Plotting of Mannual Issodose line in different Cancer cases in Radiotherapy treatment plan and it is compared with Varian Eclipse Treatment Planning System.
Comparision done in 2019 at Tata Memorial Hospital, Parel, Mumbai.
Isodose curves depict absorbed dose distributions and variations in volume and planes. They join points of equal dose. Isodose charts show the variation in dose as a function of depth and transverse distance from the central beam axis. Factors like beam energy, field size, and distance affect isodose curve shape through penumbra and dose deposition. Multiple beams are often needed to adequately treat tumors while sparing surrounding tissues. Beam arrangements, weights, and modifiers must be optimized for each plan.
This document discusses the principles and utility of 3D conformal radiation therapy (3DCRT). It begins by explaining the goals of radiotherapy to maximize dose to the tumor while minimizing dose to normal tissues. It then describes some disadvantages of conventional 2D planning, including lack of 3D visualization and irradiation of large normal tissue volumes. The document goes on to define 3DCRT as radiotherapy that closely conforms the high dose volume to the target while sparing critical tissues. It discusses the history and development of 3DCRT and provides details on target volume definition, treatment planning workflow including imaging, contouring, planning and evaluation.
1) The document discusses measurement of dose distribution in external beam radiation therapy, including beam profiles, isodose curves, and percentage depth dose.
2) Beam profiles measure dose variation across a radiation beam, while isodose curves connect points of equal absorbed dose.
3) Several parameters can affect dose distribution, including beam quality, field size, and distance from the source. Proper measurement and modeling of dose distribution is important for treatment planning.
Dosimetric Evaluation of High Energy Electron Beams Applied in RadiotherapyAYMAN G. STOHY
Electron-beam therapy: is used to treat superficial tumors at a standard 100 cm source-to-surface distance (SSD). Characteristics of electron beams from an Elekta PreciseTM linear accelerator are presented at a nominal SSD of 100 cm. However, certain clinical situations require the use of an extended SSD. The effects of extended source-to-surface distance (SSD) on the electron beam dose profiles were evaluated for various electron beam energies 6, 8, 10,12 and 15 MeV and the accuracy of various output correction methods was analyzed on an Elekta PreciseTM linear accelerator using a radiation field analyzer (RFA). Effective SSDs was evaluated for field sizes ranging from 6×6, 10×10, 14×14 and 20×20 cm2 for various energies.
Aim of the work
1.Investigate the physical properties of electron beams
at different beam energies.
2.Evaluate the accuracy of dose calculated by
Treatment Planning System (TPS) and measured for
different field configurations.
TISSUE PHANTOM RATIO - THE PHOTON BEAM QUALITY INDEXVictor Ekpo
TPR(20,10) is the recommended photon beam quality index by IAEA TRS-398 for megavoltage clinical photons generated by linear accelerators. This presentation goes through the basics of Tissue Phantom Ratio (TPR).
This document discusses central axis depth doses in water for both SSD and SAD techniques. For SSD technique:
- Percentage depth dose (PDD) curves measure attenuation at different depths and are affected by beam quality, field size, and SSD.
- Buildup region occurs as secondary electrons deposit energy downstream, increasing dose with depth until maximum.
- Depth dose maximum (zmax) depends on beam energy and field size.
- PDD increases with larger field sizes due to increased scatter radiation.
- PDD increases with longer SSD due to the inverse square law of radiation intensity.
Total skin electron therapy (TSET) is used to treat cutaneous T-cell lymphoma by delivering a uniform dose of radiation to the entire skin surface while sparing underlying organs. It requires large electron fields over the entire body and precise dosimetry. The most common technique uses six electron beams arranged at 60 degree intervals to provide circumferential coverage. Proper field design and calibration are needed to achieve uniform dose across irregular body surfaces and minimize dose from bremsstrahlung x-rays.
Isodose curves depict absorbed dose distributions and variations in volume and planes. They join points of equal dose. Isodose charts show the variation in dose as a function of depth and transverse distance from the central beam axis. Factors like beam energy, field size, and distance affect isodose curve shape through penumbra and dose deposition. Multiple beams are often needed to adequately treat tumors while sparing surrounding tissues. Beam arrangements, weights, and modifiers must be optimized for each plan.
This document discusses the principles and utility of 3D conformal radiation therapy (3DCRT). It begins by explaining the goals of radiotherapy to maximize dose to the tumor while minimizing dose to normal tissues. It then describes some disadvantages of conventional 2D planning, including lack of 3D visualization and irradiation of large normal tissue volumes. The document goes on to define 3DCRT as radiotherapy that closely conforms the high dose volume to the target while sparing critical tissues. It discusses the history and development of 3DCRT and provides details on target volume definition, treatment planning workflow including imaging, contouring, planning and evaluation.
1) The document discusses measurement of dose distribution in external beam radiation therapy, including beam profiles, isodose curves, and percentage depth dose.
2) Beam profiles measure dose variation across a radiation beam, while isodose curves connect points of equal absorbed dose.
3) Several parameters can affect dose distribution, including beam quality, field size, and distance from the source. Proper measurement and modeling of dose distribution is important for treatment planning.
Dosimetric Evaluation of High Energy Electron Beams Applied in RadiotherapyAYMAN G. STOHY
Electron-beam therapy: is used to treat superficial tumors at a standard 100 cm source-to-surface distance (SSD). Characteristics of electron beams from an Elekta PreciseTM linear accelerator are presented at a nominal SSD of 100 cm. However, certain clinical situations require the use of an extended SSD. The effects of extended source-to-surface distance (SSD) on the electron beam dose profiles were evaluated for various electron beam energies 6, 8, 10,12 and 15 MeV and the accuracy of various output correction methods was analyzed on an Elekta PreciseTM linear accelerator using a radiation field analyzer (RFA). Effective SSDs was evaluated for field sizes ranging from 6×6, 10×10, 14×14 and 20×20 cm2 for various energies.
Aim of the work
1.Investigate the physical properties of electron beams
at different beam energies.
2.Evaluate the accuracy of dose calculated by
Treatment Planning System (TPS) and measured for
different field configurations.
TISSUE PHANTOM RATIO - THE PHOTON BEAM QUALITY INDEXVictor Ekpo
TPR(20,10) is the recommended photon beam quality index by IAEA TRS-398 for megavoltage clinical photons generated by linear accelerators. This presentation goes through the basics of Tissue Phantom Ratio (TPR).
This document discusses central axis depth doses in water for both SSD and SAD techniques. For SSD technique:
- Percentage depth dose (PDD) curves measure attenuation at different depths and are affected by beam quality, field size, and SSD.
- Buildup region occurs as secondary electrons deposit energy downstream, increasing dose with depth until maximum.
- Depth dose maximum (zmax) depends on beam energy and field size.
- PDD increases with larger field sizes due to increased scatter radiation.
- PDD increases with longer SSD due to the inverse square law of radiation intensity.
Total skin electron therapy (TSET) is used to treat cutaneous T-cell lymphoma by delivering a uniform dose of radiation to the entire skin surface while sparing underlying organs. It requires large electron fields over the entire body and precise dosimetry. The most common technique uses six electron beams arranged at 60 degree intervals to provide circumferential coverage. Proper field design and calibration are needed to achieve uniform dose across irregular body surfaces and minimize dose from bremsstrahlung x-rays.
The document discusses the concepts of biological effective dose (BED) and equivalent dose in 2 Gy fractions (EQD2). BED represents the total dose required to achieve a specific biological effect based on the dose per fraction and overall treatment time. EQD2 provides a more practical dose value for clinical use by converting BED to an equivalent total dose given in 2 Gy fractions. The document provides examples of calculating BED and EQD2 for different fractionation schedules and discusses applications in isoeffective dose comparisons and interpreting clinical trial results.
This document discusses the clinical implementation of volumetric modulated arc therapy (VMAT) at UT M.D. Anderson Cancer Center. It provides an overview of VMAT, the advantages it offers over other radiation therapy techniques, and the steps taken to configure the accelerator, treatment planning system, and quality assurance processes for VMAT delivery. Key aspects covered include accelerator prerequisites, TPS commissioning, patient-specific quality assurance using films and ion chambers, monthly constancy checks, and tips for rapid arc treatment planning for prostate cases.
Quality assurance of treatment planning system by Rahim GoharRahim Gohar
The document discusses quality assurance of 3D treatment planning systems for external photon and electron beams. It covers international reports on QA of TPS from organizations like IAEA, AAPM Task Group 53, and CAPCA. The presentation reviews aspects of TPS QA like system/software configuration, data entry, and evolution over time. It provides examples of important quality control checks for components like the CPU, digitizer, backups, CT transfer, and validating basic beam data. Tolerances for dose calculation accuracy are also addressed.
This document discusses various time-dose models used in radiotherapy, including the Strandqvist, Cohen, NSD, and TDF models. It explains the need for these models to optimize treatment regimes for tumor control while sparing normal tissues. The document also covers gap correction factors used when treatment schedules are interrupted and the various factors that can affect tumor control outcomes due to gaps in treatment. Compensatory methods like accelerated scheduling and increased dosing are presented to account for treatment gaps.
Motion management strategies in radiation therapy aim to account for tumor movement during treatment. Key strategies include gating methods that deliver radiation only during specific respiratory phases, breath hold methods that immobilize tumors during deep inhalation or exhalation, tracking methods that follow tumor motion in real-time and adjust beam targeting accordingly, and encompassing methods that define larger target volumes to cover full respiratory excursion. No single approach is clearly superior, as appropriate management depends on tumor location, motion extent, and available technology. The goal of all motion management is to safely escalate dose to tumors while reducing dose to surrounding healthy tissues.
Electron beam radiotherapy uses megavoltage electron beams ranging from 6-20 MeV to treat superficial tumors within 6 cm of the skin surface. It provides a uniform dose at a specified depth with rapid dose fall-off, sparing deeper tissues. Common tumors treated include skin, lymphomas, and breast cancer. Electrons deposit dose via interactions like collision and scattering. Dose distribution is characterized by a rapid buildup to a maximum within 1 cm followed by a rapid falloff beyond the treatment depth.
Stereotactic body radiotherapy (SBRT) delivers high-dose radiation to tumors in a small number of fractions using high precision. For prostate SBRT, the target and organs at risk are contoured on planning CT. A dose of 35-38Gy in 5 fractions is used as primary treatment for low risk prostate cancer. Rigid image guidance and intrafraction monitoring are important to minimize setup errors. ExacTrac X-ray positioning co-registers X-rays with digitally reconstructed radiographs and corrects for rotational and translational deviations, achieving sub-millimeter accuracy. This allows safe dose escalation for prostate SBRT.
1. A multileaf collimator (MLC) is a device used in radiation therapy to shape radiation beams by blocking parts of the beam with independently moving leaf structures made of a dense material like tungsten.
2. MLCs allow for more precise shaping of radiation beams than traditional collimators to minimize dose to healthy tissues and conform dose to the tumor shape. They enable intensity-modulated radiation therapy (IMRT) through dynamic movement of their leaves during treatment delivery.
3. MLC leaf positioning accuracy and transmission properties must be verified through quality assurance procedures to ensure proper dose delivery, such as measurements of leaf transmission, leaf position accuracy, and dosimetric leaf gaps.
Total body irradiation (TBI) delivers a uniform dose of radiation to the entire body and is used as a conditioning regimen prior to bone marrow transplantation. It aims to suppress the immune system and eliminate cancer. Commissioning TBI requires absolute dose calibration and measurement of beam profiles, percentage depth doses, and tissue-maximum ratios under extended source-to-surface distances. Dosimetric challenges include non-uniformity of dose across the body and unreliable dose measurements from detectors under TBI conditions. AAPM Report 17 provides recommendations for TBI dosimetry including using a water phantom and measuring central axis data under full scattering conditions.
1.Aim of Radiotherapy
The goal of radiotherapy is to deliver a prescribed dose of radiation to the Target while sparing surrounding Healthy tissues to the largest extent possible
2.Organ Motion
Intra-fraction motion
during the fraction
Heartbeat
Swallowing
Coughing
Eye movement
Inter-fraction motion
- in between the fractions
Tumour change
Weight gain/loss
Positioning deviation
Breathing
Bowel and rectal filling
Bladder filling
Muscle relaxation/tension
3. Respiratory motion affects:
Respiratory motion affects all tumour sites in the thorax, abdomen and Pelvis. Tumours in the Lung, Liver, Pancreas, Oesophagus, Breast, Kidneys, prostate
Tumour displacement varies depending on the site and organ Location
Lung tumours can move several cm in any direction during irradiation
It is most prevalent and prominent in Lung cancers
4. Problems associated with respiratory motion during RT
Image acquisition limitations
Treatment planning limitations
Radiation delivery limitations
5. Methods to Account for Respiratory Motion
1. Motion encompassing methods
2. Respiratory gating methods
3. Breath hold methods
4. Forced shallow breathing with abdominal compression
5. Real-time tumor tracking methods
Summary:
The management of respiratory motion in radiation oncology is an evolving field
IGRT provides a solution for combating organ motion in radiotherapy
Delivering higher dose to tumor and less dose to normal tissue.
Limited clinical studies, needs to be studied further
IGRT – the future of radiotherapy
This document provides information about total body irradiation (TBI). It discusses that TBI uses megavoltage photon beams to destroy the recipient's bone marrow and tumor cells prior to bone marrow transplantation. It is used to treat various diseases like leukemia, lymphoma, and multiple myeloma. TBI can be delivered at high or low doses, to half the body, or total nodes. Techniques include parallel opposed beams from linear accelerators or cobalt-60 machines. Dosimetry and in vivo dosimetry are important due to the large fields and difficulty achieving uniform dose. Complications can include sterility, secondary cancers, and growth issues.
Isodose lines represent points of equal absorbed radiation dose on a dose distribution map. They are depicted as curves on isodose charts showing the volumetric and planar variations in absorbed dose. Factors influencing isodose curves include beam quality, field size, source-to-skin distance, beam modifiers like wedges or bolus, and depth. Isodose curves are used in radiation therapy treatment planning to evaluate dose distributions and ensure tumor coverage while sparing surrounding healthy tissues. They provide critical information about the radiation dose profile essential for safe and effective treatment.
This document discusses Intra-cavitary Brachytherapy (ICBT) for treating cervical cancer. It describes different historical ICBT systems like Paris, Stockholm, and Manchester systems. It also discusses modern techniques like remote afterloaders and recommendations for reporting absorbed doses and volumes in ICBT. Key points include different dose rates (LDR, MDR, HDR), advantages of remote afterloaders in maintaining geometry and dose distribution, and recommending specifying absorbed dose to the target volume rather than at a single point for ICBT.
This document discusses various methods used to evaluate radiotherapy treatment plans, including physical and biological parameters. Physically, plans are evaluated using isodose curves, dose distribution statistics, differential and cumulative dose-volume histograms (DVHs). Target coverage should be within 95-100% of the prescribed dose. Biologically, tumor control probability (TCP) and normal tissue complication probability (NTCP) models are used. The therapeutic ratio and index compare the dose required for tumor control versus normal tissue complications. NTCP models include Lyman-Kutcher-Burman and critical element/volume models. Plan evaluation ensures target doses are adequate while respecting organ tolerance doses.
The document summarizes interstitial brachytherapy, including indications, contraindications, isotopes used, and details of various planning systems like Paterson-Parker, Quimby, Paris, and computer-based systems. It discusses dose rates, types of implants, applicators, volume definition, and dosimetry parameters like reference isodose and uniformity criteria for different planning approaches.
This document discusses radiotherapy and CT simulation procedures. It begins with an introduction to radiotherapy and how it uses radiation to destroy cancer cells. It then describes the linear accelerator machine commonly used to deliver targeted radiation treatments. Finally, it outlines the mould room procedure for creating customized thermoplastic masks to immobilize patients, ensuring accurate radiation delivery to the treatment site.
The document discusses the use of Tomotherapy for radiation treatment planning and delivery. It provides examples of how Tomotherapy allows for:
1) Highly conformal radiation plans that sculpt dose around complex tumor target shapes while minimizing dose to nearby organs.
2) Daily image guidance that enables adjustment of targets to account for changes in patient anatomy and tumor size during treatment.
3) Delivery of simultaneous integrated boosts to multiple tumor sites.
CT simulators are essential for precise radiotherapy treatment planning. They use CT scanning to create a virtual 3D representation of the patient's anatomy. This allows clinicians to accurately localize tumors and delineate organs at risk. The CT images provide excellent soft tissue contrast and electron density data needed for treatment planning. Patients are immobilized using custom devices to ensure consistent positioning. Reference marks are placed to align the patient for treatment. Various protocols can be used depending on the disease site and anatomy. Contrast may also be used to differentiate tumors from healthy tissue. The high quality images from CT simulation enable optimized, precise radiotherapy plans.
Electron beam therapy uses electrically charged particles called electrons that are generated by a linear accelerator to treat superficial cancers. It deposits dose uniformly from the surface to a specific depth before rapidly falling off, sparing deeper tissues. Electron energies up to 20 MeV can treat disease within 6 cm of the surface. Accessories like applicators, cutouts, bolus and internal shields are used to shape the beam for treatment fields and protect healthy tissues. Precise dose specification and reporting is important for electron therapy due to the rapid dose fall-off and higher skin doses compared to prescription depth.
Brachytherapy techniques have evolved over time from early historical systems like the Paris and Stockholm systems to more modern techniques. The document discusses the key aspects of different brachytherapy systems including: the Paris system which used small amounts of radium over 5 days, the Stockholm system which used repeated high dose radium treatments over shorter times, and the Manchester system which modified the Paris system and introduced standardized dose measurement points like Point A. Modern brachytherapy planning incorporates 3D imaging, contouring of tumor and organ-at-risk volumes, and advanced dose reporting metrics to better optimize treatment while sparing healthy tissues.
Verification of a treatment planning system using an in-house designedtrunk p...IOSR Journals
This document summarizes a study that verified the dosimetric performance of a treatment planning system (TPS) using an in-house designed trunk phantom. The phantom was constructed with hollows containing various tissue-equivalent materials and scanned with CT to generate images for the TPS. Beams were planned and measured using the linear accelerator. Measurements from the in-house phantom were within 3.39% of TPS calculations. Comparisons to a solid water phantom also showed deviations within 3%. The results demonstrate the TPS algorithm compensates accurately for inhomogeneities irrespective of field size.
The document discusses the concepts of biological effective dose (BED) and equivalent dose in 2 Gy fractions (EQD2). BED represents the total dose required to achieve a specific biological effect based on the dose per fraction and overall treatment time. EQD2 provides a more practical dose value for clinical use by converting BED to an equivalent total dose given in 2 Gy fractions. The document provides examples of calculating BED and EQD2 for different fractionation schedules and discusses applications in isoeffective dose comparisons and interpreting clinical trial results.
This document discusses the clinical implementation of volumetric modulated arc therapy (VMAT) at UT M.D. Anderson Cancer Center. It provides an overview of VMAT, the advantages it offers over other radiation therapy techniques, and the steps taken to configure the accelerator, treatment planning system, and quality assurance processes for VMAT delivery. Key aspects covered include accelerator prerequisites, TPS commissioning, patient-specific quality assurance using films and ion chambers, monthly constancy checks, and tips for rapid arc treatment planning for prostate cases.
Quality assurance of treatment planning system by Rahim GoharRahim Gohar
The document discusses quality assurance of 3D treatment planning systems for external photon and electron beams. It covers international reports on QA of TPS from organizations like IAEA, AAPM Task Group 53, and CAPCA. The presentation reviews aspects of TPS QA like system/software configuration, data entry, and evolution over time. It provides examples of important quality control checks for components like the CPU, digitizer, backups, CT transfer, and validating basic beam data. Tolerances for dose calculation accuracy are also addressed.
This document discusses various time-dose models used in radiotherapy, including the Strandqvist, Cohen, NSD, and TDF models. It explains the need for these models to optimize treatment regimes for tumor control while sparing normal tissues. The document also covers gap correction factors used when treatment schedules are interrupted and the various factors that can affect tumor control outcomes due to gaps in treatment. Compensatory methods like accelerated scheduling and increased dosing are presented to account for treatment gaps.
Motion management strategies in radiation therapy aim to account for tumor movement during treatment. Key strategies include gating methods that deliver radiation only during specific respiratory phases, breath hold methods that immobilize tumors during deep inhalation or exhalation, tracking methods that follow tumor motion in real-time and adjust beam targeting accordingly, and encompassing methods that define larger target volumes to cover full respiratory excursion. No single approach is clearly superior, as appropriate management depends on tumor location, motion extent, and available technology. The goal of all motion management is to safely escalate dose to tumors while reducing dose to surrounding healthy tissues.
Electron beam radiotherapy uses megavoltage electron beams ranging from 6-20 MeV to treat superficial tumors within 6 cm of the skin surface. It provides a uniform dose at a specified depth with rapid dose fall-off, sparing deeper tissues. Common tumors treated include skin, lymphomas, and breast cancer. Electrons deposit dose via interactions like collision and scattering. Dose distribution is characterized by a rapid buildup to a maximum within 1 cm followed by a rapid falloff beyond the treatment depth.
Stereotactic body radiotherapy (SBRT) delivers high-dose radiation to tumors in a small number of fractions using high precision. For prostate SBRT, the target and organs at risk are contoured on planning CT. A dose of 35-38Gy in 5 fractions is used as primary treatment for low risk prostate cancer. Rigid image guidance and intrafraction monitoring are important to minimize setup errors. ExacTrac X-ray positioning co-registers X-rays with digitally reconstructed radiographs and corrects for rotational and translational deviations, achieving sub-millimeter accuracy. This allows safe dose escalation for prostate SBRT.
1. A multileaf collimator (MLC) is a device used in radiation therapy to shape radiation beams by blocking parts of the beam with independently moving leaf structures made of a dense material like tungsten.
2. MLCs allow for more precise shaping of radiation beams than traditional collimators to minimize dose to healthy tissues and conform dose to the tumor shape. They enable intensity-modulated radiation therapy (IMRT) through dynamic movement of their leaves during treatment delivery.
3. MLC leaf positioning accuracy and transmission properties must be verified through quality assurance procedures to ensure proper dose delivery, such as measurements of leaf transmission, leaf position accuracy, and dosimetric leaf gaps.
Total body irradiation (TBI) delivers a uniform dose of radiation to the entire body and is used as a conditioning regimen prior to bone marrow transplantation. It aims to suppress the immune system and eliminate cancer. Commissioning TBI requires absolute dose calibration and measurement of beam profiles, percentage depth doses, and tissue-maximum ratios under extended source-to-surface distances. Dosimetric challenges include non-uniformity of dose across the body and unreliable dose measurements from detectors under TBI conditions. AAPM Report 17 provides recommendations for TBI dosimetry including using a water phantom and measuring central axis data under full scattering conditions.
1.Aim of Radiotherapy
The goal of radiotherapy is to deliver a prescribed dose of radiation to the Target while sparing surrounding Healthy tissues to the largest extent possible
2.Organ Motion
Intra-fraction motion
during the fraction
Heartbeat
Swallowing
Coughing
Eye movement
Inter-fraction motion
- in between the fractions
Tumour change
Weight gain/loss
Positioning deviation
Breathing
Bowel and rectal filling
Bladder filling
Muscle relaxation/tension
3. Respiratory motion affects:
Respiratory motion affects all tumour sites in the thorax, abdomen and Pelvis. Tumours in the Lung, Liver, Pancreas, Oesophagus, Breast, Kidneys, prostate
Tumour displacement varies depending on the site and organ Location
Lung tumours can move several cm in any direction during irradiation
It is most prevalent and prominent in Lung cancers
4. Problems associated with respiratory motion during RT
Image acquisition limitations
Treatment planning limitations
Radiation delivery limitations
5. Methods to Account for Respiratory Motion
1. Motion encompassing methods
2. Respiratory gating methods
3. Breath hold methods
4. Forced shallow breathing with abdominal compression
5. Real-time tumor tracking methods
Summary:
The management of respiratory motion in radiation oncology is an evolving field
IGRT provides a solution for combating organ motion in radiotherapy
Delivering higher dose to tumor and less dose to normal tissue.
Limited clinical studies, needs to be studied further
IGRT – the future of radiotherapy
This document provides information about total body irradiation (TBI). It discusses that TBI uses megavoltage photon beams to destroy the recipient's bone marrow and tumor cells prior to bone marrow transplantation. It is used to treat various diseases like leukemia, lymphoma, and multiple myeloma. TBI can be delivered at high or low doses, to half the body, or total nodes. Techniques include parallel opposed beams from linear accelerators or cobalt-60 machines. Dosimetry and in vivo dosimetry are important due to the large fields and difficulty achieving uniform dose. Complications can include sterility, secondary cancers, and growth issues.
Isodose lines represent points of equal absorbed radiation dose on a dose distribution map. They are depicted as curves on isodose charts showing the volumetric and planar variations in absorbed dose. Factors influencing isodose curves include beam quality, field size, source-to-skin distance, beam modifiers like wedges or bolus, and depth. Isodose curves are used in radiation therapy treatment planning to evaluate dose distributions and ensure tumor coverage while sparing surrounding healthy tissues. They provide critical information about the radiation dose profile essential for safe and effective treatment.
This document discusses Intra-cavitary Brachytherapy (ICBT) for treating cervical cancer. It describes different historical ICBT systems like Paris, Stockholm, and Manchester systems. It also discusses modern techniques like remote afterloaders and recommendations for reporting absorbed doses and volumes in ICBT. Key points include different dose rates (LDR, MDR, HDR), advantages of remote afterloaders in maintaining geometry and dose distribution, and recommending specifying absorbed dose to the target volume rather than at a single point for ICBT.
This document discusses various methods used to evaluate radiotherapy treatment plans, including physical and biological parameters. Physically, plans are evaluated using isodose curves, dose distribution statistics, differential and cumulative dose-volume histograms (DVHs). Target coverage should be within 95-100% of the prescribed dose. Biologically, tumor control probability (TCP) and normal tissue complication probability (NTCP) models are used. The therapeutic ratio and index compare the dose required for tumor control versus normal tissue complications. NTCP models include Lyman-Kutcher-Burman and critical element/volume models. Plan evaluation ensures target doses are adequate while respecting organ tolerance doses.
The document summarizes interstitial brachytherapy, including indications, contraindications, isotopes used, and details of various planning systems like Paterson-Parker, Quimby, Paris, and computer-based systems. It discusses dose rates, types of implants, applicators, volume definition, and dosimetry parameters like reference isodose and uniformity criteria for different planning approaches.
This document discusses radiotherapy and CT simulation procedures. It begins with an introduction to radiotherapy and how it uses radiation to destroy cancer cells. It then describes the linear accelerator machine commonly used to deliver targeted radiation treatments. Finally, it outlines the mould room procedure for creating customized thermoplastic masks to immobilize patients, ensuring accurate radiation delivery to the treatment site.
The document discusses the use of Tomotherapy for radiation treatment planning and delivery. It provides examples of how Tomotherapy allows for:
1) Highly conformal radiation plans that sculpt dose around complex tumor target shapes while minimizing dose to nearby organs.
2) Daily image guidance that enables adjustment of targets to account for changes in patient anatomy and tumor size during treatment.
3) Delivery of simultaneous integrated boosts to multiple tumor sites.
CT simulators are essential for precise radiotherapy treatment planning. They use CT scanning to create a virtual 3D representation of the patient's anatomy. This allows clinicians to accurately localize tumors and delineate organs at risk. The CT images provide excellent soft tissue contrast and electron density data needed for treatment planning. Patients are immobilized using custom devices to ensure consistent positioning. Reference marks are placed to align the patient for treatment. Various protocols can be used depending on the disease site and anatomy. Contrast may also be used to differentiate tumors from healthy tissue. The high quality images from CT simulation enable optimized, precise radiotherapy plans.
Electron beam therapy uses electrically charged particles called electrons that are generated by a linear accelerator to treat superficial cancers. It deposits dose uniformly from the surface to a specific depth before rapidly falling off, sparing deeper tissues. Electron energies up to 20 MeV can treat disease within 6 cm of the surface. Accessories like applicators, cutouts, bolus and internal shields are used to shape the beam for treatment fields and protect healthy tissues. Precise dose specification and reporting is important for electron therapy due to the rapid dose fall-off and higher skin doses compared to prescription depth.
Brachytherapy techniques have evolved over time from early historical systems like the Paris and Stockholm systems to more modern techniques. The document discusses the key aspects of different brachytherapy systems including: the Paris system which used small amounts of radium over 5 days, the Stockholm system which used repeated high dose radium treatments over shorter times, and the Manchester system which modified the Paris system and introduced standardized dose measurement points like Point A. Modern brachytherapy planning incorporates 3D imaging, contouring of tumor and organ-at-risk volumes, and advanced dose reporting metrics to better optimize treatment while sparing healthy tissues.
Verification of a treatment planning system using an in-house designedtrunk p...IOSR Journals
This document summarizes a study that verified the dosimetric performance of a treatment planning system (TPS) using an in-house designed trunk phantom. The phantom was constructed with hollows containing various tissue-equivalent materials and scanned with CT to generate images for the TPS. Beams were planned and measured using the linear accelerator. Measurements from the in-house phantom were within 3.39% of TPS calculations. Comparisons to a solid water phantom also showed deviations within 3%. The results demonstrate the TPS algorithm compensates accurately for inhomogeneities irrespective of field size.
Total body irradiation (TBI) is a form of radiotherapy used prior to bone marrow transplants to reduce the risk of transplant rejection and destroy any remaining cancer cells. TBI techniques use large photon fields, usually from cobalt-60 machines or LINACs, to irradiate the entire body. Common techniques include opposing anterior-posterior beams or lateral beams. Precise dosimetry is required due to the large fields and total body exposure, with dose uniformity targets of within ±10% across the body. In vivo dosimetry using TLD or diodes is also employed to verify accurate dose delivery. Early side effects from TBI include fatigue, nausea, hair loss and skin irritation due to the whole body irradiation
Beam direction techniques are used to accurately direct radiation beams towards the tumor while sparing surrounding healthy tissues. Key steps include patient localization using imaging like CT/MRI to delineate the tumor and organs, patient positioning and immobilization, field selection using beam directing devices like lasers, collimators and pointers, and dose distribution analysis to calculate and verify the prescribed dose. Proper beam direction allows obtaining conformal dose distributions and reproducible treatments for better therapeutic outcomes.
1) CT dose index (CTDI) measures radiation output of CT scanners. Modern measures include CTDI100, CTDIvol, and dose length product (DLP).
2) Automatic exposure control (AEC) modulates tube current based on patient attenuation to maintain consistent image quality while reducing dose.
3) Dose reduction techniques in CT include AEC, bowtie filters, iterative reconstruction, prospective gating, and dynamic collimation.
This document provides an overview of different brachytherapy systems that have been developed over time for delivering radiation internally or close to the surface of the body. It describes several early systems from the 1930s-1960s including the Paterson-Parker system, Quimby system, Paris system, and Manchester system. It also covers the Stockholm, Paris, and Manchester methods for intracavitary cervical cancer treatment. Later sections discuss the Paris system improvements, computer planning systems, and the current International Commission on Radiation Units and Measurements reporting system.
Beam directed radiotherapy aims to deliver a homogenous tumor dose while minimizing radiation to normal tissues. It involves careful patient positioning, immobilization, tumor localization, field selection, dose calculations, and verification. Key steps include using positioning aids and molds to reproducibly position the patient, imaging such as CT to delineate the tumor volume, contouring to define external body outlines, and dose calculations and verification to ensure accurate delivery.
QUALITY ASSURANCE IN LINAC AND CYBERKNIFE.pptxSuryaSuganthan2
This document discusses quality assurance procedures for a linear accelerator (linac) and CyberKnife system. It outlines the various QA tools used, including phantoms for checking beam parameters like flatness, symmetry and output. Daily, weekly, monthly and yearly QA tests are described for parameters like lasers, optical distance indicator and radiation output. Tolerance levels are provided. Procedures for specific tests using tools like the Pentaguide and SunNuclear profiler are detailed step-by-step. Results of sample daily output and beam profile measurements are also shown.
8. normal distribution qt pgdm 1st semesterKaran Kukreja
The document discusses the normal distribution and its key properties. It explains that the normal distribution is a limiting case of the binomial distribution when the number of trials is large. It has a bell-shaped symmetrical curve centered around the mean. The normal distribution is uniquely defined by its mean and standard deviation. The document also covers how to convert between a normal distribution and the standard normal distribution and how to find probabilities using the standard normal distribution table.
This document discusses various techniques for arc therapy including tomotherapy, intensity modulated arc therapy (IMAT), and volumetric modulated arc therapy (VMAT). It provides details on:
- The history and basic concept of arc therapy which involves continuous radiation delivery from a rotating source.
- Techniques like tomotherapy which uses fan beams and helical delivery, and IMAT/VMAT which modulates dose rate and leaf speed during single or multiple full gantry rotations.
- The planning process for these techniques including inverse planning with direct aperture optimization to determine optimal leaf positions and weights to achieve conformal dose distributions while satisfying delivery constraints.
The document describes a study that used the MCNP5 Monte Carlo code to determine dosimetric quantities surrounding a 103Pd radioactive stent, according to AAPM TG-60 recommendations. The stent was modeled as a hollow cylinder coated with 103Pd. MCNP5 was used to calculate the dose deposited per photon, relative dose, anisotropy function F(r,h), and radial dose function gL(r) at various distances from the stent surface. The relative dose values calculated by MCNP5 agreed well with values from TG-43 and previous EGS4 simulations, with errors of less than 3%. The dosimetric parameters determined can be used in future treatment planning for intravascular brachytherapy.
Hofer ct teaching manual - a systematic approach to ct reading, 2nd ed.Michel Phuong
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This document provides information about computed tomography (CT) scans and factors that affect radiation dose, including:
1. Helical pitch affects dose, with lower pitches increasing dose and higher pitches decreasing dose. Tube current and time also affect dose linearly, with higher mAs increasing dose.
2. Effective radiation dose from CT scans is much higher than conventional x-rays but still less than typical background radiation exposure per year. Automatic exposure control helps reduce dose by modulating tube current based on patient attenuation.
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PERFORMANCE EVALUATION OF COMPUTED TOMOGRAPHY (CT) SCANNERSBhuvi palaniswamy
This document discusses performance evaluation tests for computed tomography (CT) scanners. It can be broadly classified into electromechanical tests, x-ray generator (electrical) tests, image quality tests, radiation dose tests, and general tests related to CT number. Electromechanical tests evaluate the scan localization laser lights, table movement accuracy, and gantry tilt. X-ray generator tests check the accelerating voltage, milliampere linearity, and radiation output reproducibility. Image quality tests evaluate low-contrast resolution, high-contrast resolution, and noise. Radiation dose tests measure the computed tomography dose index and multiple scan average dose using phantoms.
The document discusses a computational and experimental study on the effect of cross position and angle on hemodynamic performance within crossed stent grafts used in endovascular aneurysm repair (EVAR). Two series of idealized bifurcated stent grafts were modeled with varying cross angles (30-90 degrees) and positions (cross position ratios of 0.48-1.92). Computational fluid dynamics simulations and in vitro experiments were conducted. Results showed that absolute helicity at outlets decreased with increased cross angle and increased with decreased cross position. Oscillating shear index and relative resident time, which may indicate thrombosis risk, decreased slightly with increased cross angle and decreased cross position. Both simulations and experiments indicated that displacement force on the stent graft
This document discusses a study examining the hemodynamic performance of crossed stent grafts used to treat abdominal aortic aneurysms. Computational fluid dynamics simulations and experiments were conducted using idealized bifurcated stent graft models with varying cross angles and positions. The results showed that absolute helicity at outlets decreased with increased cross angles and increased cross positions. Oscillating shear index and relative resident time, which are risk factors for thrombosis, decreased slightly with increased cross angles and decreased cross positions. Both simulations and experiments indicated that displacement forces on the stent graft increased with larger cross angles and lower cross positions. The optimal configuration was found to be a small cross angle and high cross position, but low cross positions increase the risk of migration.
THE USE OF ADAPTIVE STATISTICAL ITERATIVE RECONSTRUCTION (ASIR) ON IMAGE QUAL...AM Publications
Use of Adaptive Statistical Iterative Reconstruction (ASIR) on CT scan of thorax has been investigated. This study aims is to determine the effect of the use of ASIR on the radiation dose and image quality. The study was conducted using phantom anthropomorphic using CT Scan GE Optima 580 with setting ASIR Dose Reduction 0% - 50%. This study was carried out by using two parameters: fixed tube current and Tube Current Modulation (TCM). Analyzing of radiation dose is done by calculation of CTDIvol. While image quality are investigated by calculated Signal to Noise Ratio (SNR) and Contrast to Noise Ratio (CNR). There is a difference in the CTDIvol value, between the fixed tube current and TCM settings. At fixed tube current strength, the CTDIvol value is measured, starting from 0% to 50% ASIR, respectively: 48.60 mGy; 43.74 mGy; 38.88 mGy; 34.02 mGy; 29.16 mGy; and 24.30 mGy. While the CTDIvol value measured in TCM settings uses 0% to 50% ASIR as follows: 21.92 mGy; 20.09 mGy; 18.33 mGy; 16.51 mGy; 14.59 mGy; and 12.75 mGy. Using ASIR with TCM can produce CTDIvol values that are smaller than ASIR with fixed tube current. The difference in the average CTDIvol value is 51.80% between the use of TCM and fixed tube current. The greater the percentage of ASIR regulated, the greater the decrease in the CTDIvol dose. There is no significant difference in the SNR and CNR values produced by 0% to 50% ASIR with a fixed current strength. There is no significant difference in the SNR and CNR values produced by ASIR 0% to 50% with TCM. The average CNR value shown in TCM is higher than that of fixed tube current. The use of ASIR influence in dose radiation decreases without change the image quality.
Speckle tracking echocardiography (STE) is an echocardiographic imaging technique that analyzes the motion of tissues in the heart by using the naturally occurring speckle pattern in the myocardium or blood when imaged by ultrasound.
Dose delivered from varian's cbct to patients receiving imrt for prostate cancerlanying
1. This study measured the dose from daily cone beam CT (CBCT) scans used for image-guided radiation therapy in prostate cancer patients receiving intensity-modulated radiation therapy (IMRT).
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Cold Sores: Causes, Treatments, and Prevention Strategies | The Lifesciences ...The Lifesciences Magazine
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Empowering ACOs: Leveraging Quality Management Tools for MIPS and BeyondHealth Catalyst
Join us as we delve into the crucial realm of quality reporting for MSSP (Medicare Shared Savings Program) Accountable Care Organizations (ACOs).
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LGBTQ+ Adults: Unique Opportunities and Inclusive Approaches to CareVITASAuthor
This webinar helps clinicians understand the unique healthcare needs of the LGBTQ+ community, primarily in relation to end-of-life care. Topics include social and cultural background and challenges, healthcare disparities, advanced care planning, and strategies for reaching the community and improving quality of care.
Rate Controlled Drug Delivery Systems, Activation Modulated Drug Delivery Systems, Mechanically activated, pH activated, Enzyme activated, Osmotic activated Drug Delivery Systems, Feedback regulated Drug Delivery Systems systems are discussed here.
Letter to MREC - application to conduct studyAzreen Aj
Application to conduct study on research title 'Awareness and knowledge of oral cancer and precancer among dental outpatient in Klinik Pergigian Merlimau, Melaka'
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Neurological system includes brain and spinal cord. It plays an important role in functioning of our body. Encephalitis is the inflammation of the brain. Causes include viral infections, infections from insect bites or an autoimmune reaction that affects the brain. It can be life-threatening or cause long-term complications. Treatment varies, but most people require hospitalization so they can receive intensive treatment, including life support.
Michigan HealthTech Market Map 2024. Includes 7 categories: Policy Makers, Academic Innovation Centers, Digital Health Providers, Healthcare Providers, Payers / Insurance, Device Companies, Life Science Companies, Innovation Accelerators. Developed by the Michigan-Israel Business Accelerator
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6. Isodose shift method
Used for Manually correction
of Isodose lines.
Along each grid lines(1 cm),
Isodose line is shifted by an
amount:
k x h
7. h (tissue deficit or tissue excess) & “k” a factor
less than 1 and is given in the following Table:
Isodose position along the grid are joined after
correction.
11. Gf
t
t
where
Gf
Gf
t
t
t
F
factor
Shift
2
..
..
2
)
(
_ '
'
FS=10x10cm2 ,SSD(f)=100cm
and for depth=7cm G=0.068
then
Shift factor:
71
.
0
100
068
.
0
2
100
068
.
0
2
Gf
Gf
F
Simillarly, corresponding values for
5x5cm2 and 20x20cm2 is 0.74 and
0.68.
(Giessen PH.A method of calculating the isodose shift in correcting for oblique incidence in radiotherapy.Br J
Radiol. 1973;46:978.)
12. • K = f(gap,radiation energy,SSD,field area and depth in absorbing medium)
• When gap(t) is small compared to SSD , then k is independent of gap.
• Example:If SSD is 50cm then k is not independent of gap
• But it is dependent on other factors.
• For depths below about 7cm, the factor is sensibly constant.
• It is shown that a single value of the factor may be used for all fields and
depths(for given radiation energy and SSD) with an error up to 1% to 2%.
(Giessen PH.A method of calculating the isodose shift in correcting for oblique incidence in radiotherapy.Br
J Radiol. 1973;46:978.)
13. Effective SSD method
It include correction of PDD with the help of ISF.
Here isodose lines are shift by an amount h (tissue deficit or
tissue excess)
14. Here h is tissue deficit
As we are interested to find PDD at
point A as shown in the figure.
15. Tissue-air ratio method
Correction of PDD done with help of TAR/TMR
actual
corrected PDD
CF
PDD *
)
(
)
(
h
d
TMR
d
TMR
CF
,Here d and h are in cm.
17. Isodose shift method
Used for Manually correction of Isodose lines.
Proposed by Greene, Steward and Sundblom.
Shift are done by amount equal to n(emperically obtained
value) times the thickness of inhomogeniety.
It is measured along the line parallel to the central axis and
passing to the point of interest.
The shift is away from skin for lung and air cavity and
opposite in case of bone.
18.
19. Small bulges are due to inoization chamber of
0.6 mm diameter fixed at position R.
Measured with air filled hole where the isodose
curve moved distally by 0.6 times the thickness
of air gap.
(Greene D, Stewart Jr. Isodose curves in non_uniform Phantoms.Br J Radiol.1965;38:378.)
20. Measured with cork
(simulating Lung density )
where the isodose curve
moved distally by 0.4 times the
thickness of cork/ Lung.
(Greene D, Stewart Jr. Isodose curves in non_uniform Phantoms.Br J Radiol.1965;38:378.)
21. • The value of n is given by the following table:
• It is seen that the factor depends on the properties of material of different
densities and independent of field size.
• Error percentage is about 2% when the above emperical rules is compared
with measured Isodose lines .
22. Other correction factors
• Tissue_Air Ratio Method.
• Power Law Tissue_Air Ratio Method.
• Equivalent Tissue_Air Ratio Method.
25. • First take a contour of a patient CT
image with possible accuracy on a
Butterpaper.
• Take Standard Isodose Chart
• Place Contoured Butterpaper over
isodose chart
26. • Adjust the isodose line chart with the surface of body
contour.
• Draw isodose line coressponding to chart for
number of fields required.
• Apply correction factor whenever required.
69. Treatment time calculation
• Fraction size=725cGy
• Field size=8 X 8cm2
FIELD EFS
(cm2)
DEPTH
(cm)
PDD (%) OUTPUT
(cGy/min)
TT(min)
AP 8 10 54.8 55.18 5.99
PA 8 12 47.2 55.18 6.96
RL 8 18 30.2 55.18 10.87
LL 8 18 30.2 55.18 10.87
70. Time required for physicist
Procedure Time(Approx)
Four Fields(Grid) 4Hr
71. Conclusion
• Time consuming.
• Grid method shifts towards more accuracy.
• Grid method gives max dose recieving by OAR along
with PTV coverage.
72. References
• KHAN'S(The physics of radiation therapy) by Faiz M. Khan and John
P.Gibbons-5th Edition published by Wolters Kluwer(2014).
• Giessen PH.A method of calculating the isodose shift in correcting for
oblique incidence in radiotherapy.Br J Radiol. 1973;46:978.
• Greene D, Stewart Jr. Isodose curves in non_uniform Phantoms.Br J
Radiol.1965;38:378.