» Articles » PMID: 24694149

Tungsten Anode Spectral Model Using Interpolating Cubic Splines: Unfiltered X-ray Spectra from 20 KV to 640 KV

Overview
Journal Med Phys
Specialty Biophysics
Date 2014 Apr 4
PMID 24694149
Citations 60
Authors
Affiliations
Soon will be listed here.
Abstract

Purpose: Monte Carlo methods were used to generate lightly filtered high resolution x-ray spectra spanning from 20 kV to 640 kV.

Methods: X-ray spectra were simulated for a conventional tungsten anode. The Monte Carlo N-Particle eXtended radiation transport code (MCNPX 2.6.0) was used to produce 35 spectra over the tube potential range from 20 kV to 640 kV, and cubic spline interpolation procedures were used to create piecewise polynomials characterizing the photon fluence per energy bin as a function of x-ray tube potential. Using these basis spectra and the cubic spline interpolation, 621 spectra were generated at 1 kV intervals from 20 to 640 kV. The tungsten anode spectral model using interpolating cubic splines (TASMICS) produces minimally filtered (0.8 mm Be) x-ray spectra with 1 keV energy resolution. The TASMICS spectra were compared mathematically with other, previously reported spectra.

Results: Using pairedt-test analyses, no statistically significant difference (i.e., p > 0.05) was observed between compared spectra over energy bins above 1% of peak bremsstrahlung fluence. For all energy bins, the correlation of determination (R(2)) demonstrated good correlation for all spectral comparisons. The mean overall difference (MOD) and mean absolute difference (MAD) were computed over energy bins (above 1% of peak bremsstrahlung fluence) and over all the kV permutations compared. MOD and MAD comparisons with previously reported spectra were 2.7% and 9.7%, respectively (TASMIP), 0.1% and 12.0%, respectively [R. Birch and M. Marshall, "Computation of bremsstrahlung x-ray spectra and comparison with spectra measured with a Ge(Li) detector," Phys. Med. Biol. 24, 505-517 (1979)], 0.4% and 8.1%, respectively (Poludniowski), and 0.4% and 8.1%, respectively (AAPM TG 195). The effective energy of TASMICS spectra with 2.5 mm of added Al filtration ranged from 17 keV (at 20 kV) to 138 keV (at 640 kV); with 0.2 mm of added Cu filtration the effective energy was 9 keV at 20 kV and 169 keV at 640 kV.

Conclusions: Ranging from 20 kV to 640 kV, 621 x-ray spectra were produced and are available at 1 kV tube potential intervals. The spectra are tabulated at 1 keV intervals. TASMICS spectra were shown to be largely equivalent to published spectral models and are available in spreadsheet format for interested users by emailing the corresponding author (JMB).

Citing Articles

Towards an intelligent integrated methodology for accurate determination of volume percentages in three-phase flow systems.

Iliyasu A, Daoud M, Salama A, Guerrero J, Hirota K Sci Rep. 2025; 15(1):8407.

PMID: 40069344 PMC: 11897127. DOI: 10.1038/s41598-025-92355-4.


Maximizing microcalcification detectability in low-dose dedicated cone-beam breast CT: parallel cascades-based theoretical analysis.

Larsen T, Tseng H, Trinate R, Fu Z, Chiang J, Karellas A J Med Imaging (Bellingham). 2024; 11(3):033501.

PMID: 38756437 PMC: 11095120. DOI: 10.1117/1.JMI.11.3.033501.


Calculation method for novel upright CT scanner isodose curves.

Kissick M, Panaino C, Criscuolo A, Hayes J, Hoffman C, Mackie R J Appl Clin Med Phys. 2024; 25(7):e14377.

PMID: 38695845 PMC: 11244660. DOI: 10.1002/acm2.14377.


Technical note: SpekPy Web-online x-ray spectrum calculations using an interface to the SpekPy toolkit.

Vorbau R, Poludniowski G J Appl Clin Med Phys. 2024; 25(3):e14301.

PMID: 38363037 PMC: 10929988. DOI: 10.1002/acm2.14301.


Extremity radiographs derived from low-dose ultra-high-resolution CT: a phantom study.

Hernandez A, Bayne C, Bateni C, Lamba R, Boone J Skeletal Radiol. 2024; 53(11):2491-2497.

PMID: 38308721 DOI: 10.1007/s00256-024-04600-y.


References
1.
Akbulut S, Grieken R, Kilic M, Cevik U, Rotondo G . Identification of heavy metal origins related to chemical and morphological soil properties using several non-destructive X-ray analytical methods. Environ Monit Assess. 2012; 185(3):2377-94. DOI: 10.1007/s10661-012-2718-6. View

2.
Kumar J, Landheer D, Barnes-Warden J, Fenne P, Attridge A, Williams M . Inconsistency in 9 mm bullets measured with non-destructive X-ray computed tomography. Forensic Sci Int. 2011; 214(1-3):48-58. DOI: 10.1016/j.forsciint.2011.07.018. View

3.
Souza E, Correa S, Silva A, Lopes R, Oliveira D . Methodology for digital radiography simulation using the Monte Carlo code MCNPX for industrial applications. Appl Radiat Isot. 2008; 66(5):587-92. DOI: 10.1016/j.apradiso.2007.11.004. View

4.
Birch R, Marshall M . Computation of bremsstrahlung X-ray spectra and comparison with spectra measured with a Ge(Li) detector. Phys Med Biol. 1979; 24(3):505-17. DOI: 10.1088/0031-9155/24/3/002. View

5.
Boone J, Fewell T, Jennings R . Molybdenum, rhodium, and tungsten anode spectral models using interpolating polynomials with application to mammography. Med Phys. 1998; 24(12):1863-74. DOI: 10.1118/1.598100. View