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P A Jursinic

Publications and source records attributed to P A Jursinic.

17 recordsLinked to original sources
PubMed2003

Characteristics of sensitometric curves of radiographic films.

A new type of radiographic film, EDR (extended dose range) film, has been recently become available for film dosimetry. It is particularly attractive for composite isodose verification of intensity modulated radiation therapy because of its low sensitivity relative to the more common Kodak XV film. For XV film, the relationship between optical density and dose, commonly known as the sensitometric curve, depends linearly on the dose at low densities. Unlike XV film, the sensitometric curve of EDR film irradiated by megavoltage x rays is not linearly dependent on the dose at low densities. In this work, to understand the mechanisms governing the shape of the sensitometric curves, EDR film was studied with kilovoltage x rays, 60Co gamma rays, megavoltage x rays, and electron beams. As a comparison, XV film was also studied with the same beams mentioned above. The model originally developed by Silberstein [J. Opt. Soc. Am. 35, 93-107, 1945)] is used to fit experimental data. It is found that the single hit model can be used to predict the sensitometric curve for XV films irradiated by all beams used in this work and for EDR films exposed to kilovoltage x rays. For EDR film irradiated by 60Co gamma rays, megavoltage x rays, and electron beams, the double hit model is used to fit the sensitometric curves. For doses less than 100 cGy, a systematic difference between measured densities and that predicted by the double hit model is observed. Possible causes of the observed differences are discussed. The results of this work provide a theoretical explanation of the sensitometric behavior of EDR film.

Dose-Response Relationship, Radiation↗
PubMed2002

Evaluation of Kodak EDR2 film for dose verification of intensity modulated radiation therapy delivered by a static multileaf collimator.

A new type of radiographic film, Kodak EDR2 film, was evaluated for dose verification of intensity modulated radiation therapy (IMRT) delivered by a static multileaf collimator (SMLC). A sensitometric curve of EDR2 film irradiated by a 6 MV x-ray beam was compared with that of Kodak X-OMAT V (XV) film. The effects of field size, depth and dose rate on the sensitometric curve were also studied. It is found that EDR2 film is much less sensitive than XV film. In high-energy x-ray beams, the double hit process is the dominant mechanism that renders the grains on EDR2 films developable. As a result, in the dose range that is commonly used for film dosimetry for IMRT and conventional external beam therapy, the sensitometric curves of EDR2 films cannot be approximated as a linear function, OD = c * D. Within experimental uncertainty, the film sensitivity does not depend on the dose rate (50 vs 300 MU/min) or dose per pulse (from 1.0 x 10(-4) to 4.21 x 10(-4) Gy/pulse). Field sizes and depths (up to field size of 10 x 10 cm2 and depth = 10 cm) have little effect on the sensitometric curves. Percent depth doses (PDDs) for both 6 and 23 MV x rays were measured with both EDR2 and XV films and compared with ion chamber data. Film data are within 2.5% of the ion chamber results. Dose profiles measured with EDR2 film are consistent with those measured with an ion chamber. Examples of measured IMRT isodose distributions versus calculated isodoses are presented. We have used EDR2 films for verification of all IMRT patients treated by SMLC in our clinic. In most cases, with EDR2 film, actual clinical daily fraction doses can be used for verification of composite isodose distributions of SMLC-based IMRT.

Adult↗
PubMed2001

Implementation of an in vivo diode dosimetry program and changes in diode characteristics over a 4-year clinical history.

An in vivo dosimetry system that used n-type semiconductor diodes with integral build-up caps was introduced into the clinic. Measurements were made on the entrance surface of the patient and were compared to calculated diode readings expected from monitor units delivered by each beam. A method is given for calibration and correction for changes in diode sensitivity, dose-per-pulse effects, collimated field-size (head-scatter factor), wedges, compensators, and scatter from blocks and block trays. Clinically relevant temperature corrections are determined based on temperature measurements made with the diode used as a thermistor. Changes in diode characteristics over 4 years of clinical use are presented. With proper correction for clinical variables it is shown that difference between calculated and measured diode readings are within +/- 1% for phantom measurements and within +/- 3% for clinical measurements at a 95% confidence level. The correlation of dose measurements on the patient surface to dose inside a target volume is discussed.

Biophysical Phenomena↗
PubMed2000

Comparison of dosimetric characteristics of Siemens virtual and physical wedges.

Dosimetric properties of Virtual Wedge (VW) and physical wedge (PW) in 6 and 23 MV photon beams from a Siemens Primus linear accelerator, including wedge factors, depth doses, dose profiles, peripheral doses and surface doses, are compared. While there is a great difference in absolute values of wedge factors, VW factors (VWFs) and PW factors (PWFs) have a similar trend as a function of field size. PWFs have a stronger depth dependence than VWF due to beam hardening in PW fields. VW dose profiles in the wedge direction, in general, match very well with PW, except in the toe area of large wedge angles with large field sizes. Dose profiles in the nonwedge direction show a significant reduction in PW fields due to off-axis beam softening and oblique filtration. PW fields have significantly higher peripheral doses than open and VW fields. VW fields have similar surface doses as the open fields while PW fields have lower surface doses. Surface doses for both VW and PW increase with field size and slightly with wedge angle. For VW fields with wedge angles 45 degrees and less, the initial gap up to 3 cm is dosimetrically acceptable when compared to dose profiles of PW. VW fields in general use less monitor units than PW fields.

Humans↗
PubMed1999

Measurements of head-scatter factors with cylindrical build-up caps and columnar miniphantoms.

Head-scatter factors, Sh, also referred to as output factors, are measured in-air with an ion chamber and a semiconductor diode fitted with cylindrical build-up caps and columnar miniphantoms fabricated from materials of different atomic number. Sh increases with field size less rapidly when cylindrical build-up caps are constructed from high atomic number materials. This is a consequence of a net scatter of contamination electrons away from the detector. Ion chambers and diodes give identical results when the same type of build-up caps are used. Contamination electrons can be avoided by the use of columnar miniphantoms that have sufficient wall thickness in the radial direction. This radial wall thickness is characterized in this work for 6, 10, and 18 MV x-ray beams. Sh increases with field size less rapidly when columnar miniphantoms are constructed from high atomic number materials. This is due to the decrease in the average energy of photons at large field sizes. It is concluded that to obtain Sh for dosimetry in water, cylindrical build-up caps and columnar miniphantoms should be constructed from material with an atomic number close to that of water.

Calibration↗
PubMed1999

Changes in incident photon fluence of 6 and 18 MV x rays caused by blocks and block trays.

When a block and tray are placed in a x-ray beam the dose to a point in a phantom is changed by the following factors: (1) attenuation of photon and electron fluence from the head of the accelerator by the tray and the block, (2) decrease in the scatter in the phantom by a reduction in the phantom volume that receives radiation, and (3) generation of scatter off the tray and block. This third factor is generally ignored in dosimetry calculation but has been measured in this work. Measurements of incident photon fluence for 6 and 18 MV x rays were made with a columnar miniphantom of 10 cm depth. The tray factor for a 9 mm thick Lexan tray is found to be variable and to increase by 1.8% due to scatter off the tray when the field size is increased from a 3cm x 3 cm to 40cm x 40 cm field. Also, it was found that scatter off a block could increase the incident photon fluence by as much as 2%. The magnitude of this block scatter depends on the length of the inner edge of the opening in the block and on amount of block that is being irradiated, the overlap of the block by the radiation field. The total block-tray factor can be as much as 3% larger than the single-value tray factor measured with a 10cm x 10cm field that is traditionally used. An analytical equation is developed that accurately models the block-tray factor.

Models, Theoretical↗
PubMed1997

A sector-integration method for calculating the output factors of irregularly shaped electron fields.

An empirical model is presented that uses a sector-integration method for calculating the output factors of irregularly shaped electron fields. The sector-integration method accounts for changes in electron fluence, lateral scatter equilibrium, and scatter from the edge of a cutout shield. This method is tested for elliptical and rectangular fields with a ratio of the long-to-short axis as great as 4 to 1. Differences between measured and calculated values for output factors were less than +/- 1%. Comparisons were also carried out for a large number of cutout shields that were used in the clinic and similar levels of accuracy were obtained.

Biophysical Phenomena↗
PubMed1997

Clinical implementation of a two-component x-ray source model for calculation of head-scatter factors.

A calculation method is described, which presumes that linac output has two components. One component is direct x rays from the target and the remaining component is an extra-focal, distributed source of radiation that is scattered from the flattening filter, primary collimator, and the jaws of the moveable collimator. This calculation method gives values for output factors that differ from measured values by no more than 0.5% for field widths from 4 to 40 cm, rectangular fields with long to short axis ratios as great as 10, symmetric and asymmetric fields, and source-to-axis distances from 65 to 360 cm. While this calculation method has great accuracy and flexibility, a minimal amount of input data is required: (1) measured output factors at a source-to-axis distance of 100 cm for square fields; (2) positions of the collimator with respect to the x-ray source target; and (3) output factors measured at various source-to-axis distances for a 10 cm x 10 cm field.

Models, Theoretical↗
PubMed1996

Characteristics of secondary electrons produced by 6, 10 and 24 MV x-ray beams.

Megavoltage x-ray beams generated by linear accelerators (linacs) deliver their maximum dose a few centimetres below the treatment or phantom surface. This skin-sparing effect is degraded by the generation of secondary electrons as the x-ray beam passes to the patient or phantom. This work measures the characteristics of these electrons. A light-weight electromagnet was constructed that could be mounted in the block-tray position, 58 cm from the x-ray source of a Varian Clinac 2100C or 2500 linac. A field strength as high as 0.1500 T was generated, which was strong enough to sweep secondary electrons out of a 10 cm x 10 cm field. For 6, 10 and 24 MV x-ray beams, secondary contamination electrons produced 18, 38 and 65% of the surface dose, corresponding to 3, 5 and 12% of the maximum dose, respectively. A parameterized depth-dose curve for the contamination electrons was produced and was valid for all the x-ray energies studied.

Biophysical Phenomena↗
PubMed1994

Evaluation and quality control of a commercial 3-D dose compensator system.

A commercially available software/hardware system for automated design and fabrication of three-dimensional dose compensator molds has been tested for accuracy and precision as well as for its ability to provide adequate dose compensation at depth. To date, we have used this system to treat more than 50 patients with either head and neck or lung malignancies. In 19 head and neck patients (38 compensators) the use of a customized compensator resulted in an average reduction of dose variance in the target volume from 13.8% (range of 7%-21%) with uncompensated parallel-opposed fields to 4.5% (2%-7%) with custom-compensated parallel-opposed fields. A similar reduction was seen in the dose variation across lung tumor volumes. The custom compensators were also tested for accuracy of fabrication and positioning; both were found to be accurate within +/- 1 mm of the design specifications for all compensators tested. Last, the dosimetric properties of the compensators were studied. The ratios of measured open-beam dose profiles to measured compensated-beam dose profiles were compared with the ratio of similar profiles calculated with a treatment planning system. These ratios were equal within +/- 2.9%, thus providing evidence of the fidelity of the compensator to its design and the accuracy of the treatment planning algorithm that designs 34 each compensator.

Algorithms↗
PubMed1994

Implementation of a three-dimensional compensation system based on computed tomography generated surface contours and tissue inhomogeneities.

A computed tomography (CT) based system that compensates for patient surface contour and internal tissue inhomogeneity was implemented in our clinic. The compensators are fabricated with a mixture of tin granules and bee's wax. The tin/wax mixture was optimized for tin granule size and tin granule to wax ratio. The narrow beam attenuation coefficients were measured for 4-, 6-, 10-, and 24-MV photon beams. The compensator design and fabrication methodology were verified by measuring the dose distribution for a known surface contour irradiated with a compensated beam and for a known inhomogeneity that was submerged in a water phantom and irradiated with a compensated beam. For the surface contour, the uncompensated isodose levels varied by as much as 10% in the compensation plane and the compensator restored the isodose level to a variation of less than 1.3%. Measured and calculated doses for this surface contour were found to differ by less than 3.4%. For the inhomogeneity, the uncompensated isodose levels varied by 27% in the compensation plane and the compensator restored the isodose level to a variation of less than 1.5%. Measured and calculated doses for the known inhomogeneity were found to differ by less than 2%. Measurements of depth-dose curves indicate that the presence of the compensator in the beam does not significantly increase the surface dose. Twenty-six compensators have now been fabricated for clinical cases. In these patients, dose variations as great as 19% occurred in the plane of compensation prior to placing the compensator in the beam.(ABSTRACT TRUNCATED AT 250 WORDS)

Animals↗
PubMed1993

The relationship between the capacity to evolve oxygen and the variable fluorescence of chlorophyll after microsecond illumination in Chlorella, pea leaves and pea thylakoids.

The relationship between the capacity to evolve oxygen following a flash of a few microseconds duration and the variable fluorescence of chlorophyll was determined in Chlorella, leaf disks of peas, and thylakoids of pea leaves. It was found that this relationship is linear in intact plant material, while it is nonlinear in thylakoids. However, in thylakoids, the recovery of the capacity to evolve oxygen does not track the decay of the variable yield of Chl a fluorescence. This nonlinear relationship in thylakoids results from a reduced rate in the oxygen evolution reaction with no change in the decay of the variable yield of Chl a fluorescence. From a new application of the matrix analysis method to oxygen flash yields, the S1'-->S2, S2'-->S3 and S3'-->S4-->S0 transitions are found to be slowed or delayed in pea thylakoids and this underlies the slower rate of the recovery of the capacity to evolve oxygen in thylakoids. It is concluded that in intact cells the QA-QB(-)-->QA QB- reaction was rate-limiting for the recovery of the capacity to evolve oxygen, the equal energy-transfer hypothesis and the sequential double-hit model are valid in pea leaves and that the apparent invalidity in thylakoids is actually due to slowing of reaction steps in the oxygen evolution mechanism.

Chlorella↗
PubMed1992

Oxygen yield and thermoluminescence characteristics of a cyanobacterium lacking the manganese-stabilizing protein of photosystem II.

Previous experiments have shown that a Synechocystis sp. PCC 6803 mutant (delta psbO) lacking the extrinsic manganese-stabilizing protein (MSP) exhibits impaired, but significant levels of H2O-splitting activity [Burnap, R., & Sherman, L.A. (1991) Biochemistry 30, 440-446]. [14C]DCMU-binding experiments now show that the number and affinity of DCMU-binding sites (normalized to chlorophyll) are equivalent in delta psbO and the wild type, suggesting equal concentrations of assembled reaction centers. A similar conclusion is reached on the basis of measurements of PSII electron transport (DPC-supported DCPIP reduction) by mutant and wild-type thylakoids. The pattern of flash O2 yield by delta psbO cells measured with a bare platinum electrode exhibits a period four oscillation (with a maximum on the third flash), indicating that the H2O-splitting enzyme in delta psbO retains the basic mechanistic features found in normal cells. However, the amplitude of these signals is smaller and more highly damped than those obtained from wild-type cells, suggesting the absence of MSP results in a higher miss probability and/or a reduction in the number of centers competent in oxygen evolution. Analysis of the rise kinetics of the ampermeric signal on the bare platinum electrode indicates that the S3-[S4]-S0 transition is retarded by at least a factor of 5 in the mutant. Thermoluminescence emission peak temperatures indicate that the S2QA-, S2QB-, and S3QB-charge pairs are significantly more stable with respect to recombination in the mutant. The intensities of the thermoluminescence emissions are also significantly reduced in the mutant.(ABSTRACT TRUNCATED AT 250 WORDS)

Binding Sites↗
PubMed1990

Growth under Red Light Enhances Photosystem II Relative to Photosystem I and Phycobilisomes in the Red Alga Porphyridium cruentum.

Acclimation of the photosynthetic apparatus to light absorbed primarily by photosystem I (PSI) or by photosystem II (PSII) was studied in the unicellular red alga Porphyridium cruentum (ATCC 50161). Cultures grown under green light of 15 microeinsteins per square meter per second (PSII light; absorbed predominantly by the phycobilisomes) exhibited a PSII/PSI ratio of 0.26 +/- 0.05. Under red light (PSI light; absorbed primarily by chlorophyll) of comparable quantum flux, cells contained nearly five times as many PSII per PSI (1.21 +/- 0.10), and three times as many PSII per cell. About 12% of the chlorophyll was attributed to PSII in green light, 22% in white light, and 39% in red light-grown cultures. Chlorophyll antenna sizes appeared to remain constant at about 75 chlorophyll per PSII and 140 per PSI. Spectral quality had little effect on cell content or composition of the phycobilisomes, thus the number of PSII per phycobilisome was substantially greater in red light-grown cultures (4.2 +/- 0.6) than in those grown under green (1.6 +/- 0.3) or white light (2.9 +/- 0.1). Total photosystems (PSI + PSII) per phycobilisome remained at about eight in each case. Carotenoid content and composition was little affected by the spectral composition of the growth light. Zeaxanthin comprised more than 50% (mole/mole), beta-carotene about 40%, and cryptoxanthin about 4% of the carotenoid pigment. Despite marked changes in the light-harvesting apparatus, red and green light-grown cultures have generation times equal to that of cultures grown under white light of only one-third the quantum flux.

Journal Article↗
PubMed1989

Stoichiometry of Photosystem I, Photosystem II, and Phycobilisomes in the Red Alga Porphyridium cruentum as a Function of Growth Irradiance.

Cells of the red alga Porphyridium cruentum (ATCC 50161) exposed to increasing growth irradiance exhibited up to a three-fold reduction in photosystems I and II (PSI and PSII) and phycobilisomes but little change in the relative numbers of these components. Batch cultures of P. cruentum were grown under four photon flux densities of continuous white light; 6 (low light, LL), 35 (medium light, ML), 180 (high light, HL), and 280 (very high light, VHL) microeinsteins per square meter per second and sampled in the exponential phase of growth. Ratios of PSII to PSI ranged between 0.43 and 0.54. About three PSII centers per phycobilisome were found, regardless of growth irradiance. The phycoerythrin content of phycobilisomes decreased by about 25% for HL and VHL compared to LL and ML cultures. The unit sizes of PSI (chlorophyll/P(700)) and PSII (chlorophyll/Q(A)) decreased by about 20% with increase in photon flux density from 6 to 280 microeinsteins per square meter per second. A threefold reduction in cell content of chlorophyll at the higher photon flux densities was accompanied by a twofold reduction in beta-carotene, and a drastic reduction in thylakoid membrane area. Cell content of zeaxanthin, the major carotenoid in P. cruentum, did not vary with growth irradiance, suggesting a role other than light-harvesting. HL cultures had a growth rate twice that of ML, eight times that of LL, and slightly greater than that of VHL cultures. Cell volume increased threefold from LL to VHL, but volume of the single chloroplast did not change. From this study it is evident that a relatively fixed stoichiometry of PSI, PSII, and phycobilisomes is maintained in the photosynthetic apparatus of this red alga over a wide range of growth irradiance.

Journal Article↗
PubMed1988

Determination of the Rate Limiting Step for Photosynthesis in a Nearly Isonuclear Rapeseed (Brassica napus L.) Biotype Resistant to Atrazine.

Plant biotypes that are resistant to S-triazines under most conditions often grow less vigorously and have lower quantum yields and lower maximum rates of photosynthesis. The photosynthetic reactions responsible for these effects were identified in whole leaves and thylakoids of nearly isonuclear lines of oilseed rape (Brassica napus L.). The lower quantum yield was a result of poor efficiency in the use of separated charge at the photosystem II reaction center. Charge separation occurred normally, but over 30% of the charges recombined instead of being used for oxygen evolution and for reduction capacity in photosystem I. The lower maximum rate of photosynthesis in the resistant biotype was set by the transfer of electrons between the primary, Q(A), and secondary, Q(B), acceptors of photosystem II. This charge transfer reaction became rate limiting in resistant biotypes. The decreased quantum yield and decreased maximum rate of photosynthesis are both believed to be consequences of changes in the 32 kilodalton herbicide binding protein. As such, it is likely that these traits will not be genetically separable.

Journal Article↗