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Absorbed Dose to Water Calibration of a Radiation Detector

Absorbed Dose to Water Calibration of a Radiation Detector

SKU: 46110C
Availability:

This service is temporarily unavailable until further notice due to building renovations.


Primary NIST Technical Contact:
Name: Ronaldo Minniti
Phone: (301) 975-5586

Secondary NIST Technical Contact:
Name: Michael Mitch
Phone: (301) 975-5491

In a 60Co Gamma-Ray Beam (1 dose rate)


NIST calibrated x-ray measuring instruments are calibrated in terms of air kerma or exposure by a substitution method in an x-ray beam at a point where the rate has been determined by means of a free-air ionization chamber standard. In order to provide instrument calibrations over a wide range of x-ray beam qualities, many combinations of generating potential and filtration are available. Tungsten (W) anode, x-ray beams with U.S. established beam qualities are listed in Table 6 as lightly (L), moderately (M), and heavily (H) filtered beams. Two beam qualities that do not fit into these categories are considered as special (S) qualities. Cobalt-60 and cesium-137 gamma-ray beams are also listed in Table 6. New W-anode, ISO x-ray beam qualities, listed in Table 7 have been installed. Molybdenum (Mo) and rhodium (Rh) anode x-ray beam qualities, with application to mammography, are listed in Table 8. Tungsten-anode beam qualities used in international comparisons are listed in Table 9. Beam qualities are identified by beam codes given in the first column. The calibration beam qualities requested should be appropriate to the instrument submitted.

Gamma-ray measuring instruments are calibrated in terms of air kerma or absorbed dose at points in the collimated cobalt-60 and cesium-137 gamma-ray beams that have been standardized by means of graphite cavity chambers or a water (or graphite) calorimeter. Rates at the time of calibration are computed from the original beam standardization data and appropriate decay corrections. Ionization chambers submitted for an air kerma calibration should have sufficient wall thickness to provide electron equilibrium for the highest energy selected. Ionization chambers submitted for an absorbed-dose calibration must be suitable for calibration in a phantom.

An ionization chamber submitted without an electrometer is calibrated in terms of air kerma or absorbed dose per unit charge, normalized to reference conditions of 295.15 K and 101.325 kPa. Calibration can be based on measurements for positive or negative polarizing potential, or on the mean of measurements for both potentials, as requested. The ratio of ionization currents for full and half polarizing potentials and the corresponding ionization current will be stated in the calibration certificate, based on pre-calibration measurements. An ionization chamber and electrometer combination, with the electrometer scale in units of air kerma, exposure, or absorbed dose, is calibrated by providing a dimensionless calibration factor for the electrometer scale. An ionization chamber and electrometer combination marked in electrical units is calibrated as follows: (1) the chamber is calibrated in terms of air kerma or absorbed dose per unit charge using an NIST electrometer; (2) the customer's electrometer is checked for linearity and charge measurement accuracy; and (3) the combination of chamber and electrometer is checked for consistency. Chambers found unsuitable for calibration will be returned with a statement of the reason for rejection. A charge may be made for time incurred on the tests.

The calibration of well-type ionization chambers, instruments that measure x-rays from electronic brachytherapy sources, is performed in terms of the physical quantity air-kerma in units of Gy. Calibrations are performed by comparing the well-type ionization chamber response to air kerma realized by a NIST primary x-ray standard. The measurement process results in a NIST calibration coefficient for the well chamber for each source in units of the NIST air-kerma rate (Gy/s) at 50 cm per ampere, Gy/(A s) normalized to 295.15 K (22 oC) and 101.325 kPa (1 Atm). Only well-ionization chambers known to be stable and reproducible are accepted for calibration in this program. Facilities submitting well-ionization chambers for calibration are strongly urged to perform stability checks involving redundant measurements in highly reproducible radiation fields before sending their instruments to NIST, and to repeat those checks after NIST calibration, and again at suitable intervals. The appropriate chamber insert must be provided by the customer.

Each instrument submitted to NIST for dosimetry calibration or test must be uniquely identified, usually by the manufacturer's name, model number, and instrument serial number. When the serial number is lacking, an alternative identifying mark should be provided. If none is found, NIST will mark the piece with an identification number. If the apparatus submitted has been calibrated previously by NIST, the serial number or identifying mark should be given on the new order so that a continuing record of stability can be maintained.

All shipments to NIST of instruments for dosimetry calibration must be in reusable containers. Even if properly packed, there can be no assurance that a calibrated instrument has maintained its calibration during shipment unless a method of verifying instrument stability has been established. Measurement should be made of the instrument response both before and after shipment, using a long-lived radioactive source and a highly reproducible measurement procedure. A long-term record of instrument stability using a suitable constancy check procedure is the most effective method for assuring the validity of the instrument calibration.

Irradiation of passive dosimeters, for readout by the customer, is available for most of the beam qualities listed in Table 6. These irradiations are generally in terms of air kerma; for passive dosimeters suitable for insertion in a phantom, irradiation in terms of absorbed dose can be provided by in-phantom irradiation using cobalt-60 gamma rays.

Calibrations of x-ray and gamma-ray measuring instruments and of passive dosimeters, described above, have a relative expanded uncertainty of 1 %.


Table 6. Tungsten-Anode X-Ray and Gamma-Ray Beam-Quality Parameters

Beam codeaAdditional filtrationbHalf-value layerc (HVL)Homogeneity Coefficientd (HC)Effective Energy (keV)
 Al
(mm)
Cu
(mm)
Sn
(mm)
Pb
(mm)
Al
(mm)
Cu
(mm)
AlCu 
X-Ray Beam Qualities
L100   0.037 86  
L150   0.059 70  
L200   0.070 72  
L300.3   0.23 60  
L400.53   0.52 61  
L500.71   0.79 63  
L801.45   1.81 56  
L1001.98   2.80 58  
M200.27   0.15 72  
M300.5   0.36 65  
M400.89   0.74 67  
M501.07   1.04 68  
M601.81   1.680.0526360 
M802.86   3.080.16761 
M1005.25   5.100.27455 
M1207.12   6.770.317653 
M1505.250.25  10.300.668663 
M2004.351.12  14.731.649468 
M2505.253.2  18.493.29885 
M3004.25 6.5 21.775.310097 
H100.105   0.051 77  
H150.5   0.16 87  
H201.01   0.36 89  
H304.50   1.20 86  
H404.530.26  2.93 94  
H504.0  0.14.160.14929338
H604.00.61  6..060.25929446
H1004.05.2  13.511.15989280
H1504.041.51 16.932.439996120
H2004.00.64.160.7719.724.109999166
H2504.00.61.042.7221.595.199998211
H3004.1 3.05.023.556.199898252
S604.35   2.810.097466 
S751.50   1.81 58  
Gamma-Ray Beams
137Cs     10.8  662
60Co     14.9  1250

aFor the x-ray beam codes, the letter indicates light (L), moderate (M), heavy (H) and special (S) filtration, and the number is the constant potential in kilovolts.
bThe additional filtration value does not include the inherent filtration. The inherent filtration is approximately 1.0 mm Be for beam codes L10-L100, M20-M50, H10-H40 and S75; and 3.0 mm Be for beam codes M60-M300, H50-H300 and S60.
bThe x-ray tubes were installed in 2008 and 2015.
cThe HVL values were determined for the tubes installed in 2006 and 2008. For 137Cs and 60Co, the half-value layers are calculated,
d The homogeneity coefficient is taken as 100 (1st HVL / 2nd HVL).

Table 7. Tungsten-Anode ISO X-Ray Beam-Quality Parameters

Beam codeAdditional filtration (mm)aFirst HVLbSecond HVLb
 AlCuSnPbAl
(mm)
Cu
(mm)
Al
(mm)
Cu
(mm)
HK10    0.042 0.045 
HK200.15   0.128 0.170 
HK300.52   0.408 0.569 
HK603.19    0.079 0.113
HK1003.900.15   0.298 0.463
HK200 1.15   1.669 2.447
HK250 1.60   2.463 3.37
HK280 3.06   3.493 4.089
HK300 2.51   3.474 4.205
WS60 0.3   0.179 0.206
WS80 0.529   0.337 0.44
WS110 2.0295   0.97 1.13
WS150  1.03  1.88 2.13
WS200  2.01  3.09 3.35
WS250  4.01  4.30 4.50
WS300  6.54  5.23 5.38
NS100.095   0.049 0.061 
NS150.49   0.153 0.167 
NS200.90   0.324 0.351 
NS252.04   0.691 0.762 
NS304.02   1.154 1.374 
NS40 0.21   0.082 0.094
NS60 0.6   0.241 0.271
NS80 2.0   0.59 0.62
NS100 5.0   1.14 1.19
NS120 4.991.04  1.76 1.84
NS150  2.50  2.41 2.57
NS200 2.042.98

1.003

 4.09 4.20
NS250  2.012.97 5.34 5.40
NS300  2.994.99 6.17 6.30
LK100.30   0.061   
LK202.04   0.441   
LK303.980.18  1.492   
LK35 0.25  2.21   
LK55 1.19   0.260  
LK70 2.64   0.509  
LK100 0.522.0  1.27  
LK125 1.04.0  2.107 2.094
LK170 1.03.01.5 3.565 3.952
LK210 0.52.03.5 4.726 4.733
LK240 0.52.05.5 5.515 5.542

aThe additional filtration does not include the inherent filtration. The inherent filtration is a combination of the filtration due to the monitor chamber plus 1 mm Be for beam codes LK10-LK30, NS10-NS30, HK10-HK30; for all other techniques the inherent filtration is adjusted to 4 mm Al. 
bThe HVL values were determined for the tubes installed in 2008 and 2008.


Table 8. Mammography X-Ray Beam-Quality Parameters

Beam codeTube voltage kV)Additional filtrationa (mm)Half-value layer (mm Al)
Mo Anodeb
Mo/Mo23230.032 Mo0.288
Mo/Mo25250.032 Mo0.313
Mo/Mo28280.032 Mo0.346
Mo/Mo30300.032 Mo0.370
Mo/Mo35350.032 Mo0.404
Mo/Rh28280.029 Rh0.420
Mo/Rh32320.029 Rh0.453
Mo/Mo25x250.030 Mo + 2.0 Al0.551
Mo/Mo28x280.030 Mo + 2.0 Al0.589
Mo/Mo30x300.030 Mo + 2.0 Al0.633
Mo/Mo35x350.030 Mo + 2.0 Al0.715
Rh Anode
Rh/Rh25250.029 Rh0.351
Rh/Rh30300.029 Rh0.438
Rh/Rh35350.029 Rh0.512
Rh/Rh40400.029 Rh0.559
Rh/Rh30x300.029 Rh + 2.0 Al0.814
Rh/Rh35x350.029 Rh + 2.0 Al0.898

aThe additional filtration value does not include the inherent filtration, which is comprised of 1.0 mm Be from the x-ray tube window and 0.075 mm polyamide from the transmission monitor.
bThe HVL values were measured directly using the Mo anode installed in December 2008.


Table 9. CCRIa Medium-Energy X-Ray Beam Quality Parameters Offered at NIST

Beam codeTube voltage (kV)Additional filtrationbHalf-value layerc (mm Cu) voltage (kV)
(mm Al)(mm Cu)
BIPM25250.373 0.240 mm Al
BIPM30300.208 0.167 mm Al
BIPM40403.9890.2122.649 mm Al
BIPM50a503.989 2.291 mm Al
BIPM50b501.007 1.038 mm Al
BIPM1001003.248 0.149 mm Cu
BIPM1351351.0600.2650.496 mm Cu
BIPM1801803.8420.4821.003 mm Cu
BIPM2502503.8421.6182.502 mm Cu

a BIPM, Qualites de rayonnements, Consultative Committee for Ionizing Radiation (CCEMRI) (Section I), 1972, 2, R15. Details of these reference radiation qualities can be found in the following: Burns, D. T. and O'Brien, M. , "Comparison of the NIST and BIPM Standards for Air Kerma in Medium-Energy X-rays," J.Res. Natl. Inst. Stand. Technol. 111, 385-391 (2006) and Burns, D.T., Kessler, C. and O'Brien, M., "Key comparison BIPM.RI(I)-K2 of the air-kerma standards of the NIST, USA and the BIPM in low-energy x-rays," Metrologia 49 06006 (2012).
b The additional filtration does not include the inherent filtration of x-ray tubes which is approximately 3mm Be and 1 mm Be.
c The HVL values were determined for the tubes installed in 2008 and 2015.

Calibration of a 137Cs δ-ray beam irradiator using large size chambers, R. Minniti, S. M. Seltzer, Applied Radiation and Isotopes 65, (2007) 401-406.

Absorbed Dose to Water Calibration of Ionization Chambers in a 60Co Gamma-Ray Beam, R. Minniti, J. Shobe, S. M. Seltzer, H. Chen-Mayer, S. R. Domen, NIST Special Publ. 250-74, (Mar. 2007).

NIST Measurement Services: Calibration of X-Ray and Gamma-Ray Measuring Instruments, P. J. Lamperti, and M. O'Brien, Natl. Inst. Stand. Technol. Spec. Publ. 250-58 (Apr. 2001).

The photon-fluence scaling theorem for Compton-scattered radiation, J. S. Pruitt and R. Loevinger, Med. Phys. 9, 176 (1982).

The Graphite Calorimeter as a Standard of Absorbed Dose for Cobalt-60 Gamma Radiation, J. S. Pruitt, S. R. Domen, and R. Loevinger, J. Res. Natl. Bur. Stand. (U.S.) 86 (5), 495-502 (1981).

Medical Dosimetry Standards Program of the National Bureau of Standards, R. Loevinger, Proc. Symp. on Natl. and Intl. Standardization in Rad. Dosimetry, Atlanta, GA, Dec. 5-9, 1977, Intl. Atomic Energy Agency, Vienna (1978). (This article provides references for earlier publications on NBS exposure and absorbed-dose standards.)

Uncertainty in the Delivery of Absorbed Dose, R. Loevinger and T. P. Loftus, Ionizing Radiation Metrology, International Course at Varenna, Italy, 1974 (E. Casnati, Ed.) G-6, 459, Editrice Compositori, Bologna (1977).

Exposure Spectra from the NBS Vertical-Beam 60Co Gamma-Ray Source, M. Ehrlich and C. G. Soares, Natl. Bur. Stand. (U.S.) NBSIR 76-1117 (1976).

Spectrometry of a 60Co Gamma-Ray Beam Used for Instrument Calibration, M. Ehrlich, S. M. Seltzer, M. J. Bielefeld, and J. I. Trombka, Metrologia 12, 169 (1976).

Please contact the NIST Technical Contact listed above before sending your equipment for calibration. A shipping address and RMA number will be provided after an order is placed.