1. Electron irradiation of sapphire (Al2O3) results in both electronic and nuclear damage.
2. Electronic damage includes electron excitation and ionization via interactions between the incident 1 MeV electrons and the aluminum and oxygen atoms in Al2O3.
3. Nuclear damage, or displacement damage, occurs when electrons transfer sufficient energy to atomic nuclei to displace them from their lattice sites, calculated using models of electron-atom cross sections and displacement thresholds.
The document discusses various units used to measure radiation. It begins by explaining that ionizing radiation removes electrons from atoms, causing ionization. It then discusses the early unit of exposure (SED), before introducing the roentgen (R) as the unit adopted in 1928. The roentgen measures ionization in air. Exposure is defined as charge per unit mass. Relationships between the SI unit of coulomb/kg and the roentgen are provided. Different types of ionization chambers used to measure exposure, such as free air chambers and thimble chambers, are described. Limitations of the roentgen are noted. Various units used to measure radiation energy, exposure, dose, and dose equivalents are defined.
Cyclotrons accelerate charged particles using oscillating electric fields generated between hollow metal chambers called dees. A positive ion is placed between the dees and accelerated toward the first dee when it is negatively charged. It follows a semicircular path due to a strong magnetic field until the dee polarities are reversed, accelerating it toward the second dee and to higher energies with each pass through the oscillating field. Cyclotrons can be used to accelerate ion beams for nuclear physics experiments and cancer treatment through proton therapy.
This document discusses various radiation quantities and units used to characterize ionizing radiation. It describes key concepts such as activity, kerma, exposure, absorbed dose, equivalent dose, effective dose, annual limit intake (ALI), and derived air concentration (DAC). The International Commission on Radiation Protection (ICRP) and International Commission on Radiation Units (ICRU) help define these quantities and their relationships. Primary quantities like equivalent dose relate radiation risk, while operational quantities like exposure are used for measurements. Tissue weighting factors account for different tissue sensitivities in calculating effective dose from equivalent dose.
A betatron is a device that accelerates electrons using an expanding magnetic field within a doughnut-shaped vacuum chamber. Electrons are injected into the chamber and accelerated as the magnetic field strength increases over time. This increasing magnetic flux induces an electric field that increases the electrons' energy, allowing them to gain extremely high speeds. The betatron condition requires that the rate of change of magnetic flux through the circular orbit equals 2π times the radius squared times the rate of change of the magnetic field, in order to maintain the electrons' constant orbital radius as they accelerate.
INTERACTION OF IONIZING RADIATION WITH MATTERVinay Desai
The document discusses the interaction of ionizing radiation with matter. It describes the main interaction processes including photoelectric effect, Compton scattering, and pair production. For radiation therapy, Compton scattering is the most important interaction as it allows high energy beams to penetrate tissue more uniformly depositing dose. The photoelectric effect is more significant for diagnostic radiology due to its dependence on atomic number.
Measurement of Radiation (Thimble Ionization Chamber, Free air Ionization Cha...Upakar Paudel
The document discusses different methods for measuring ionizing radiation, including early methods based on chemical or biological effects and later adoption of the roentgen unit based on ionization in air. It focuses on the free-air ionization chamber, which measures exposure (roentgens) by collecting ions produced in a known mass of air. Limitations led to the development of thimble chambers, which mimic free-air chambers using solid, air-equivalent walls of appropriate thickness to achieve electronic equilibrium within the chamber.
This document discusses various radiation units used to quantify radiation exposure and its effects. It defines units of radioactivity like curie and becquerel, exposure units like roentgen, absorbed dose units like rad and gray, and equivalent and effective dose units like rem and sievert used to account for radiation type and organ sensitivity. It also discusses concepts like attenuation, kerma, absorbed dose, and weighting factors used to calculate equivalent and effective doses from radiation exposure.
Charged particle interaction with matterSabari Kumar
This document discusses charged particle interactions with matter. It begins by outlining the topics to be covered, including interactions of heavy charged particles like protons, electrons, and light ions. It then explains that charged particle interactions are mediated by Coulomb forces and may involve ionization or excitation of orbital electrons or interactions with atomic nuclei. Different types of interactions like elastic and inelastic collisions are described. Equations for energy loss by heavy charged particles during collisions are shown. The interactions of protons, electrons, neutrons, and light and heavy ions are then discussed in more detail.
The document discusses various units used to measure radiation. It begins by explaining that ionizing radiation removes electrons from atoms, causing ionization. It then discusses the early unit of exposure (SED), before introducing the roentgen (R) as the unit adopted in 1928. The roentgen measures ionization in air. Exposure is defined as charge per unit mass. Relationships between the SI unit of coulomb/kg and the roentgen are provided. Different types of ionization chambers used to measure exposure, such as free air chambers and thimble chambers, are described. Limitations of the roentgen are noted. Various units used to measure radiation energy, exposure, dose, and dose equivalents are defined.
Cyclotrons accelerate charged particles using oscillating electric fields generated between hollow metal chambers called dees. A positive ion is placed between the dees and accelerated toward the first dee when it is negatively charged. It follows a semicircular path due to a strong magnetic field until the dee polarities are reversed, accelerating it toward the second dee and to higher energies with each pass through the oscillating field. Cyclotrons can be used to accelerate ion beams for nuclear physics experiments and cancer treatment through proton therapy.
This document discusses various radiation quantities and units used to characterize ionizing radiation. It describes key concepts such as activity, kerma, exposure, absorbed dose, equivalent dose, effective dose, annual limit intake (ALI), and derived air concentration (DAC). The International Commission on Radiation Protection (ICRP) and International Commission on Radiation Units (ICRU) help define these quantities and their relationships. Primary quantities like equivalent dose relate radiation risk, while operational quantities like exposure are used for measurements. Tissue weighting factors account for different tissue sensitivities in calculating effective dose from equivalent dose.
A betatron is a device that accelerates electrons using an expanding magnetic field within a doughnut-shaped vacuum chamber. Electrons are injected into the chamber and accelerated as the magnetic field strength increases over time. This increasing magnetic flux induces an electric field that increases the electrons' energy, allowing them to gain extremely high speeds. The betatron condition requires that the rate of change of magnetic flux through the circular orbit equals 2π times the radius squared times the rate of change of the magnetic field, in order to maintain the electrons' constant orbital radius as they accelerate.
INTERACTION OF IONIZING RADIATION WITH MATTERVinay Desai
The document discusses the interaction of ionizing radiation with matter. It describes the main interaction processes including photoelectric effect, Compton scattering, and pair production. For radiation therapy, Compton scattering is the most important interaction as it allows high energy beams to penetrate tissue more uniformly depositing dose. The photoelectric effect is more significant for diagnostic radiology due to its dependence on atomic number.
Measurement of Radiation (Thimble Ionization Chamber, Free air Ionization Cha...Upakar Paudel
The document discusses different methods for measuring ionizing radiation, including early methods based on chemical or biological effects and later adoption of the roentgen unit based on ionization in air. It focuses on the free-air ionization chamber, which measures exposure (roentgens) by collecting ions produced in a known mass of air. Limitations led to the development of thimble chambers, which mimic free-air chambers using solid, air-equivalent walls of appropriate thickness to achieve electronic equilibrium within the chamber.
This document discusses various radiation units used to quantify radiation exposure and its effects. It defines units of radioactivity like curie and becquerel, exposure units like roentgen, absorbed dose units like rad and gray, and equivalent and effective dose units like rem and sievert used to account for radiation type and organ sensitivity. It also discusses concepts like attenuation, kerma, absorbed dose, and weighting factors used to calculate equivalent and effective doses from radiation exposure.
Charged particle interaction with matterSabari Kumar
This document discusses charged particle interactions with matter. It begins by outlining the topics to be covered, including interactions of heavy charged particles like protons, electrons, and light ions. It then explains that charged particle interactions are mediated by Coulomb forces and may involve ionization or excitation of orbital electrons or interactions with atomic nuclei. Different types of interactions like elastic and inelastic collisions are described. Equations for energy loss by heavy charged particles during collisions are shown. The interactions of protons, electrons, neutrons, and light and heavy ions are then discussed in more detail.
This presentation discusses calorimetry dosimetry, which measures energy imparted to matter through temperature change. It can provide the most precise absolute dose measurements. Thermocouples and thermistors are commonly used temperature sensors. Thermistors are preferable due to their greater sensitivity. Different materials have different thermal capacities that determine the temperature increase per unit of absorbed dose. Energy fluence calorimeters contain a stopping material core to measure radiation beam energy, and calculate fluence based on temperature increase and material properties. Calorimetry provides advantages at high dose rates where other dosimeters saturate.
This document summarizes the ionization chamber thimble type. It explains that a thimble ionization chamber has a central electrode surrounded by an outer electrode. When a high voltage is applied, air between the electrodes is ionized and electrons are emitted. The electrons move toward the positive electrode, inducing a current. The current is proportional to radiation dose absorbed by the air volume. Thimble chambers are cylindrical with volumes of 0.1-1 cm3, radii of 2-7 mm, and lengths of 4-25 mm. They are commonly used to calibrate megavoltage photon beams and have advantages of accuracy and precision but require high voltage supply and corrections for high energies.
This document discusses scintillation detectors and their properties. Scintillation detectors work by emitting light when exposed to radiation, and this light output can be used to measure incident radiation. The key properties of scintillation detectors are that they must have high scintillation efficiency, light yield proportional to deposited energy, short decay time, transparency to emitted wavelengths, and be able to be made in large sizes and desired shapes. Common inorganic scintillators discussed are NaI(Tl), which is widely used due to its availability and high detection efficiency, and BGO, which has high intrinsic efficiency for high gamma energies.
Radiation units can be divided into units of radioactivity and units of radiation dose. The curie and becquerel are units of radioactivity, with 1 curie equal to 3.7x1010 decays per second. Exposure dose is measured in roentgens or C/kg, while absorbed dose is measured in rads or grays. Equivalent dose accounts for radiation type and takes the Q factor into account, measured in rems or sieverts. Effective dose considers radiation exposure to different tissues, calculated from equivalent dose and tissue weighting factors.
Treatment Planning Ii Patient Data, Corrections, And Set Upfondas vakalis
The document discusses treatment planning for radiation therapy patients. It covers acquiring accurate patient data through CT, MRI, and ultrasound scans. It also discusses corrections that must be made for tissue inhomogeneities, contour irregularities, and patient positioning. Various methods are described for correcting for the effects of bone, lung tissue, air cavities, and other inhomogeneities on radiation dose distribution.
This document discusses radiation protection and safety criteria related to ionizing radiation. It begins by defining radiation hazards and outlining the biological effects of radiation exposure, which can be either deterministic or probabilistic. Key aspects of radiation protection covered include determining radiation hazards, evaluating radiation doses, and the principles and recommendations established by the International Commission on Radiological Protection. The document then provides examples of calculating radiation intensity and shielding requirements for various radiation sources and energies. It emphasizes protecting workers and the public through principles of time, distance and shielding, and highlights planning considerations for medical x-ray facilities to ensure safe and compliant operation.
The document discusses various types of ionizing radiation and their interactions with matter. It describes electromagnetic radiation as composed of photons that can interact via photoelectric effect, Compton scattering, pair production, and other processes. Compton scattering results in energy transfer between photons and recoil electrons. The probability of interaction depends on photon energy and material properties like atomic number. Higher energy photons have a greater chance of depositing energy through secondary electrons.
interaction of ionizing radiation
1) Interaction of photon with matter
2) Interaction of Electron and proton with matter
3)Interaction of Neutron with matter
This document discusses the concept of relative biological effectiveness (RBE), which compares the biological effects of different types of ionizing radiation. It defines RBE as the ratio of doses of radiation (such as x-rays versus neutrons) required to produce the same biological effect. Higher RBE values indicate radiation that causes greater biological damage. The document explains that RBE depends on factors like radiation dose, number of fractions, and biological endpoint. It also discusses how RBE varies with linear energy transfer (LET), being highest around 100 keV/μm, and how RBE and oxygen enhancement ratio are inversely related and peak around the same LET value.
The document discusses beam quality, half value layer (HVL), and filters used in radiation beams. It defines HVL as the thickness of an absorber required to attenuate the beam intensity to half its original value. Beam quality and HVL are influenced by factors like energy, thickness, and density. Different types of filters are used such as inherent, added, combination, and flattening filters to modify the beam spectrum by removing low energy photons through beam hardening. The quality of megavoltage beams is specified by peak energy rather than HVL since they are heavily filtered.
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.
Dr. Vijay P Raturi presented on radiation dosimetry methods. The key points are:
1. Thermoluminescent dosimeters (TLD) like LiF:Mg,Ti are commonly used for personnel radiation monitoring and measure absorbed dose by emitting light when heated that is proportional to radiation exposure.
2. TLDs have advantages over film badges including a wider measurable dose range, smaller size allowing point measurements, and reusability. However, TLDs can lack uniformity and have storage instability issues.
3. Geiger-Müller counters are also used to detect ionizing radiation by measuring radiation induced ionization in a gas-filled tube. They are useful for radiation
1) The document discusses the interaction of radiation with matter, including the different types of radiation and their properties. It describes electromagnetic radiation and the electromagnetic spectrum.
2) The main interactions that occur between radiation and matter are photoelectric effect, Compton scattering, and pair production. The photoelectric effect involves the ejection of an electron from an atom when a photon transfers all its energy. Compton scattering is the scattering of photons by loosely bound electrons, resulting in energy transfer. Pair production occurs when a photon converts into an electron-positron pair in the vicinity of a nucleus.
3) The dominant interaction depends on the photon energy - photoelectric effect dominates at low energies, Compton scattering in the soft
Occupational radiation safety in Radiotherapy, Timothy Peace Sohscmcvellore
This document discusses occupational radiation safety in radiotherapy. It outlines potential radiation hazards from teletherapy equipment like telecobalt units and linear accelerators, as well as brachytherapy sources. Case studies of accidents are presented to illustrate hazards that can occur from equipment malfunctions, improper safety procedures, and lack of regulatory oversight. The document recommends strict adherence to safety guidelines and regulatory standards to minimize risks and ensure occupational exposures are kept as low as reasonably achievable. Regular equipment maintenance, staff training, and quality assurance are emphasized.
Proton therapy is able to more precisely target radiation dose to tumor tissues while minimizing dose to surrounding healthy tissues. Photon therapy deposits radiation throughout the tissues it passes through, whereas proton therapy deposits most of its energy at a specific depth called the Bragg peak. This allows protons to deliver a high radiation dose to the tumor with little exit dose, improving treatment of cancers near critical structures.
LiF:Mg,Ti (TLD-100) is a nearly tissue-equivalent thermoluminescent dosimeter material that is widely used for radiation dosimetry. It has good reproducibility and sensitivity for low doses. TLDs must be calibrated against absolute dosimeters. The TL response of TLD-100 depends on radiation quality and dose, and it exhibits fading over time. Computerized glow curve analysis can provide information on individual TL peaks. LiF:Mg,Cu,P has higher sensitivity and better tissue equivalence than TLD-100. CaF:Tm (TLD-300) can separate high and low LET radiation components based on peak heights. Various TLD materials are used for different applications
An x-ray machine produces x-rays through two processes when high-energy electrons hit a heavy metal target such as tungsten:
1) Bremsstrahlung occurs when the electrons are decelerated upon impact, producing a spectrum of photon wavelengths below the electrons' initial energy.
2) K-shell emission occurs when an electron is ejected from the target atom's inner shell, causing a higher-energy electron to fill the vacancy and emit a photon of a single wavelength unique to each element.
This document discusses different types of gas-filled and scintillation radiation detectors. It provides information on GM counters, proportional counters, scintillators, photomultiplier tubes, and thermoluminescent dosimeters. Key points include: how GM counters differ from proportional counters in their avalanche chain reactions; common scintillator materials like NaI(Tl) and BGO; how photomultiplier tubes convert light photons to electrical signals and amplify signals through dynode multiplication; and applications of different detector types in nuclear medicine imaging. The document is in a question-answer format where various concepts are explained in response to questions.
Radiation protection, also known as radiological protection, is defined by the International Atomic Energy Agency (IAEA) as "The protection of people from harmful effects of exposure to ionizing radiation, and the means for achieving this". Exposure can be from a source of radiation external to the human body or due to internal irradiation caused by the ingestion of radioactive contamination.
Ionizing radiation is widely used in industry and medicine, and can present a significant health hazard by causing microscopic damage to living tissue. There are two main categories of ionizing radiation health effects. At high exposures, it can cause "tissue" effects, also called "deterministic" effects due to the certainty of them happening, conventionally indicated by the unit gray and resulting in acute radiation syndrome. For low level exposures there can be statistically elevated risks of radiation-induced cancer, called "stochastic effects" due to the uncertainty of them happening, conventionally indicated by the unit sievert.
Fundamental to radiation protection is the avoidance or reduction of dose using the simple protective measures of time, distance and shielding. The duration of exposure should be limited to that necessary, the distance from the source of radiation should be maxi mised, and the source shielded wherever possible. To measure personal dose uptake in occupational or emergency exposure, for external radiation personal dosimeters are used, and for internal dose to due to ingestion of radioactive contamination, bioassay techniques are applied.
This presentation discusses calorimetry dosimetry, which measures energy imparted to matter through temperature change. It can provide the most precise absolute dose measurements. Thermocouples and thermistors are commonly used temperature sensors. Thermistors are preferable due to their greater sensitivity. Different materials have different thermal capacities that determine the temperature increase per unit of absorbed dose. Energy fluence calorimeters contain a stopping material core to measure radiation beam energy, and calculate fluence based on temperature increase and material properties. Calorimetry provides advantages at high dose rates where other dosimeters saturate.
This document summarizes the ionization chamber thimble type. It explains that a thimble ionization chamber has a central electrode surrounded by an outer electrode. When a high voltage is applied, air between the electrodes is ionized and electrons are emitted. The electrons move toward the positive electrode, inducing a current. The current is proportional to radiation dose absorbed by the air volume. Thimble chambers are cylindrical with volumes of 0.1-1 cm3, radii of 2-7 mm, and lengths of 4-25 mm. They are commonly used to calibrate megavoltage photon beams and have advantages of accuracy and precision but require high voltage supply and corrections for high energies.
This document discusses scintillation detectors and their properties. Scintillation detectors work by emitting light when exposed to radiation, and this light output can be used to measure incident radiation. The key properties of scintillation detectors are that they must have high scintillation efficiency, light yield proportional to deposited energy, short decay time, transparency to emitted wavelengths, and be able to be made in large sizes and desired shapes. Common inorganic scintillators discussed are NaI(Tl), which is widely used due to its availability and high detection efficiency, and BGO, which has high intrinsic efficiency for high gamma energies.
Radiation units can be divided into units of radioactivity and units of radiation dose. The curie and becquerel are units of radioactivity, with 1 curie equal to 3.7x1010 decays per second. Exposure dose is measured in roentgens or C/kg, while absorbed dose is measured in rads or grays. Equivalent dose accounts for radiation type and takes the Q factor into account, measured in rems or sieverts. Effective dose considers radiation exposure to different tissues, calculated from equivalent dose and tissue weighting factors.
Treatment Planning Ii Patient Data, Corrections, And Set Upfondas vakalis
The document discusses treatment planning for radiation therapy patients. It covers acquiring accurate patient data through CT, MRI, and ultrasound scans. It also discusses corrections that must be made for tissue inhomogeneities, contour irregularities, and patient positioning. Various methods are described for correcting for the effects of bone, lung tissue, air cavities, and other inhomogeneities on radiation dose distribution.
This document discusses radiation protection and safety criteria related to ionizing radiation. It begins by defining radiation hazards and outlining the biological effects of radiation exposure, which can be either deterministic or probabilistic. Key aspects of radiation protection covered include determining radiation hazards, evaluating radiation doses, and the principles and recommendations established by the International Commission on Radiological Protection. The document then provides examples of calculating radiation intensity and shielding requirements for various radiation sources and energies. It emphasizes protecting workers and the public through principles of time, distance and shielding, and highlights planning considerations for medical x-ray facilities to ensure safe and compliant operation.
The document discusses various types of ionizing radiation and their interactions with matter. It describes electromagnetic radiation as composed of photons that can interact via photoelectric effect, Compton scattering, pair production, and other processes. Compton scattering results in energy transfer between photons and recoil electrons. The probability of interaction depends on photon energy and material properties like atomic number. Higher energy photons have a greater chance of depositing energy through secondary electrons.
interaction of ionizing radiation
1) Interaction of photon with matter
2) Interaction of Electron and proton with matter
3)Interaction of Neutron with matter
This document discusses the concept of relative biological effectiveness (RBE), which compares the biological effects of different types of ionizing radiation. It defines RBE as the ratio of doses of radiation (such as x-rays versus neutrons) required to produce the same biological effect. Higher RBE values indicate radiation that causes greater biological damage. The document explains that RBE depends on factors like radiation dose, number of fractions, and biological endpoint. It also discusses how RBE varies with linear energy transfer (LET), being highest around 100 keV/μm, and how RBE and oxygen enhancement ratio are inversely related and peak around the same LET value.
The document discusses beam quality, half value layer (HVL), and filters used in radiation beams. It defines HVL as the thickness of an absorber required to attenuate the beam intensity to half its original value. Beam quality and HVL are influenced by factors like energy, thickness, and density. Different types of filters are used such as inherent, added, combination, and flattening filters to modify the beam spectrum by removing low energy photons through beam hardening. The quality of megavoltage beams is specified by peak energy rather than HVL since they are heavily filtered.
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.
Dr. Vijay P Raturi presented on radiation dosimetry methods. The key points are:
1. Thermoluminescent dosimeters (TLD) like LiF:Mg,Ti are commonly used for personnel radiation monitoring and measure absorbed dose by emitting light when heated that is proportional to radiation exposure.
2. TLDs have advantages over film badges including a wider measurable dose range, smaller size allowing point measurements, and reusability. However, TLDs can lack uniformity and have storage instability issues.
3. Geiger-Müller counters are also used to detect ionizing radiation by measuring radiation induced ionization in a gas-filled tube. They are useful for radiation
1) The document discusses the interaction of radiation with matter, including the different types of radiation and their properties. It describes electromagnetic radiation and the electromagnetic spectrum.
2) The main interactions that occur between radiation and matter are photoelectric effect, Compton scattering, and pair production. The photoelectric effect involves the ejection of an electron from an atom when a photon transfers all its energy. Compton scattering is the scattering of photons by loosely bound electrons, resulting in energy transfer. Pair production occurs when a photon converts into an electron-positron pair in the vicinity of a nucleus.
3) The dominant interaction depends on the photon energy - photoelectric effect dominates at low energies, Compton scattering in the soft
Occupational radiation safety in Radiotherapy, Timothy Peace Sohscmcvellore
This document discusses occupational radiation safety in radiotherapy. It outlines potential radiation hazards from teletherapy equipment like telecobalt units and linear accelerators, as well as brachytherapy sources. Case studies of accidents are presented to illustrate hazards that can occur from equipment malfunctions, improper safety procedures, and lack of regulatory oversight. The document recommends strict adherence to safety guidelines and regulatory standards to minimize risks and ensure occupational exposures are kept as low as reasonably achievable. Regular equipment maintenance, staff training, and quality assurance are emphasized.
Proton therapy is able to more precisely target radiation dose to tumor tissues while minimizing dose to surrounding healthy tissues. Photon therapy deposits radiation throughout the tissues it passes through, whereas proton therapy deposits most of its energy at a specific depth called the Bragg peak. This allows protons to deliver a high radiation dose to the tumor with little exit dose, improving treatment of cancers near critical structures.
LiF:Mg,Ti (TLD-100) is a nearly tissue-equivalent thermoluminescent dosimeter material that is widely used for radiation dosimetry. It has good reproducibility and sensitivity for low doses. TLDs must be calibrated against absolute dosimeters. The TL response of TLD-100 depends on radiation quality and dose, and it exhibits fading over time. Computerized glow curve analysis can provide information on individual TL peaks. LiF:Mg,Cu,P has higher sensitivity and better tissue equivalence than TLD-100. CaF:Tm (TLD-300) can separate high and low LET radiation components based on peak heights. Various TLD materials are used for different applications
An x-ray machine produces x-rays through two processes when high-energy electrons hit a heavy metal target such as tungsten:
1) Bremsstrahlung occurs when the electrons are decelerated upon impact, producing a spectrum of photon wavelengths below the electrons' initial energy.
2) K-shell emission occurs when an electron is ejected from the target atom's inner shell, causing a higher-energy electron to fill the vacancy and emit a photon of a single wavelength unique to each element.
This document discusses different types of gas-filled and scintillation radiation detectors. It provides information on GM counters, proportional counters, scintillators, photomultiplier tubes, and thermoluminescent dosimeters. Key points include: how GM counters differ from proportional counters in their avalanche chain reactions; common scintillator materials like NaI(Tl) and BGO; how photomultiplier tubes convert light photons to electrical signals and amplify signals through dynode multiplication; and applications of different detector types in nuclear medicine imaging. The document is in a question-answer format where various concepts are explained in response to questions.
Radiation protection, also known as radiological protection, is defined by the International Atomic Energy Agency (IAEA) as "The protection of people from harmful effects of exposure to ionizing radiation, and the means for achieving this". Exposure can be from a source of radiation external to the human body or due to internal irradiation caused by the ingestion of radioactive contamination.
Ionizing radiation is widely used in industry and medicine, and can present a significant health hazard by causing microscopic damage to living tissue. There are two main categories of ionizing radiation health effects. At high exposures, it can cause "tissue" effects, also called "deterministic" effects due to the certainty of them happening, conventionally indicated by the unit gray and resulting in acute radiation syndrome. For low level exposures there can be statistically elevated risks of radiation-induced cancer, called "stochastic effects" due to the uncertainty of them happening, conventionally indicated by the unit sievert.
Fundamental to radiation protection is the avoidance or reduction of dose using the simple protective measures of time, distance and shielding. The duration of exposure should be limited to that necessary, the distance from the source of radiation should be maxi mised, and the source shielded wherever possible. To measure personal dose uptake in occupational or emergency exposure, for external radiation personal dosimeters are used, and for internal dose to due to ingestion of radioactive contamination, bioassay techniques are applied.
Glazes Theory And Practice Bryant HudsonBryant Hudson
This document provides an overview of ceramic glazes, including their composition, ingredients, and firing processes. It discusses how glazes are made of glass that sticks to pottery, with silica as the main component and fluxes like sodium and calcium added to lower the melting point. It describes the common elements used in glazes like alkali metals, alkaline earth metals, aluminum, and transition metals which provide color. Specific glaze recipes from a firehouse studio are detailed. Health and safety considerations for glaze materials are also covered.
This document discusses the Al2O3-ZrO2 phase diagram through several figures and studies:
1) It presents experimental and calculated Al2O3-ZrO2 phase diagrams showing the different phases like tetragonal ZrO2, monoclinic ZrO2, and liquid present at different temperatures and compositions.
2) Studies found the eutectic composition to be around 42.5% ZrO2 with a eutectic temperature of around 1910°C.
3) One study using solar furnace and electron microprobe analysis examined 17 compositions between 0-100% ZrO2 and identified phase transitions between tetragonal, monoclinic,
This document discusses inclusion control for clean steel production. It defines inclusions as non-metallic compounds that form separate phases in steel. Strict inclusion control is important for producing quality steel products. Inclusions are assessed and controlled by examining their source, shape, composition and distribution. Common inclusions include oxides, sulfides, and carbides. Modification techniques aim to make inclusions less harmful by modifying their shape, composition and dispersion in the steel matrix. Calcium additions are often used to modify alumina and manganese sulfide inclusions. Proper inclusion control is important at all stages of steelmaking and processing to achieve clean steel.
This document discusses using Al2O3/water nanofluid as a coolant in a double-tube heat exchanger. Nanofluids are discussed as a promising new class of heat transfer fluids made by dispersing nanoparticles in conventional fluids to enhance thermal conductivity. Mathematical models are developed to analyze heat transfer and pressure drop characteristics of Al2O3/water nanofluids flowing as coolant in the heat exchanger. Results show that nanofluids can increase heat transfer coefficients and reduce wall temperatures, heat transfer area, and coolant flowrates required compared to using water alone. However, nanofluids also increase friction factors and pressure drops, especially at higher nanoparticle concentrations.
Dental ceramics include porcelain and are used for dental restorations. Porcelain is made from a glass matrix containing mineral phases and feldspars. It is used for dental crowns, veneers, dentures, and other prosthetics. Porcelain has good biocompatibility and esthetics but is brittle. Metal-ceramic restorations combine a metal substructure with porcelain for strength. All-ceramic restorations are made entirely of ceramic materials and provide superior esthetics but require more tooth reduction. Common all-ceramic systems include machinable blocks, castable ceramics, pressable ceramics, and infiltrated glass ceramics.
NATURAL CONVECTIVE HEAT TRANSFER BY Al2O3 &PbO NANOFLUIDSAlagappapandian M
In this presentation related about natural convective heat transfer incresed by using different nano particles. in this fluid is called nanofluids. Nanofluids improve the heat transfer rate of base fluid.
This document discusses carbon compounds and their chemical reactions. It outlines several types of organic compounds including hydrocarbons, alcohols, carboxylic acids, and esters. Hydrocarbons are further broken down into saturated and unsaturated types. Chemical reactions such as combustion, hydration, dehydration, halogenation, oxidation, and esterification are described along with examples like the production of ethanol through fermentation.
This document contains links to 10 different memioronline.com pages related to thin film research projects. The pages focus on characterization of thin film materials like tungsten, ZnO, and their properties when used in gas sensors and how deposition methods like spray coating and laser ablation can be used to dope or alter the structure of these thin films.
This document discusses Portland cement and the cement manufacturing process. It begins with an overview of what cement is and how it is used to make concrete. It then describes the industrial process for manufacturing cement, involving grinding raw materials like limestone and clay at high temperatures in a kiln to form clinker, which is then pulverized with gypsum to become Portland cement powder. The document also provides a brief history of cement development and explains how cement kilns can beneficially reuse solid and hazardous wastes as a source of energy and raw material replacement due to the kilns' high temperatures and long retention times.
Protection des métaux contre la corrosionCHTAOU Karim
Cette présentation présentent tout d’abord les principaux types de la corrosion et il présente une description détaillée des trois grandes méthodes, préventives et curatives, utilisées en anticorrosion.
effet de l'incorporation d'ajuvant minéraux sur les propriétés des ciments g...Noël Djobo
Volcanic ashes are raw materials with variable chemical and mineralogical compositions from one deposit to another. When combined with suitable alkali activators they can be converted to geopolymer cements at ambient temperature. In this study we investigate the possibility of use bauxite and calcined oyster shell powders as mineral additives to volcanic ashes in other to enhance the properties of the resulted geopolymers. Different methods of analyses such as Fourier Transform Infrared Spectroscopy, X- Ray Diffractometry and Scanning Electron Microscopy were used to assess the variations of setting time, linear shrinkage and 28 days compressive strength of geopolymer pastes. Also, chemical and mineralogical compositions of bauxite and calcined oyster shell were determined. It appeared that bauxite and calcined oyster shell are respectively sources of Al2O3 and CaO and can compensate the deficiency of these oxides in volcanic ashes. These mineral additives are weakly dissolved in alkaline medium due to their high crystalline phase content. Addition of about 20 % of bauxite or 10 % calcined oyster shell lead to the decreasing of the setting time respectively from 415 to 275 min (bauxite) and 195 min (calcined oyster shell). Addition of any percentage of these minerals lead to the decrease of linear shrinkage and 10 % of bauxite is enough to prevent efflorescence. The increasing of the 28 days compressive strength of the geopolymers synthesized is trivial up to 10 to 20% addition of bauxite and calcined oyster shell respectively. More than these percentages additives have deleterious effect on the compressive strength.
Présentation de la plate-forme d'éco-conception CORINEBrice Kosinski
Eurocopter, leader mondial de la filière hélicoptère, a pris l’initiative du projet CORINE pour réduire l’impact environnemental sur la chaîne d’approvisionnement de ses produits civils.
Planifié sur trois ans, CORINE a pour objectif de fournir aux PME un outil d’éco-conception collaboratif entre donneurs d’ordre et fournisseurs. Il permettra d’identifier et d’intégrer de nouveaux matériaux et procédés tout au long du cycle de vie de l’hélicoptère.
CORINE est un outil collaboratif d'éco-conception unique en son genre. Les points clés innovants de l’outil d’éco-conception :
- Interface collaborative entre donneurs d’ordre et fournisseurs permettant de faire des choix en matière d’éco-conception
- Outil simple d’utilisation pour sélectionner les matériaux et procédés améliorant la performance environnementale
- Outil conçu pour la filière aéronautique et adaptable à des secteurs similaires
This document discusses types of radiation, their interaction with matter, and radiation detectors. It covers the following types of radiation: photons (gamma rays and x-rays), neutrons, electrons, ions, protons, and alpha particles. It describes the processes of photoelectric effect, Compton scattering, and pair production for photon interaction, as well as scattering, capture and other interactions for neutrons. The document also discusses why radiation detection is important and gives examples of different types of radiation detectors like gas detectors, scintillation detectors, and semiconductor detectors.
The document discusses key concepts in quantum mechanics including:
1. Photons carry energy and momentum that depends on their frequency or wavelength. Electrons also behave as both particles and waves with an associated wavelength.
2. Heisenberg's uncertainty principle establishes that the more precisely one property of a particle is measured, the less precisely its complementary property can be known.
3. Atomic spectra are unique to each element and arise from electrons transitioning between discrete energy levels in atoms. The wavelength of emitted photons corresponds to energy differences between levels.
interaction of radiation with matter modified.pptxGeet501819
Heavy charged particles like protons, alpha particles, and heavy ions interact with matter through Coulombic interactions that can cause ionization or excitation of orbital electrons. The interaction depends on the mass of the incoming particle - heavy particles travel in straight paths while lighter electrons undergo large angle scattering. The momentum and energy transferred from an incoming heavy particle to orbital electrons is calculated based on the particle's impact parameter and velocity. This transferred energy causes the heavy particle to lose energy as it passes through matter. The stopping power, or energy lost per unit length, can be determined from these interactions and depends on parameters like the particle's charge and velocity as well as material properties.
The document discusses atomic structure and bonding. It describes the structure of atoms including protons, neutrons, and electrons. It explains how atomic number determines the element and how isotopes have the same number of protons but different neutrons. Electron configuration and quantum numbers are also summarized. The three main types of bonds - ionic, covalent, and metallic - are introduced along with how they influence material properties.
Electron beam therapy uses accelerated electrons to treat superficial tumors. Electrons interact with matter through inelastic collisions that cause ionization and excitation, and elastic collisions that scatter the electrons. This gives electron beams a characteristically sharp dose drop-off beyond the tumor depth. Key applications of electron beams include treatment of skin cancers, chest wall irradiation for breast cancer, and boost doses to lymph nodes.
The document discusses the structure of atoms and the development of atomic models. It summarizes:
1) The subatomic particles that make up atoms - electrons, protons, and neutrons - along with their relative charges and masses.
2) Early experiments that led to the discovery of electrons and the Thomson and Rutherford atomic models.
3) Quantum numbers like atomic number and mass number that are used to describe atoms.
4) Developments in quantum theory that resulted in Bohr's model of the hydrogen atom and explanation of atomic spectra through quantized energy levels.
This document discusses the wave-particle duality of light and matter. It explains how experiments demonstrating the photoelectric effect and electron diffraction show that electromagnetic radiation and electrons exhibit both wave-like and particle-like properties depending on the situation. De Broglie hypothesized that all particles can behave as waves, and he formulated an equation showing that particles are associated with a wavelength determined by their momentum and Planck's constant.
1. The document discusses optical properties of semiconductors when exposed to electromagnetic radiation like light.
2. It explains concepts like absorption, reflection, transmission and emission spectra that can be obtained from materials and how they provide information about electronic band structures.
3. Key optical phenomena discussed include photon absorption promoting electrons from the valence to conduction band if the photon energy exceeds the semiconductor bandgap, and the interaction of light with materials leading to processes like reflection, refraction, scattering and dispersion.
The document discusses the wave-particle duality of electrons and their behavior in atoms. It describes how J.J. Thomson and his son George Thomson won Nobels for describing electrons as particles and waves respectively. Later, the document covers the quantum mechanical model of the atom, including energy levels, orbitals, quantum numbers, electron spin and configuration. It explains how electrons fill orbitals based on Aufbau's principle, Hund's rule, Pauli exclusion principle and the diagonal rule.
All you need_to_know_about_additional_science[2]mcconvillezoe
This document provides an overview of additional science topics including atomic structure, bonding, properties of materials, quantitative chemistry concepts like moles and reacting masses, rates of reaction influenced by factors like concentration and catalysts, energy changes in reactions, electrolysis and information about acids, bases, salts and their reactions. It includes chapter outlines, explanations of concepts, diagrams and examples to illustrate essential ideas in chemistry.
The document discusses nuclear chemistry, including the structure of the nucleus, radioactive decay via alpha, beta, and gamma emissions, nuclear reactions like fission and fusion, and applications of nuclear processes like using fission to generate energy in nuclear reactors. Key concepts covered are the strong nuclear force, isotopes, radioactivity, decay modes, particle accelerators, and kinetics of radioactive decay. Nuclear reactions produce immense amounts of energy from tiny mass changes according to Einstein's equation E=mc2.
All you need_to_know_about_additional_science[1]lucywalshaw
Structures and bonding, properties of materials, quantitative chemistry and rates of reaction are discussed. Key topics covered include atomic structure, ionic and covalent bonding, properties of materials like conductivity and melting points, amounts of substances and moles, balancing chemical equations, factors that affect rates of reaction like temperature, concentration and surface area. The document provides an overview of content to be covered in additional science chapters on these core chemistry concepts.
Electrons in Atoms can be summarized as follows:
1) Light exhibits both wave-like and particle-like properties, with electrons in atoms also displaying wave-like characteristics that help explain atomic structure.
2) Atoms are arranged according to a set of rules, with electrons occupying specific energy levels and orbitals around the nucleus according to the aufbau principle and other quantum rules.
3) The Bohr and quantum mechanical models both describe the discrete energy levels electrons can occupy in atoms, with the latter treating electrons as waves rather than fixed orbits and establishing probability distributions rather than precise paths.
Radioactivity and production of X-rays - SachinSACHINS700327
This document discusses radioactivity and the production of x-rays. It begins by describing the structure of atoms and different types of radioactive decay such as alpha, beta, and gamma rays. It then discusses concepts like decay constant and half-life. Different modes of radioactive decay like alpha and beta particle decay are explained. The document also covers nuclear reactions, fission, fusion, and how x-rays are produced when high-speed electrons interact with matter. It provides details on the components of an x-ray tube and the physics behind bremsstrahlung and characteristic x-ray production.
This dictionary provides definitions for physics terms ranging from A to C. Some key entries include:
- Atom: The fundamental building block of matter that consists of a nucleus and electrons.
- Absolute Zero: The minimum possible temperature, which is 0K or -273.15°C.
- Acceleration: How fast an object's motion is changing, defined as the rate of change of velocity over time.
- Activity: The rate of radioactive decay in a sample, measured in disintegrations per second.
Physics dictionary for CBSE, ISCE, Class X Students by Arun Umraossuserd6b1fd
Dictionaries are very important. Without definitions of scientific words you can not understand the theories or theorems. This dictionary explains nearly all the terms used in CBSE Class X science book.
This document summarizes key concepts in plasma chemistry from Chapter 2 of the reference book, including:
1) Elementary plasma reactions are determined by micro-kinetic characteristics like cross-sections and reaction probabilities, as well as kinetic distribution functions.
2) Collisions can be elastic, inelastic, or superelastic depending on whether the total kinetic energy and internal energies change during the collision.
3) Ionization processes include direct electron impact ionization, stepwise ionization, ion-molecule collisions, photoionization, and surface ionization.
4) The Thomson formula describes direct electron impact ionization cross-sections at high energies, while the Frank-Condon principle applies to ionization
Elementary plasma-chemical reactions can be described by micro-kinetic characteristics like cross-sections and reaction probabilities. There are several types of ionization processes including direct electron impact ionization, stepwise ionization, and ionization by photons or heavy particles. Collision parameters include the cross-section, probability, mean free path, and reaction rates. Direct ionization follows the Thomson formula at high energies. Molecular ionization is affected by the Frank-Condon principle where atomic positions remain fixed. Stepwise ionization occurs through excitation to an energy above the ionization potential. High-energy electrons like in beams follow the Bethe-Bloch formula for energy loss per unit length.
Similar to Electron irradiation effect on Al2O3 (20)
1) A wave is a disturbance that transfers energy through a medium without permanent transfer of matter. This document discusses mechanical and electromagnetic waves, their characteristics such as wavelength and frequency, and how waves behave in different media like strings and pipes.
2) Resonance occurs when an object vibrates at its natural frequency, causing large oscillations. Standing waves can form in pipes and strings, with nodes and antinodes depending on boundary conditions and wavelength.
3) The Doppler effect describes the change in frequency heard by an observer due to relative motion between the source and observer. The pitch is higher if approaching and lower if receding due to the change in wavelength reaching the observer each second.
This document discusses the expansion of gases and the relationships between pressure, volume, temperature, and number of moles in gases. It introduces the ideal gas law (PV=nRT) and describes some key gas processes including isobaric (constant pressure), isothermal (constant temperature), and isometric (constant volume) processes. Examples are provided to demonstrate how to use the ideal gas law and gas equations of state to calculate pressure, volume, temperature, or number of moles given values of the other variables.
The document discusses temperature, heat, and phase changes. It defines temperature as a measure of the average kinetic energy of particles in an object. Temperature scales like Fahrenheit, Celsius, and Kelvin are introduced. Heat is a form of energy that transfers between objects due to temperature differences. Equations are provided to calculate heat transfer during temperature changes and phase changes using values like specific heat and latent heat. Examples demonstrate using the equations to solve heat and temperature problems involving substances like water, ice, and metals.
This document contains examples and solutions related to fluid statics concepts such as pressure, density, buoyancy, and Pascal's principle. It begins with examples calculating the mass, weight, density, and pressure using given values. Later examples apply concepts like buoyancy, pressure at depths, and pressure transmission using hydraulic jacks. Key formulas introduced include pressure (p=F/A), fluid pressure (p=hρg), and buoyancy (B=Vfluidρfluid). Overall, the document provides practice problems and solutions for understanding fundamental fluid statics principles.
1. A mass attached to a linear spring undergoes simple harmonic motion as it moves up and down. Its motion can be described by equations involving displacement, velocity, acceleration, angular frequency, and the spring constant.
2. For a mass-spring system undergoing simple harmonic motion, the maximum displacement from equilibrium occurs at the amplitude. The spring force is greatest and acceleration is largest at the amplitude, while velocity is greatest at mid-displacement and acceleration is zero at the equilibrium position.
3. Examples are worked through to find displacement as a function of time, angular frequency, maximum velocity and acceleration, and displacement at given times for masses undergoing simple harmonic motion on springs or circular paths. Equations are derived from given
This document provides examples and explanations of concepts related to rotational kinetics, including:
- Torque is calculated as the product of a force and its perpendicular distance from the axis of rotation. Net torque is the sum of all torques acting on an object.
- Rotational equilibrium occurs when the net torque on an object is zero, meaning the sum of clockwise and counterclockwise torques are equal.
- The center of mass of a uniformly distributed object is located at its geometric center. For rotational problems involving uniform objects, the center of mass can be treated as the axis of rotation.
- Newton's second law for rotational motion states that the net torque equals the product of the object's moment
This chapter discusses rotational kinematics, including angular displacement (θ), angular velocity (ω), angular acceleration (α), and time (t). Key relationships are developed between these rotational variables and their linear motion counterparts. Examples are provided to demonstrate calculating angular acceleration, angular displacement, angular velocity, tangential acceleration, centripetal acceleration, and tangential and centripetal forces for objects undergoing rotational motion. Homework problems 1 through 5 at the end of the chapter are assigned.
This document discusses work, energy, and power. It defines work as the product of parallel force and distance. Kinetic energy and gravitational potential energy are forms of mechanical energy. The work-kinetic energy theorem states that work done by net force equals change in kinetic energy. The law of conservation of energy says energy cannot be created or destroyed, only converted from one form to another. Power is defined as work done per unit time. Examples calculate work, kinetic energy, potential energy, efficiency, and power for various situations.
This document summarizes key concepts about uniform circular motion including:
- Radians are the SI unit for measuring angles where 1 radian is the central angle that spans an arc equal to the circle's radius.
- Formulas relate angular quantities like speed (ω) and displacement (θ) to linear quantities like speed (v) and arc length (s) using the radius (R).
- Centripetal force (Fc) is required to cause circular motion and is given by Fc = Mv2/R, where M is the object's mass and v is its speed.
- Banked roads allow vehicles to safely take curved portions faster by providing tilt that replaces needed friction with
Force may cause motion or deformation of an object. Newton's second law relates the net force on an object to its acceleration. An example calculates the engine force needed to accelerate a car based on its mass, acceleration, and frictional force. The document provides additional examples applying Newton's laws to calculate accelerations, forces, distances, and times for objects undergoing different motions.
This document summarizes projectile motion in two dimensions. It explains that a projectile's curved motion can be analyzed as the combination of horizontal and vertical linear motion. In the horizontal direction, the motion is at a constant speed due to the lack of acceleration. In the vertical direction, gravity causes acceleration, resulting in parabolic motion. The document provides an example problem of analyzing the motion of a cannon ball fired at an angle, solving for variables like time, distance, and the equation of its parabolic path. It also gives another example of determining how far a ball will land after rolling off a table.
The document provides information about uniformly accelerated motion along a straight line. It defines key terms like velocity, acceleration, displacement and equations of motion. Several examples are presented to demonstrate the use of equations to solve problems involving uniformly accelerated motion. Examples include calculating acceleration, distance traveled, time taken and velocities given information about an object's motion under constant acceleration along a straight path.
This document discusses fundamental units, vectors, and trigonometry. It begins by defining basic units like length, time, and velocity. It then explains that vectors require both a magnitude and direction, while scalars only require a magnitude. The document provides examples of adding vectors graphically using the head-to-tail method and analytically using trigonometric functions. It also discusses solving for unknown sides of triangles using trigonometric functions like sine, cosine, and tangent.
This study investigated the implantation of sapphire by zirconium and zirconium plus oxygen ions. Important factors that influence amorphization during ion implantation include temperature, ion mass, energy, and fluence. Rutherford backscattering spectrometry was used to determine the threshold fluence for amorphization in sapphire by zirconium implantation and examine the effect of additional oxygen implantation. Optical absorption and photoluminescence measurements provided information about induced color centers and defects from the ion irradiation.
The document describes an experiment to measure Rydberg's constant using the emission spectrum of hydrogen. Electrons in hydrogen atoms absorb energy and transition to higher energy levels. When they drop down, they emit photons of specific wavelengths according to Planck's law. By measuring the wavelengths of photons emitted during transitions from higher to lower energy levels in the Balmer series, Rydberg's constant can be calculated and verified. Measurements of hydrogen's spectral lines will be used to calculate Rydberg's constant and compare to the accepted value.
Nuclear Radiation, the chart of nuclidesYounes Sina
This document provides information about nuclear radiation and the chart of nuclides. It defines key terms like thermal neutrons and fast neutrons. It also summarizes how nuclear reactors work through the fission of U-235 when it absorbs a neutron, and the concept of critical mass. The bulk of the document provides a guide to reading and understanding the chart of nuclides, defining various symbols and indicators on the chart.
Ion implantation effects in sapphire-Poster for advisory meeting at utkYounes Sina
This document discusses a study on the effects of ion implantation in sapphire. Zirconium and boron ions were implanted into sapphire single crystals at room temperature. For zirconium implantation, an amorphous layer was formed at fluences above 4x10^16 Zr+/cm^2. RBS-C, XRD, and other analysis found zirconium formed clusters in the amorphous region. For boron implantation, a high defect density was found without complete loss of crystallinity for fluences up to 1x10^17 B+/cm^2. The study aims to identify the nature of defects introduced and how implanted species interact with the material.
This document discusses backscattering spectrometry, which uses elastic scattering of ions to determine the elemental composition of materials. It describes how Rutherford scattering can be used for low energy particles, while higher energies require solving the Schrodinger equation. Examples are given of using kinematic factors to identify elements in a spectrum and calculating stopping power and cross sections. The document outlines approaches for thin film analysis using peak integration and mean energy calculations to determine areal densities and stoichiometry.
Why You Should Replace Windows 11 with Nitrux Linux 3.5.0 for enhanced perfor...SOFTTECHHUB
The choice of an operating system plays a pivotal role in shaping our computing experience. For decades, Microsoft's Windows has dominated the market, offering a familiar and widely adopted platform for personal and professional use. However, as technological advancements continue to push the boundaries of innovation, alternative operating systems have emerged, challenging the status quo and offering users a fresh perspective on computing.
One such alternative that has garnered significant attention and acclaim is Nitrux Linux 3.5.0, a sleek, powerful, and user-friendly Linux distribution that promises to redefine the way we interact with our devices. With its focus on performance, security, and customization, Nitrux Linux presents a compelling case for those seeking to break free from the constraints of proprietary software and embrace the freedom and flexibility of open-source computing.
Sudheer Mechineni, Head of Application Frameworks, Standard Chartered Bank
Discover how Standard Chartered Bank harnessed the power of Neo4j to transform complex data access challenges into a dynamic, scalable graph database solution. This keynote will cover their journey from initial adoption to deploying a fully automated, enterprise-grade causal cluster, highlighting key strategies for modelling organisational changes and ensuring robust disaster recovery. Learn how these innovations have not only enhanced Standard Chartered Bank’s data infrastructure but also positioned them as pioneers in the banking sector’s adoption of graph technology.
Threats to mobile devices are more prevalent and increasing in scope and complexity. Users of mobile devices desire to take full advantage of the features
available on those devices, but many of the features provide convenience and capability but sacrifice security. This best practices guide outlines steps the users can take to better protect personal devices and information.
In his public lecture, Christian Timmerer provides insights into the fascinating history of video streaming, starting from its humble beginnings before YouTube to the groundbreaking technologies that now dominate platforms like Netflix and ORF ON. Timmerer also presents provocative contributions of his own that have significantly influenced the industry. He concludes by looking at future challenges and invites the audience to join in a discussion.
Encryption in Microsoft 365 - ExpertsLive Netherlands 2024Albert Hoitingh
In this session I delve into the encryption technology used in Microsoft 365 and Microsoft Purview. Including the concepts of Customer Key and Double Key Encryption.
How to Get CNIC Information System with Paksim Ga.pptxdanishmna97
Pakdata Cf is a groundbreaking system designed to streamline and facilitate access to CNIC information. This innovative platform leverages advanced technology to provide users with efficient and secure access to their CNIC details.
LF Energy Webinar: Electrical Grid Modelling and Simulation Through PowSyBl -...DanBrown980551
Do you want to learn how to model and simulate an electrical network from scratch in under an hour?
Then welcome to this PowSyBl workshop, hosted by Rte, the French Transmission System Operator (TSO)!
During the webinar, you will discover the PowSyBl ecosystem as well as handle and study an electrical network through an interactive Python notebook.
PowSyBl is an open source project hosted by LF Energy, which offers a comprehensive set of features for electrical grid modelling and simulation. Among other advanced features, PowSyBl provides:
- A fully editable and extendable library for grid component modelling;
- Visualization tools to display your network;
- Grid simulation tools, such as power flows, security analyses (with or without remedial actions) and sensitivity analyses;
The framework is mostly written in Java, with a Python binding so that Python developers can access PowSyBl functionalities as well.
What you will learn during the webinar:
- For beginners: discover PowSyBl's functionalities through a quick general presentation and the notebook, without needing any expert coding skills;
- For advanced developers: master the skills to efficiently apply PowSyBl functionalities to your real-world scenarios.
zkStudyClub - Reef: Fast Succinct Non-Interactive Zero-Knowledge Regex ProofsAlex Pruden
This paper presents Reef, a system for generating publicly verifiable succinct non-interactive zero-knowledge proofs that a committed document matches or does not match a regular expression. We describe applications such as proving the strength of passwords, the provenance of email despite redactions, the validity of oblivious DNS queries, and the existence of mutations in DNA. Reef supports the Perl Compatible Regular Expression syntax, including wildcards, alternation, ranges, capture groups, Kleene star, negations, and lookarounds. Reef introduces a new type of automata, Skipping Alternating Finite Automata (SAFA), that skips irrelevant parts of a document when producing proofs without undermining soundness, and instantiates SAFA with a lookup argument. Our experimental evaluation confirms that Reef can generate proofs for documents with 32M characters; the proofs are small and cheap to verify (under a second).
Paper: https://eprint.iacr.org/2023/1886
“An Outlook of the Ongoing and Future Relationship between Blockchain Technologies and Process-aware Information Systems.” Invited talk at the joint workshop on Blockchain for Information Systems (BC4IS) and Blockchain for Trusted Data Sharing (B4TDS), co-located with with the 36th International Conference on Advanced Information Systems Engineering (CAiSE), 3 June 2024, Limassol, Cyprus.
Climate Impact of Software Testing at Nordic Testing DaysKari Kakkonen
My slides at Nordic Testing Days 6.6.2024
Climate impact / sustainability of software testing discussed on the talk. ICT and testing must carry their part of global responsibility to help with the climat warming. We can minimize the carbon footprint but we can also have a carbon handprint, a positive impact on the climate. Quality characteristics can be added with sustainability, and then measured continuously. Test environments can be used less, and in smaller scale and on demand. Test techniques can be used in optimizing or minimizing number of tests. Test automation can be used to speed up testing.
Pushing the limits of ePRTC: 100ns holdover for 100 daysAdtran
At WSTS 2024, Alon Stern explored the topic of parametric holdover and explained how recent research findings can be implemented in real-world PNT networks to achieve 100 nanoseconds of accuracy for up to 100 days.
Observability Concepts EVERY Developer Should Know -- DeveloperWeek Europe.pdfPaige Cruz
Monitoring and observability aren’t traditionally found in software curriculums and many of us cobble this knowledge together from whatever vendor or ecosystem we were first introduced to and whatever is a part of your current company’s observability stack.
While the dev and ops silo continues to crumble….many organizations still relegate monitoring & observability as the purview of ops, infra and SRE teams. This is a mistake - achieving a highly observable system requires collaboration up and down the stack.
I, a former op, would like to extend an invitation to all application developers to join the observability party will share these foundational concepts to build on:
Removing Uninteresting Bytes in Software FuzzingAftab Hussain
Imagine a world where software fuzzing, the process of mutating bytes in test seeds to uncover hidden and erroneous program behaviors, becomes faster and more effective. A lot depends on the initial seeds, which can significantly dictate the trajectory of a fuzzing campaign, particularly in terms of how long it takes to uncover interesting behaviour in your code. We introduce DIAR, a technique designed to speedup fuzzing campaigns by pinpointing and eliminating those uninteresting bytes in the seeds. Picture this: instead of wasting valuable resources on meaningless mutations in large, bloated seeds, DIAR removes the unnecessary bytes, streamlining the entire process.
In this work, we equipped AFL, a popular fuzzer, with DIAR and examined two critical Linux libraries -- Libxml's xmllint, a tool for parsing xml documents, and Binutil's readelf, an essential debugging and security analysis command-line tool used to display detailed information about ELF (Executable and Linkable Format). Our preliminary results show that AFL+DIAR does not only discover new paths more quickly but also achieves higher coverage overall. This work thus showcases how starting with lean and optimized seeds can lead to faster, more comprehensive fuzzing campaigns -- and DIAR helps you find such seeds.
- These are slides of the talk given at IEEE International Conference on Software Testing Verification and Validation Workshop, ICSTW 2022.
Goodbye Windows 11: Make Way for Nitrux Linux 3.5.0!SOFTTECHHUB
As the digital landscape continually evolves, operating systems play a critical role in shaping user experiences and productivity. The launch of Nitrux Linux 3.5.0 marks a significant milestone, offering a robust alternative to traditional systems such as Windows 11. This article delves into the essence of Nitrux Linux 3.5.0, exploring its unique features, advantages, and how it stands as a compelling choice for both casual users and tech enthusiasts.
Enchancing adoption of Open Source Libraries. A case study on Albumentations.AIVladimir Iglovikov, Ph.D.
Presented by Vladimir Iglovikov:
- https://www.linkedin.com/in/iglovikov/
- https://x.com/viglovikov
- https://www.instagram.com/ternaus/
This presentation delves into the journey of Albumentations.ai, a highly successful open-source library for data augmentation.
Created out of a necessity for superior performance in Kaggle competitions, Albumentations has grown to become a widely used tool among data scientists and machine learning practitioners.
This case study covers various aspects, including:
People: The contributors and community that have supported Albumentations.
Metrics: The success indicators such as downloads, daily active users, GitHub stars, and financial contributions.
Challenges: The hurdles in monetizing open-source projects and measuring user engagement.
Development Practices: Best practices for creating, maintaining, and scaling open-source libraries, including code hygiene, CI/CD, and fast iteration.
Community Building: Strategies for making adoption easy, iterating quickly, and fostering a vibrant, engaged community.
Marketing: Both online and offline marketing tactics, focusing on real, impactful interactions and collaborations.
Mental Health: Maintaining balance and not feeling pressured by user demands.
Key insights include the importance of automation, making the adoption process seamless, and leveraging offline interactions for marketing. The presentation also emphasizes the need for continuous small improvements and building a friendly, inclusive community that contributes to the project's growth.
Vladimir Iglovikov brings his extensive experience as a Kaggle Grandmaster, ex-Staff ML Engineer at Lyft, sharing valuable lessons and practical advice for anyone looking to enhance the adoption of their open-source projects.
Explore more about Albumentations and join the community at:
GitHub: https://github.com/albumentations-team/albumentations
Website: https://albumentations.ai/
LinkedIn: https://www.linkedin.com/company/100504475
Twitter: https://x.com/albumentations
Essentials of Automations: The Art of Triggers and Actions in FMESafe Software
In this second installment of our Essentials of Automations webinar series, we’ll explore the landscape of triggers and actions, guiding you through the nuances of authoring and adapting workspaces for seamless automations. Gain an understanding of the full spectrum of triggers and actions available in FME, empowering you to enhance your workspaces for efficient automation.
We’ll kick things off by showcasing the most commonly used event-based triggers, introducing you to various automation workflows like manual triggers, schedules, directory watchers, and more. Plus, see how these elements play out in real scenarios.
Whether you’re tweaking your current setup or building from the ground up, this session will arm you with the tools and insights needed to transform your FME usage into a powerhouse of productivity. Join us to discover effective strategies that simplify complex processes, enhancing your productivity and transforming your data management practices with FME. Let’s turn complexity into clarity and make your workspaces work wonders!
2. Ionization vs. Excitation
Excitation transfers enough energy to an orbital electron to displace it
further away from the nucleus.
IONISATION
EXCITATION
Incident electron with a specific energy
Atomic electron absorbs energy and moves into a higher orbit
High energy incident electron
Ejected electron
In ionization the electron is removed, resulting in an ion pair.
3. Bremsstralung (or Braking) Radiation
•High speed electrons may lose energy in the form of X-
rays when they quickly decelerate upon striking a heavy
material.
4. Bremsstrahlung
Probability of bremsstrahlung production per atom is
proportional to the square of Z of the absorber
Energy emission via bremsstrahlung varies inversely with the
square of the mass of the incident particle
Protons and alpha particles produce less than one-millionth
the amount of bremsstrahlung radiation as electrons of the
same energy
5. Bremsstrahlung
Ratio of electron energy loss by bremsstrahlung production to
that lost by excitation and ionization = EZ/820
E = kinetic energy of incident electron in MeV
Z = atomic number of the absorber
Energy loss for Al: Brem./ (Exc. & Ion.) = 1×13/820 = 1.58%
6. Charged Particle Tracks
Electrons follow tortuous paths in matter as the result of multiple
scattering events
• Ionization track is sparse and nonuniform
Larger mass of heavy charged particle results in dense and usually linear
ionization track
Path length is actual distance particle travels; range is actual depth of
penetration in matter
7. Particle interactions
Energetic charged particles interact with matter by
electrical forces and lose kinetic energy via:
Excitation
Ionization
Radiative losses
~ 70% of charged particle energy deposition leads
to nonionizing excitation
8. Dose = Absorbed Energy Density
Absorbed energy normalized by weight, volume, atoms, etc.
J
1 Gy = 1
kg
SI units
8
9. Water: heat to boiling point
H2O J
cp = 4.1813 (@ 25°C)
gK
specific heat of water
T 80 K
3
J 10 g
c H2O
p T = 334.5
g kg
5 J
3.345 10
kg
0.3345 MGy Energy
Absorbed
9
18. Electron irradiation-induced amorphization
of sapphire (Al2O3)
Two components of damage:
1. electronic component
(electron excitation/ionization; radiolysis)
2. nuclear component
(ballistic or displacement damage)
20. Electron Excitation/Ionization
Bethe-Ashkin expression for ionization energy loss per unit length
H. A. Bethe, and J. Ashkin, in Experimental Nuclear Physics. Volume I, edited by E. Segrè (John Wiley &
Sons, Inc., New York, 1953), pp. 166-357.
22. E0 me c rest energy of the electron
2
me rest mass of the electron
c speed of light
e 14.4 eV Å
2
23. v
c
v velocity of electron
c speed of light
2
E0
1
E E
0
E0 rest energy of the electron
E kinetic energy of the electron
24. e Z a
e electron density
Z atomic number
a atomic density
25. 0.19
J 9.76 Z 58.5 Z (eV)
mean electron excitation potential
M. J. Berger, and S. M. Seltzer, Nat. Acad. Sci. / Nat. Res. Council Publ. 1133 (Washington,
1964), p. 205.
26. Bragg’s Rule for Additivity of Stopping Powers
W. H. Bragg, and M. A. Elder, Phil. Mag. 10, 318
(1905)
27. Stopping Power
1 dE eV Å2
e Se E atom e
a dx e
28. Bragg’s Rule for Additivity of Stopping Powers
For binary compound with molecular unit, A B :
m n
Am Bn
e
m e n e
A B
where m is the number of A atoms in molecule A B
m n
and n is the number of B atoms in molecule A B
m n
One can show that:
Am Bn A B
dE dE dE
Am Bn
m Am Bn
dx e
e
dx e dx e
where
Am Bn
is the molecular density of A B
m m n
molecules in the compound.
30. E = 1000 keV= 1 MeV
dE/dx (E = 1 MeV) = -0.0377 eV/Å . e-
thickness = 1000 Å
TEM sample thickness
Total ionization energy
= 37.7 eV/e- = 6.032x10-18 J/e-
loss over sample thickness
32. dE
Areal Energy Density =
dx electronic
J 11
3.504 10
=37.7×108 eV/Ȧ2= 3.77×10-10 J/Ȧ2Å 2
Areal Energy Density
Total Energy Density =
thickness
14 J
3.504 10 3
=3.77×10-13 J/Ȧ3 Å
35. Electron displacement damage calculation
Primary damage cross-section after Seitz & Koehler (1956):
F. Seitz, and J. S. Koehler, in Solid State Physics: Advances in Research & Applications, edited by F.
Seitz, and D. Turnbull (Academic Press, 1956), pp. 305-448.
Based on the relativistic electron cross-section expression derived by McKinley & Feshbach (1948):
W. A. McKinley, Jr., and H. Feshbach, Physical Review 74, 1759 (1948).
Total cross-section (primary plus secondaries) after Oen (1973):
O. S. Oen, (Oak Ridge National Laboratory, Oak Ridge, TN, 1973), pp. 204.
36. Differential displacement cross-section, dσ
b 2 T T T dT
d (T ) T 1 2 2
4 m Tm Tm Tm T
where T is the kinetic energy of the electron
2
E0
v / c 1
E0 E
Z
where is the fine structure constant (~1/137)
37.
Tm maximum energy transfer from e to target atom
4 me M E
Tm E 1
me M 2 E0
2
where E is the incident electron energy
O
Ca
42. Primary displacement cross-section:
Tm area
p (E) d (T )
Ed
atom
where E d is the displacement threshold energy
Cascade cross-section:
Tm area
tot (E) (T ) d (T )
Ed
atom
where (T ) is the number of secondary displacements,
given most simply by the Kinchin-Pease expression:
(T ) 0; T < Ed
(T ) 1; Ed T < 2Ed
T
(T ) ; T 2Ed
2Ed
43. E = 1000 keV
ZO = 8 TmO =271
ZAl = 13 TmAl =161
ZAve =10 TmAve =227
44. Ed = 20 eV
ZO = 8 EtO = 129,000
ZAl = 13 EtAl = 205,000
Zave =10 EtAve = 159,400
45. Ed = 40 eV
ZO= 8 EO= 238,000
ZAl= 13 EAl= 365,000
ZAve=10
46. Ed = 50 eV
ZO= 8 EO = 290,000
ZAl= 13 EAl = 430,000
ZAve=10
47. E=1 MeV
Ed=40 eV
ZO= 8 EtO= 290,000 eV
ZAl= 13 EtAl= 430,000 eV
ZAve=10
TmAve=227 eV
2Ed=80 eV
50. E 300 keV
powellite (CaMoO4) Ed 25 eV
Z ave
15.67 Ethreshold 295 keV
ave
Tm 25.54 eV
ave
2Ed 50 eV
2
Å
tot (E) p (E) 0.588 barns = 5.88 10 9
atom
55. where (T ) is the number of secondary displaceme
given most simply by the Kinchin-Pease expression
(T ) 0; TmT < Ed area
tot (E) (T ) d (T )
(T ) 1; EdEd T < 2Ed atom
where (TT is the number of secondary displacemen
)
(T ) ; T 2Ed
given most simply by the Kinchin-Pease expression:
2Ed
(T ) 0; T < Ed
section Ed T < for
Cross(T ) 1; calculation 2EdAl (Ed=20 eV):
T
(T ) ; T 2Ed
2Ed
σ =42 barns/atom= 4.2×10-7 Å2/atom
tot
1 barn = 10-24 cm 2 10 8 Å2
56. Electron fluence:
Φ=1×1028 e/m2=1×108 e/Å2
Irradiation time, t = 2 hr = 7200 s
φ= 1.38×104 e-/Å2s
displacements per atom = tot
Å2 e
σtot=42 barns/atom= 4.2×10-7 Å2/atom310 6 2
5.88 10 6
atom Å
= 0.018 dpa
dpa=(4.2×10-7 Å2/e).(1×108 e/Å2) = 42
57. RADIATION DAMAGE OF α-Al2O3 IN THE HVEM
II. Radiation damage at high temperature and high dose
G.P. PELLS and D.C. PHILLIPS
58. C. L. Chen, H. Furusho and H. Mori
• The decomposition of α- Al2O3 under 200 keV
(Ultra High Vacuum) electron irradiation
• Aluminum precipitated from α- Al2O3 under 200
keV electron irradiation for less than 1 min over
the temperature range 700 to 1273 K.
• φ (electron dose rate)= 1023 e m-2s-1
• Vacuum level < 3×10-8 Pa
Model:
Thermally activated atom movement
Forced atom displacement ( knock-on collision)
59.
60. RADIATION DAMAGE OF α-Al2O3 IN THE HVEM
II. Radiation damage at high temperature and high dose
G.P. PELLS and D.C. PHILLIPS
Single-crystal α-Al2O3 irradiated with 1 MeV electrons in a high-voltage
electron microscope at several fixed temperatures in the range 320-
1070 K.
• At 770 K and below the nature of the observed damage could not be
resolved.
• At 870 K and above island-like surface features rapidly formed followed
by dislocations which grew to form a dense network.
• After high doses (>l0 dpa) precipitates were observed.
• The associated diffraction patterns and their temperature dependence
suggested that the precipitates were of aluminum metal.
61. Cryogenic radiation response of sapphire
R. Devanathan, W.J. Weber, K.E. Sickafus, M. Nastasi, L.M. Wang, S.X. Wang
Sapphire (a-Al2O3) irradiated by heavy-ion and electron at cryogenic
temperatures using a high-voltage electron microscope.
1.5 MeV Xe
1 MeV Kr
Dual beam of 1 MeV Kr and 900 keV electrons
T=20 to 100 K
At 20 K, α-alumina is amorphized by 1.5 MeV Xe about 3.8 (dpa)
Critical temperature for amorphization is about 170 K
The material remains crystalline when irradiated at 26 K with a dual beam
of heavy ions and electrons.
Electron irradiation can promote damage annealing, even at cryogenic
temperatures, by causing the migration of point-defects produced in
ceramics by ion irradiation.
62. Effects of ionizing radiation in ceramics
R. Devanathan ,K.E. Sickafus, W.J. Weber, M. Nastasi
α-Al2O3 was irradiated with 1 MeV Kr+ or 1.5 MeV Xe+ and 1
MeV electrons in a high-voltage electron microscope interfaced
to an ion accelerator that enabled the in situ observation of the
structural changes.
The results indicate that simultaneous electron irradiation can
retard or prevent amorphization by heavy ions.
Comparison with similar experiments in metals suggests that
highly ionizing radiation can anneal damage to the crystal lattice
in ceramics by enhancing the mobility of point defects.
63. High flux e-
O2
~1000 Å heat
Al ppt.
Vacuum
>40 dpa
Long time
Surface at high stress