically and exhibit range behavior. That is, all alpha particles emitted with the same energy will travel about the same distance in a medium. Alpha particles are made up of two protons and two neutrons and, therefore have a mass number of 4 and a charge of +2. The large mass, relative to surrounding electrons, and the associated relatively slow velocity, in addition to the strong attractive force of the alpha particle for surrounding electrons, make the alpha interaction with matter one of the alpha causing ion pairs along its track and eventually becoming neutralized by capturing electrons. If we plot the number of alphas along a track versus the absorber thickness, a curve like that shown in Exhibit 3-1 results. Where the number of alphas goes to zero is the distance referred to as the range. It is this quantity that is the focus of problems in this chapter. Because each ion pair created by the passage of the alpha particle requires the same amount of energy (about 35 ev), it is observed that the more initial energy given the alpha particle, the longer the range. The question before us, then, is what is the mathematical relationship between the range and the energy of alpha particles? For air as the absorbing medium, the empirical relationships are: R a [cm] = 0.56E for E<4 MeV Equation 3-1a R a [cm] = 1.24E for 4<E<8 MeV Equation 3-1b 3.1
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58 These variables, constants, conversion factors and definitions are used in the design, calibration, operation and interpretation of outputs from capacitor-type detectors used for radiation protection purposes. This will be demonstrated in the following example problems. Problem 6-1 A pocket ionization chamber with a capacitance of 3 ( F) and a volume of 1 cm 3 is initially charged to 150V. What exposure to gamma radiation will discharge the chamber to 130 V? Step 1: Isolate the unknown variable: C = Q V Q = CV Step 2: Simplify the equation: The equation is already simplified. Step 3: Validate the problem setup: [coulomb] = [Farad][Volt] Step 4: Plug in known quantities: Q 1 = 3 x x 10 2 = 4.5 x coul Q 2 = 3 x x 10 2 = 3.9 x coul Q = 4.5 x x = 0.6 x coul IP 0.6 x coul = x 10 9 IP 16. x10 19 coul x 10 9 IP 35eV IP MeV 3 erg 1.6 x ev MeV Rg cm erg 129. x10 g cm Step 5: Solve for the unknown: 1.8 x 10 1 R= 180 mr Step 6: Conduct a reality check: A 180 mr exposure is a realistic outcome, based on experience with such chambers. 6.2
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69 Step 5: Solve for the unknown: P = 2.7 atm Step 6: Conduct reality check: Chambers often operate at pressures in this range. Solid State Detectors One concept that is unique to solid state detectors is their ability to indicate the energies of incident radiations. However, for this type of information to be interpreted for beneficial purposes, the detector and its associated instrumentation must be calibrated, that is, the location of the output peaks from the detector on the energy scale must be calibrated to the known energy of the radiations that gave rise to the peaks. This calibration is in addition to the calibration of NCPM/DPM discussed in the last section. In most cases, it can be assumed and confirmed that the relationship between channel number (or spectrometer setting) and energy is linear. This means that, theoretically, only two points need be specified before the line covering the whole energy spectrum can be drawn. In reality, several points are usually experimentally determined during the calibration process, to more accurately establish the location of the calibration line. Such a line is shown in Exhibit 6-4. Once the location of the calibration line is established for a detector system, then the locations of unknown lines can be translated to energies with the objective of either identifying unknown radionuclides or determining the amount of radionuclide present in the sample being counted. The utility of this process is demonstrated in the following problems Exhibit 6-4 Energy Calibration Curve Energy [kev] Channel Number 6.13
70 Problem 6-8 If the calibration line for a NaI(Tl) detector is characterized as 10 kev/channel, what is the energy of a peak observed at channel 66? Step 1: Isolate the unknown variable: Multiplicative model. Step 2: Simplify the equation: Multiplicative model. Step 3: Validate the problem setup: Will be done while solving the problem. Step 4: Plug in known quantities: 66 channel 10keV channel MeV 10 3 kev Step 5: Solve for the unknown: Energy = 0.66 MeV Step 6: Conduct reality check: Problem 6-9 Energy recognizable as that of Cs-137. If the 1.33 MeV peak from Co-60 is found in channel 1000, in what channel would its 1.17 MeV peak be expected? Step 1: Isolate the unknown variable: MeV1 = MeV 2 channel channel Step 2: Simplify the equation: 1 The equation is already simplified. Step 3: Validate the problem setup:
71 Ratio is unitless. Step 4: Plug in known quantities: 133. MeV 1000channel = 1.17MeV channel2 Step 5: Solve for unknown: channel 2 = 880 Step 6: Conduct reality check: Problem 6-10 Check arithmetic. What is the efficiency of a scintillation detector if exposure of the detector to a 10 pci sample yields 1 cpm for a peak known to have a photon yield per disintegration of 80%? Step 1: Isolate the unknown variable: CF = cpm dpm Step 2: Simplify the equation: The equation is already simplified. Step 3: Validate the problem setup: Ratio is unitless. Step 4: Plug in known quantities: CF = 1cpm ( ) 08. dpm 100 dpm = 10pCi 3.7 x 10 2 Step 5: Solve for the unknown: dis pci sec 60sec = 22.2 dpm min 6.15
72 CF = 1 ( ) = 5.63% Step 6: Conduct reality check: Answer is in a range of reasonable efficiencies. 6.16
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84 Step 4: Plug in known quantities: concentration in soil = Step 5: Solve for unknown: 1 Ci 10l 240 min l min 100m 2 0.1m Ci concentration in soil = 3 10 m Step 6: Conduct reality check: m = 3 Make independent order of magnitude estimate. 2 Ci 7.12
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