M [scale units/s] of the system

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APPENDIX TO IAEA CALIBRATION CERTIFICATE RADIATION PROTECTION IONIZATION CHAMBER CALIBRATION PROCEDURES AT THE IAEA DOSIMETRY LABORATORY 1. INTRODUCTION 1.1 General Ionization chambers and electrometers are calibrated at the IAEA Dosimetry Laboratory in terms of air kerma free in air (N K ) and ambient dose equivalent (H*(10)), in 60 Co, 137 Cs gamma radiation and also ISO 4037 X ray narrow spectra series [1]. Calibrations are either made for a system composed of an ionization chamber plus an electrometer (from here on called system calibration ) or for an ionization chamber only. Calibrations are performed using the beam output data that was measured using the IAEA reference standard chamber. This reference standard is calibrated at the BIPM or a Primary Standards Dosimetry Laboratory (PSDL) participating in the mutual recognition arrangement (MRA), every 3 years. For calibrations of the ionization chamber only, the current is measured with the IAEA reference electrometer. With system calibrations, the internal bias supply in the electrometer/dosimeter is used for the polarizing voltage. No correction for the possible lack of saturation is applied. The relative air humidity at the dosimetry laboratory is kept between 30 % and 70 %. No correction is applied for this influence quantity (see Section 4). The air kerma calibration coefficient N K [mgy/nc] of the chamber alone is determined as the ratio of the air kerma rate K [mgy/s] obtained with the IAEA reference standard, and the ionization current I [na] from the chamber air under calibration corrected for the influence quantities for pressure (P) and temperature (T). The ambient conditions (temperature, pressure and humidity), prevailing at the IAEA Laboratory during the calibrations, are monitored continuously. Typically, the temperature fluctuations in the laboratory are within 20 C - 24 C and during measurements about 0.5 C. The air kerma calibration coefficient N K [mgy/scale unit] of the system is determined as the ratio of the air kerma rate K [mgy/s] obtained with the IAEA reference standard, and the reading rate air M [scale units/s] of the system (electrometer and ionization chamber), corrected for the influence quantities P and T. The same procedure is followed to determine the ambient dose equivalent calibration coefficient. 1.2 Reference conditions The reference point of the ionization chamber, where the calibration coefficients apply, is considered to be in the geometrical centre of the collecting volume as defined by the external walls (unless another indication is given). Details on the geometrical centre for each specific chamber are given in the operation manual of the ionization chamber. If the chamber stem has a mark, this mark is oriented towards the radiation source during the calibration. The distance between the reference point and the source is 3 m (see Figures 1 and 2). 2 AIR KERMA CALIBRATIONS 2.1 137 Cs and 60 Co gamma radiation The chamber, with the build-up cap (where applicable), is positioned free in air, so that its reference point is on the central axis of the beam. The chamber reference plane is perpendicular to the central axis of the beam. The distance from the source to the reference point of the chamber is 3 m. The size of the radiation field (50 % isodose level) at the reference plane is 75 cm. Fig. 1 shows the set-up. 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 1 of 9

Fig. 1: Set-up for calibration in terms of air kerma for 137 Cs and 60 Co gamma radiation. 2.2 X ray beams Two X ray tubes are used to generate the ISO 4037 narrow spectrum X ray beam series reference radiation. The characteristics of the beams are shown in Table I [1]. The chamber, with its build-up cap (if applicable), is positioned free in air, so that its reference point is on the central axis of the beam. The reference plane of the chamber must be perpendicular to the central axis of the beam. The distance from the focus of the X ray tube to the reference point of the chamber is 2 m. The size of the radiation field (50 % isodose level) at the reference plane is 26 cm. Fig. 2 shows the set-up. Fig. 2: Set-up for calibration in terms of air kerma for X ray beams. The characteristics of the X ray beams used for calibration are given in Table I below. 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 2 of 9

TABLE I: Beam qualities at the IAEA for the ISO 4037 Narrow Spectrum Series [1] Radiation quality H.V. [kv] Al [mm] Added filtration * Cu Sn [mm] [mm] Pb [mm] HVL Al Cu [mm] [mm] N40 40 4.0 0.22 2.72 N60 60 4.0 0.74 0.24 N80 80 4.0 2.0 0.59 N100 100 4.0 5.0 1.13 N120 120 4.0 5.0 1.0 1.75 N150 150 4.0 2.5 2.42 N200 200 4.0 2.0 3.0 0.5 3.92 N250 250 4.0 2.1 2.0 5.18 N300 300 4.0 3.0 3.9 6.20 * ) Permanent filtration is 3 mm Be 3 CALIBRATIONS IN TERMS OF AMBIENT DOSE EQUIVALENT The ambient dose equivalent is an operational quantity. Definitions of operational quantities used in radiation protection dosimetry are given in IAEA Basic Safety Standards [3] and IAEA Safety Series No.16 [4]. The set-up used of the calibration of ionization chambers in terms of ambient dose equivalent is identical to that of air kerma calibrations. 4. USE OF CALIBRATION COEFFICIENTS The reference instruments calibrated at the IAEA can be used, in another radiation beam, to determine that beam s output rate (air kerma or absorbed dose to water), subject to the provisions listed below: - The humidity conditions should not differ significantly from those prevailing at the IAEA Dosimetry Laboratory. If the relative humidity is outside the range of 30 % - 70 %, corrections based on [4] should be made. - The condition of measurement must not differ significantly from those of the calibration at the IAEA. Otherwise, additional corrections may be needed. In particular: the radiation quality (particularly for X ray beams); the calibration distance and beam dimensions of the radiation beam; the radial non-uniformity of the beam over the cross section of the ionization chamber; the beam intensity. It should be noted that the calibration coefficients determined at the IAEA are not corrected for or the lack of saturation due to recombination. If the instrument is used in beams different from those listed in the calibration certificate, the user is advised to correct for this effect. Additional information on this effect can be found in [1]; and the polarity and scale used during the calibration at the IAEA are reported in the calibration certificate. If the instrument is used with a different polarity or scale from those listed in the calibration certificate, the user is advised to determine the effect of these differences and decide on their effects on the measurements. Additional information on these effects and ways to correct for them can be found in [1]. 5. CALIBRATION UNCERTAINTIES The methodology for estimating the uncertainties of calibrations at the IAEA Dosimetry Laboratory is based on the recommendations of the ISO and IAEA guides on uncertainty [5] and [6]. All sources of uncertainty are identified and classified as Type A or Type B, as per ISO classification. The uncertainty associated to IAEA calibrations is a combined standard uncertainty, with a coverage factor of k=2, which for a normal distribution corresponds to a level of confidence of approximately 95 %. The contributions to the total uncertainty in the calibration coefficient are determined in 2 steps: 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 3 of 9

1. uncertainties arising from measurements made to determine the output rate (air kerma rate or absorbed dose to water rate) of the radiation beams, with the IAEA reference instrument (including the stability of the measurement standards), and 2. uncertainties related to the instruments to be calibrated (user s instrument). Instruments calibrated at the IAEA are reference class instruments. Typical uncertainties are assumed for these instruments. These 2 components are further divided into sub-components and their classification (Type A or Type B) determined. Uncertainty budgets of IAEA calibrations are given in Tables II-VI. 6. REFERENCES [1] INTERNATIONAL ORGANIZATION FOR STANDARDIZATION, X and gamma reference radiation for calibrating dosemeters and doserate meters and for determining their response as a function of photon energy, ISO 4037 Parts 1-3, Geneva (1999). [2] INTERNATIONAL ATOMIC ENERGY AGENCY, Calibration of Dosimeters Used in Radiotherapy, Technical Report Series No. 374, IAEA, Vienna (1994). [3] INTERNATIONAL ATOMIC ENERGY AGENCY, International Basic Safety Standards for Protection Against Ionizing Radiation and for the Safety of Radiation Sources, Safety Series No. 115, IAEA, Vienna (1996). [4] INTERNATIONAL ATOMIC ENERGY AGENCY, Calibration of Radiation Protection Monitoring Instruments, Safety Series No.16, IAEA, Vienna (2000). [5] INTERNATIONAL ATOMIC ENERGY AGENCY, Absorbed Dose Determination in External Radiotherapy: an International Code of Practice for Dosimetry Based on Standards on Absorbed Dose to Water, Technical Reports Series No. 398, IAEA, Vienna (2000). [6] INTERNATIONAL ATOMIC ENERGY AGENCY, Measurement Uncertainty A Practical Guide for. Secondary Standards Dosimetry Laboratories, TECDOC-1585, IAEA, VIENNA (2008). 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 4 of 9

Table II ISO 4037 Narrow Spectrum Series: Air kerma rate Corresponding to CMC entry: IAEA-RAD-1008 Air kerma rate Type A Type B Calibration from BIPM/PSDL 0.39 Long term stability of the secondary standard 0.29 Temperature and Pressure 0.06 0.10 Current 0.06 0.10 Monitor chamber 0.01 Relative combined standard uncertainty in Step 1 0.09 0.51 Chamber positioning 0.01 Monitor chamber 0.01 Beam quality 0.17 Uniformity of radiation field 0.12 Relative combined standard uncertainty in Step 2 0.09 0.31 Relative combined standard uncertainty (Steps 1 + 2) 0.12 0.59 Overall relative uncertainty 0.60 Relative expanded uncertainty (k=2) 1.2 % 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 5 of 9

Table III 60 Co and 137 Cs gamma radiation: Air kerma rate Corresponding to CMC entry: IAEA-RAD-1009 and IAEA-RAD-1010 Air kerma rate Type A Type B Calibration from BIPM/PSDL 0.25 Long term stability of the secondary standard 0.17 Current 0.05 0.10 Relative combined standard uncertainty in Step 1 0.06 0.33 Chamber positioning 0.01 Uniformity of radiation field 0.10 Relative combined standard uncertainty in Step 2 0.07 0.25 Relative combined standard uncertainty (Steps 1 + 2) 0.09 0.41 Overall relative uncertainty 0.42 Relative expanded uncertainty (k=2) 0.8 % 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 6 of 9

Table IV ISO 4037 Narrow Spectrum Series: Ambient dose equivalent rate Corresponding to CMC entry: IAEA-RAD-1011 Ambient dose equivalent rate Type A Type B Calibration from BIPM/PSDL 1.50 Long term stability of the secondary standard 0.23 Current 0.06 0.10 Monito chamber 0.01 Relative combined standard uncertainty in Step 1 0.07 1.52 Chamber positioning 0.01 Monitor chamber 0.01 Beam quality 0.17 Uniformity of radiation field 0.12 Relative combined standard uncertainty in Step 2 0.07 0.31 Relative combined standard uncertainty (Steps 1 + 2) 0.10 1.55 Overall relative uncertainty 1.56 Relative expanded uncertainty (k=2) 3.1 % 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 7 of 9

Table V 137 Cs gamma radiation: Ambient dose equivalent rate Corresponding to CMC entry: IAEA-RAD- 1012 Ambient dose equivalent rate Type A Type B Calibration from BIPM/PSDL 0.52 Long term stability of the secondary standard 0.17 Current 0.05 0.10 Relative combined standard uncertainty in Step 1 0.06 0.57 Chamber positioning 0.05 Uniformity of radiation field 0.10 Relative combined standard uncertainty in Step 2 0.07 0.25 Combined standard uncertainty (Steps 1 + 2) 0.09 0.62 Overall relative uncertainty 0.62 Relative expanded uncertainty (k=2) 1.2 % 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 8 of 9

Table VI 60 Co gamma radiation: Ambient dose equivalent rate Corresponding to CMC entry: IAEA-RAD-1013 Ambient dose equivalent rate Type A Type B Calibration from BIPM/PSDL 0.33 Long term stability of the secondary standard 0.36 Current 0.05 0.10 Relative combined standard uncertainty in Step 1 0.06 0.51 Chamber positioning 0.05 Uniformity of radiation field 0.12 Relative combined standard uncertainty in Step 2 0.07 0.26 Combined standard uncertainty (Steps 1 + 2) 0.09 0.57 Overall relative uncertainty 0.58 Relative expanded uncertainty (k=2) 1.2 % 2011-08-25 rev. 6 Appendix 3B DOLP.011 Page 9 of 9