This document discusses cavity theory, stopping-power ratios, and correction factors for dosimetry in radiation therapy. It begins with an introduction and overview of topics to be covered, including "large" photon detectors, Bragg-Gray cavity theory, stopping-power ratios, thick-walled ion chambers, correction factors, general cavity theory, and practical detectors. The key points are that detectors almost never directly measure dose to tissue, so interpretation requires dosimetry theory like cavity theory; and the Bragg-Gray cavity theory and stopping-power ratios provide methods to relate detector readings to actual dose in tissue.
The hairpin probe is a well known technique for measuring local electron density in low temperature plasmas. In reactive plasmas, the probe characteristics are affected by surface sputtering, contamination, and secondary electron emission. At higher densities, the plasma absorbs the entire electromagnetic energy of hairpin and hence limits the density measurements. These issues can be resolved by covering the hairpin surface with a thin layer of dielectric. In this letter, the dielectric contribution to the probe characteristics is incorporated in a theory which is experimentally verified. The dielectric covering improves the performance of probe and also allows the hairpin tip to survive in reactive plasma where classical electrical probes are easily damaged.
Direct detection of a break in the teraelectronvolt cosmic-ray spectrum of el...Sérgio Sacani
High-energy cosmic-ray electrons and positrons (CREs), which
lose energy quickly during their propagation, provide a probe of
Galactic high-energy processes1–7 and may enable the observation
of phenomena such as dark-matter particle annihilation or
decay8–10. The CRE spectrum has been measured directly up to
approximately 2 teraelectronvolts in previous balloon- or spaceborne
experiments11–16, and indirectly up to approximately 5
teraelectronvolts using ground-based Cherenkov γ-ray telescope
arrays17,18. Evidence for a spectral break in the teraelectronvolt
energy range has been provided by indirect measurements17,18,
although the results were qualified by sizeable systematic
uncertainties. Here we report a direct measurement of CREs in the
energy range 25 gigaelectronvolts to 4.6 teraelectronvolts by the
Dark Matter Particle Explorer (DAMPE)19 with unprecedentedly
high energy resolution and low background. The largest part of
the spectrum can be well fitted by a ‘smoothly broken power-law’
model rather than a single power-law model. The direct detection of
a spectral break at about 0.9 teraelectronvolts confirms the evidence
found by previous indirect measurements17,18, clarifies the behaviour
of the CRE spectrum at energies above 1 teraelectronvolt and sheds
light on the physical origin of the sub-teraelectronvolt CREs.
A Nano Capacitor Including Graphene Layers Composed with Doped Boron and Nitr...CrimsonPublishersRDMS
A Nano Capacitor Including Graphene Layers Composed with Doped Boron and Nitrogen by Majid Monajjemi* in Crimson Publishers: Peer Reviewed Material Science Journals
»Over the last two decades several patents and research papers have reported purported practical methods to extract useful energy from the vacuum. I describe the inventions and analyze the underlying physics. From an analysis based on first principles it is clear that most of the inventions have fundamental errors and cannot work. The basic concept of harvesting zero-point energy remains viable, and at least one patented concept might work.
The vacuum is filled with a high density of zero-point energy, in the form of modes (vibrational patterns) of electromagnetic field. Over the last eight decades it has become clear that this zero-point field (ZPF) vacuum energy is not simply a mathematical formalism, but produces demonstrable effects on physical systems. Along with that realization has come the desire to extract energy from the ZPF.
One set of methods use nonlinear elements to convert the ZPF into a usable form. A rectifier (used to convert AC to DC) is a strongly nonlinear element. One patent makes use of antennas to capture the ZPF. This energy is then rectified and used. Another set of inventions simply rectify fluctuations (noise) in electronic elements as an extraction method. Using a detailed balance argument, I show that these methods cannot work.
Another set of patents describe using a Casimir cavity to mechanically extract energy from the ZPF. A Casimir cavity consists of two closely space reflecting plates that exclude ZPF electromagnetic modes having wavelengths larger than twice the gap spacing. The result is that the imbalance in the density of the ZPF inside and outside the cavity causes the plates to be attracted to each other. This attractive potential can be used, but only once. To produce power continuously, a method must be devised to form a reciprocating Casimir engine. The patents purport to switch off the Casimir attraction while the plates are pulled apart, so that they can repeatedly accelerate together and produce power. This approach is shown to be fundamentally flawed, and cannot produce power continuously.
A recently issued patent describes a method by which vacuum energy is extracted from gas flowing through a Casimir cavity. According to stochastic electrodynamics, the electronic orbitals in atoms are supported by ambient ZPF. When the gas atoms are pumped into a Casimir cavity, where long-wavelength ZPF modes are excluded, the electrons spin down into lower orbitals, releasing energy. This energy is harvested in a local absorber. When the electrons exit the Casimir cavity, they are re-energized to their original orbitals by the ambient ZPF. The process is repeated to produce continuous power. This method does not suffer from the fundamental flaws of the other approaches, and might work.«
Welcome to International Journal of Engineering Research and Development (IJERD)IJERD Editor
journal publishing, how to publish research paper, Call For research paper, international journal, publishing a paper, IJERD, journal of science and technology, how to get a research paper published, publishing a paper, publishing of journal, publishing of research paper, reserach and review articles, IJERD Journal, How to publish your research paper, publish research paper, open access engineering journal, Engineering journal, Mathemetics journal, Physics journal, Chemistry journal, Computer Engineering, Computer Science journal, how to submit your paper, peer reviw journal, indexed journal, reserach and review articles, engineering journal, www.ijerd.com, research journals,
yahoo journals, bing journals, International Journal of Engineering Research and Development, google journals, hard copy of journal
The hairpin probe is a well known technique for measuring local electron density in low temperature plasmas. In reactive plasmas, the probe characteristics are affected by surface sputtering, contamination, and secondary electron emission. At higher densities, the plasma absorbs the entire electromagnetic energy of hairpin and hence limits the density measurements. These issues can be resolved by covering the hairpin surface with a thin layer of dielectric. In this letter, the dielectric contribution to the probe characteristics is incorporated in a theory which is experimentally verified. The dielectric covering improves the performance of probe and also allows the hairpin tip to survive in reactive plasma where classical electrical probes are easily damaged.
Direct detection of a break in the teraelectronvolt cosmic-ray spectrum of el...Sérgio Sacani
High-energy cosmic-ray electrons and positrons (CREs), which
lose energy quickly during their propagation, provide a probe of
Galactic high-energy processes1–7 and may enable the observation
of phenomena such as dark-matter particle annihilation or
decay8–10. The CRE spectrum has been measured directly up to
approximately 2 teraelectronvolts in previous balloon- or spaceborne
experiments11–16, and indirectly up to approximately 5
teraelectronvolts using ground-based Cherenkov γ-ray telescope
arrays17,18. Evidence for a spectral break in the teraelectronvolt
energy range has been provided by indirect measurements17,18,
although the results were qualified by sizeable systematic
uncertainties. Here we report a direct measurement of CREs in the
energy range 25 gigaelectronvolts to 4.6 teraelectronvolts by the
Dark Matter Particle Explorer (DAMPE)19 with unprecedentedly
high energy resolution and low background. The largest part of
the spectrum can be well fitted by a ‘smoothly broken power-law’
model rather than a single power-law model. The direct detection of
a spectral break at about 0.9 teraelectronvolts confirms the evidence
found by previous indirect measurements17,18, clarifies the behaviour
of the CRE spectrum at energies above 1 teraelectronvolt and sheds
light on the physical origin of the sub-teraelectronvolt CREs.
A Nano Capacitor Including Graphene Layers Composed with Doped Boron and Nitr...CrimsonPublishersRDMS
A Nano Capacitor Including Graphene Layers Composed with Doped Boron and Nitrogen by Majid Monajjemi* in Crimson Publishers: Peer Reviewed Material Science Journals
»Over the last two decades several patents and research papers have reported purported practical methods to extract useful energy from the vacuum. I describe the inventions and analyze the underlying physics. From an analysis based on first principles it is clear that most of the inventions have fundamental errors and cannot work. The basic concept of harvesting zero-point energy remains viable, and at least one patented concept might work.
The vacuum is filled with a high density of zero-point energy, in the form of modes (vibrational patterns) of electromagnetic field. Over the last eight decades it has become clear that this zero-point field (ZPF) vacuum energy is not simply a mathematical formalism, but produces demonstrable effects on physical systems. Along with that realization has come the desire to extract energy from the ZPF.
One set of methods use nonlinear elements to convert the ZPF into a usable form. A rectifier (used to convert AC to DC) is a strongly nonlinear element. One patent makes use of antennas to capture the ZPF. This energy is then rectified and used. Another set of inventions simply rectify fluctuations (noise) in electronic elements as an extraction method. Using a detailed balance argument, I show that these methods cannot work.
Another set of patents describe using a Casimir cavity to mechanically extract energy from the ZPF. A Casimir cavity consists of two closely space reflecting plates that exclude ZPF electromagnetic modes having wavelengths larger than twice the gap spacing. The result is that the imbalance in the density of the ZPF inside and outside the cavity causes the plates to be attracted to each other. This attractive potential can be used, but only once. To produce power continuously, a method must be devised to form a reciprocating Casimir engine. The patents purport to switch off the Casimir attraction while the plates are pulled apart, so that they can repeatedly accelerate together and produce power. This approach is shown to be fundamentally flawed, and cannot produce power continuously.
A recently issued patent describes a method by which vacuum energy is extracted from gas flowing through a Casimir cavity. According to stochastic electrodynamics, the electronic orbitals in atoms are supported by ambient ZPF. When the gas atoms are pumped into a Casimir cavity, where long-wavelength ZPF modes are excluded, the electrons spin down into lower orbitals, releasing energy. This energy is harvested in a local absorber. When the electrons exit the Casimir cavity, they are re-energized to their original orbitals by the ambient ZPF. The process is repeated to produce continuous power. This method does not suffer from the fundamental flaws of the other approaches, and might work.«
Welcome to International Journal of Engineering Research and Development (IJERD)IJERD Editor
journal publishing, how to publish research paper, Call For research paper, international journal, publishing a paper, IJERD, journal of science and technology, how to get a research paper published, publishing a paper, publishing of journal, publishing of research paper, reserach and review articles, IJERD Journal, How to publish your research paper, publish research paper, open access engineering journal, Engineering journal, Mathemetics journal, Physics journal, Chemistry journal, Computer Engineering, Computer Science journal, how to submit your paper, peer reviw journal, indexed journal, reserach and review articles, engineering journal, www.ijerd.com, research journals,
yahoo journals, bing journals, International Journal of Engineering Research and Development, google journals, hard copy of journal
1 ECE 6340 Fall 2013 Homework 8 Assignment.docxjoyjonna282
1
ECE 6340
Fall 2013
Homework 8
Assignment: Please do Probs. 1-9 and 13 from the set below.
1) In dynamics, we have the equation
E j Aω= − −∇Φ .
(a) Show that in statics, the scalar potential function Φ can be interpreted as a voltage
function. That is, show that in statics
( ) ( )
B
AB
A
V E dr A B≡ ⋅ = Φ −Φ∫ .
(b) Next, explain why this equation is not true (in general) in dynamics.
(c) Explain why the voltage drop (defined as the line integral of the electric field, as
defined above) depends on the path from A to B in dynamics, using Faraday’s law.
(d) Does the right-hand side of the above equation (the difference in the potential
function) depend on the path, in dynamics?
Hint: Note that, according to calculus, for any function ψ we have
dr dx dy dz d
x y z
ψ ψ ψ
ψ ψ
∂ ∂ ∂
∇ ⋅ = + + =
∂ ∂ ∂
.
2) Starting with Maxwell’s equations, show that the electric field radiated by an impressed
current density source J i in an infinite homogeneous region satisfies the equation
( )2 2 iE k E E j Jωµ∇ + = ∇ ∇⋅ + .
Then use Ampere’s law (or, if you prefer, the continuity equation and the electric Gauss
law) to show that this equation may be written as
( )2 2 1 i iE k E J j J
j
ωµ
σ ωε
∇ + = − ∇ ∇⋅ +
+
.
2
Note that the total current density is the sum of the impressed current density and the
conduction current density, the latter obeying Ohm’s law (J c = σE).
Explain why this equation for the electric field would be harder to solve than the equation
that was derived in class for the magnetic vector potential.
3) Show that magnetic field radiated by an impressed current density source satisfies the
equation
2 2 iH k H J∇ + = −∇× .
Explain why this equation for the magnetic field would be harder to solve than the
equation that was derived in class for the magnetic vector potential.
4) Show that in a homogenous region of space the scalar electric potential satisfies the
equation
2 2
i
v
c
k
ρ
ε
∇ Φ + Φ = − ,
where ivρ is the impressed (source) charge density, which is the charge density that goes
along with the impressed current density, being related by
i ivJ jωρ∇⋅ = −
Hint: Start with E j Aω= − −∇Φ and take the divergence of both sides. Also, take the
divergence of both sides of Ampere’s law and use the continuity equation for the
impressed current (given above) to show that
1 ii v
c c
E J
j
ρ
ωε ε
∇⋅ = − ∇⋅ = .
Note: It is also true from the electric Gauss law that
vE
ρ
ε
∇⋅ = ,
but we prefer to have only an impressed (source) charge density on the right-hand side of
the equation for the potential Φ. In the time-harmonic steady state, assuming a
homogeneous and isotropic region, it follows that ρv = ρvi. That is, there is no charge
3
density arising from the conduction current. (If there were no impressed current sources,
the total charge density would therefore be ze ...
Poster of my master\'s research presented at the Physics@FOM conference at Veldhoven on 20 januari 2010. There\'s one error in the equations, can you find it?
Capacitance-voltage Profiling Techniques for Characterization of Semiconduct...eeiej_journal
A new capacitance-voltage profiling technique of semiconductor junctions is proposed for characterisation of semiconductor materials and devices. The measurement technique is simple, non-destructive and it has a greater accuracy compared with the classical C-V method of J. Hilibrand and R. D. Gold, developed in 1960.
I am Irene M. I am an Electromagnetism Assignment Expert at eduassignmenthelp.com. I hold a Ph.D. in Electromagnetism, from California, USA. I have been helping students with their homework for the past 8 years. I solve assignments related to Electromagnetism.
Visit eduassignmenthelp.com or email info@eduassignmenthelp.com.
You can also call on +1 678 648 4277 for any assistance with Electromagnetism Assignments.
Enhancing the Performance of P3HT/Cdse Solar Cells by Optimal Designing of Ac...IOSRJEEE
The present study examined the influence of different condition like as doping , in active layer, on the performance of P3HT/CdSe Solar cells .In this work, we analyzed the best doping for the configuration of P3HT/ CdSe in order to improve the performance of the solar cell. For this aim, we investigated the current density of electrons, the electric field, the short-circuit current and the open-circuit voltage in different doping . The results indicate that when the doping is increased in P3Ht and is decreased in CdSe, the current density of electrons, the electric field, the short-circuit current, and the open-circuit voltage are increased. Finally, we obtained doping of and for electron and hole donor respectively as the best doping for this configuration
1 ECE 6340 Fall 2013 Homework 8 Assignment.docxjoyjonna282
1
ECE 6340
Fall 2013
Homework 8
Assignment: Please do Probs. 1-9 and 13 from the set below.
1) In dynamics, we have the equation
E j Aω= − −∇Φ .
(a) Show that in statics, the scalar potential function Φ can be interpreted as a voltage
function. That is, show that in statics
( ) ( )
B
AB
A
V E dr A B≡ ⋅ = Φ −Φ∫ .
(b) Next, explain why this equation is not true (in general) in dynamics.
(c) Explain why the voltage drop (defined as the line integral of the electric field, as
defined above) depends on the path from A to B in dynamics, using Faraday’s law.
(d) Does the right-hand side of the above equation (the difference in the potential
function) depend on the path, in dynamics?
Hint: Note that, according to calculus, for any function ψ we have
dr dx dy dz d
x y z
ψ ψ ψ
ψ ψ
∂ ∂ ∂
∇ ⋅ = + + =
∂ ∂ ∂
.
2) Starting with Maxwell’s equations, show that the electric field radiated by an impressed
current density source J i in an infinite homogeneous region satisfies the equation
( )2 2 iE k E E j Jωµ∇ + = ∇ ∇⋅ + .
Then use Ampere’s law (or, if you prefer, the continuity equation and the electric Gauss
law) to show that this equation may be written as
( )2 2 1 i iE k E J j J
j
ωµ
σ ωε
∇ + = − ∇ ∇⋅ +
+
.
2
Note that the total current density is the sum of the impressed current density and the
conduction current density, the latter obeying Ohm’s law (J c = σE).
Explain why this equation for the electric field would be harder to solve than the equation
that was derived in class for the magnetic vector potential.
3) Show that magnetic field radiated by an impressed current density source satisfies the
equation
2 2 iH k H J∇ + = −∇× .
Explain why this equation for the magnetic field would be harder to solve than the
equation that was derived in class for the magnetic vector potential.
4) Show that in a homogenous region of space the scalar electric potential satisfies the
equation
2 2
i
v
c
k
ρ
ε
∇ Φ + Φ = − ,
where ivρ is the impressed (source) charge density, which is the charge density that goes
along with the impressed current density, being related by
i ivJ jωρ∇⋅ = −
Hint: Start with E j Aω= − −∇Φ and take the divergence of both sides. Also, take the
divergence of both sides of Ampere’s law and use the continuity equation for the
impressed current (given above) to show that
1 ii v
c c
E J
j
ρ
ωε ε
∇⋅ = − ∇⋅ = .
Note: It is also true from the electric Gauss law that
vE
ρ
ε
∇⋅ = ,
but we prefer to have only an impressed (source) charge density on the right-hand side of
the equation for the potential Φ. In the time-harmonic steady state, assuming a
homogeneous and isotropic region, it follows that ρv = ρvi. That is, there is no charge
3
density arising from the conduction current. (If there were no impressed current sources,
the total charge density would therefore be ze ...
Poster of my master\'s research presented at the Physics@FOM conference at Veldhoven on 20 januari 2010. There\'s one error in the equations, can you find it?
Capacitance-voltage Profiling Techniques for Characterization of Semiconduct...eeiej_journal
A new capacitance-voltage profiling technique of semiconductor junctions is proposed for characterisation of semiconductor materials and devices. The measurement technique is simple, non-destructive and it has a greater accuracy compared with the classical C-V method of J. Hilibrand and R. D. Gold, developed in 1960.
I am Irene M. I am an Electromagnetism Assignment Expert at eduassignmenthelp.com. I hold a Ph.D. in Electromagnetism, from California, USA. I have been helping students with their homework for the past 8 years. I solve assignments related to Electromagnetism.
Visit eduassignmenthelp.com or email info@eduassignmenthelp.com.
You can also call on +1 678 648 4277 for any assistance with Electromagnetism Assignments.
Enhancing the Performance of P3HT/Cdse Solar Cells by Optimal Designing of Ac...IOSRJEEE
The present study examined the influence of different condition like as doping , in active layer, on the performance of P3HT/CdSe Solar cells .In this work, we analyzed the best doping for the configuration of P3HT/ CdSe in order to improve the performance of the solar cell. For this aim, we investigated the current density of electrons, the electric field, the short-circuit current and the open-circuit voltage in different doping . The results indicate that when the doping is increased in P3Ht and is decreased in CdSe, the current density of electrons, the electric field, the short-circuit current, and the open-circuit voltage are increased. Finally, we obtained doping of and for electron and hole donor respectively as the best doping for this configuration
Basavarajeeyam is a Sreshta Sangraha grantha (Compiled book ), written by Neelkanta kotturu Basavaraja Virachita. It contains 25 Prakaranas, First 24 Chapters related to Rogas& 25th to Rasadravyas.
The Gram stain is a fundamental technique in microbiology used to classify bacteria based on their cell wall structure. It provides a quick and simple method to distinguish between Gram-positive and Gram-negative bacteria, which have different susceptibilities to antibiotics
Recomendações da OMS sobre cuidados maternos e neonatais para uma experiência pós-natal positiva.
Em consonância com os ODS – Objetivos do Desenvolvimento Sustentável e a Estratégia Global para a Saúde das Mulheres, Crianças e Adolescentes, e aplicando uma abordagem baseada nos direitos humanos, os esforços de cuidados pós-natais devem expandir-se para além da cobertura e da simples sobrevivência, de modo a incluir cuidados de qualidade.
Estas diretrizes visam melhorar a qualidade dos cuidados pós-natais essenciais e de rotina prestados às mulheres e aos recém-nascidos, com o objetivo final de melhorar a saúde e o bem-estar materno e neonatal.
Uma “experiência pós-natal positiva” é um resultado importante para todas as mulheres que dão à luz e para os seus recém-nascidos, estabelecendo as bases para a melhoria da saúde e do bem-estar a curto e longo prazo. Uma experiência pós-natal positiva é definida como aquela em que as mulheres, pessoas que gestam, os recém-nascidos, os casais, os pais, os cuidadores e as famílias recebem informação consistente, garantia e apoio de profissionais de saúde motivados; e onde um sistema de saúde flexível e com recursos reconheça as necessidades das mulheres e dos bebês e respeite o seu contexto cultural.
Estas diretrizes consolidadas apresentam algumas recomendações novas e já bem fundamentadas sobre cuidados pós-natais de rotina para mulheres e neonatos que recebem cuidados no pós-parto em unidades de saúde ou na comunidade, independentemente dos recursos disponíveis.
É fornecido um conjunto abrangente de recomendações para cuidados durante o período puerperal, com ênfase nos cuidados essenciais que todas as mulheres e recém-nascidos devem receber, e com a devida atenção à qualidade dos cuidados; isto é, a entrega e a experiência do cuidado recebido. Estas diretrizes atualizam e ampliam as recomendações da OMS de 2014 sobre cuidados pós-natais da mãe e do recém-nascido e complementam as atuais diretrizes da OMS sobre a gestão de complicações pós-natais.
O estabelecimento da amamentação e o manejo das principais intercorrências é contemplada.
Recomendamos muito.
Vamos discutir essas recomendações no nosso curso de pós-graduação em Aleitamento no Instituto Ciclos.
Esta publicação só está disponível em inglês até o momento.
Prof. Marcus Renato de Carvalho
www.agostodourado.com
These simplified slides by Dr. Sidra Arshad present an overview of the non-respiratory functions of the respiratory tract.
Learning objectives:
1. Enlist the non-respiratory functions of the respiratory tract
2. Briefly explain how these functions are carried out
3. Discuss the significance of dead space
4. Differentiate between minute ventilation and alveolar ventilation
5. Describe the cough and sneeze reflexes
Study Resources:
1. Chapter 39, Guyton and Hall Textbook of Medical Physiology, 14th edition
2. Chapter 34, Ganong’s Review of Medical Physiology, 26th edition
3. Chapter 17, Human Physiology by Lauralee Sherwood, 9th edition
4. Non-respiratory functions of the lungs https://academic.oup.com/bjaed/article/13/3/98/278874
- Video recording of this lecture in English language: https://youtu.be/kqbnxVAZs-0
- Video recording of this lecture in Arabic language: https://youtu.be/SINlygW1Mpc
- Link to download the book free: https://nephrotube.blogspot.com/p/nephrotube-nephrology-books.html
- Link to NephroTube website: www.NephroTube.com
- Link to NephroTube social media accounts: https://nephrotube.blogspot.com/p/join-nephrotube-on-social-media.html
263778731218 Abortion Clinic /Pills In Harare ,sisternakatoto
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These lecture slides, by Dr Sidra Arshad, offer a quick overview of the physiological basis of a normal electrocardiogram.
Learning objectives:
1. Define an electrocardiogram (ECG) and electrocardiography
2. Describe how dipoles generated by the heart produce the waveforms of the ECG
3. Describe the components of a normal electrocardiogram of a typical bipolar lead (limb II)
4. Differentiate between intervals and segments
5. Enlist some common indications for obtaining an ECG
6. Describe the flow of current around the heart during the cardiac cycle
7. Discuss the placement and polarity of the leads of electrocardiograph
8. Describe the normal electrocardiograms recorded from the limb leads and explain the physiological basis of the different records that are obtained
9. Define mean electrical vector (axis) of the heart and give the normal range
10. Define the mean QRS vector
11. Describe the axes of leads (hexagonal reference system)
12. Comprehend the vectorial analysis of the normal ECG
13. Determine the mean electrical axis of the ventricular QRS and appreciate the mean axis deviation
14. Explain the concepts of current of injury, J point, and their significance
Study Resources:
1. Chapter 11, Guyton and Hall Textbook of Medical Physiology, 14th edition
2. Chapter 9, Human Physiology - From Cells to Systems, Lauralee Sherwood, 9th edition
3. Chapter 29, Ganong’s Review of Medical Physiology, 26th edition
4. Electrocardiogram, StatPearls - https://www.ncbi.nlm.nih.gov/books/NBK549803/
5. ECG in Medical Practice by ABM Abdullah, 4th edition
6. Chapter 3, Cardiology Explained, https://www.ncbi.nlm.nih.gov/books/NBK2214/
7. ECG Basics, http://www.nataliescasebook.com/tag/e-c-g-basics
New Drug Discovery and Development .....NEHA GUPTA
The "New Drug Discovery and Development" process involves the identification, design, testing, and manufacturing of novel pharmaceutical compounds with the aim of introducing new and improved treatments for various medical conditions. This comprehensive endeavor encompasses various stages, including target identification, preclinical studies, clinical trials, regulatory approval, and post-market surveillance. It involves multidisciplinary collaboration among scientists, researchers, clinicians, regulatory experts, and pharmaceutical companies to bring innovative therapies to market and address unmet medical needs.
Local Advanced Lung Cancer: Artificial Intelligence, Synergetics, Complex Sys...Oleg Kshivets
Overall life span (LS) was 1671.7±1721.6 days and cumulative 5YS reached 62.4%, 10 years – 50.4%, 20 years – 44.6%. 94 LCP lived more than 5 years without cancer (LS=2958.6±1723.6 days), 22 – more than 10 years (LS=5571±1841.8 days). 67 LCP died because of LC (LS=471.9±344 days). AT significantly improved 5YS (68% vs. 53.7%) (P=0.028 by log-rank test). Cox modeling displayed that 5YS of LCP significantly depended on: N0-N12, T3-4, blood cell circuit, cell ratio factors (ratio between cancer cells-CC and blood cells subpopulations), LC cell dynamics, recalcification time, heparin tolerance, prothrombin index, protein, AT, procedure type (P=0.000-0.031). Neural networks, genetic algorithm selection and bootstrap simulation revealed relationships between 5YS and N0-12 (rank=1), thrombocytes/CC (rank=2), segmented neutrophils/CC (3), eosinophils/CC (4), erythrocytes/CC (5), healthy cells/CC (6), lymphocytes/CC (7), stick neutrophils/CC (8), leucocytes/CC (9), monocytes/CC (10). Correct prediction of 5YS was 100% by neural networks computing (error=0.000; area under ROC curve=1.0).
Knee anatomy and clinical tests 2024.pdfvimalpl1234
This includes all relevant anatomy and clinical tests compiled from standard textbooks, Campbell,netter etc..It is comprehensive and best suited for orthopaedicians and orthopaedic residents.
1. C it Th
Cavity Theory,
Stopping-Power Ratios,
pp g
Correction Factors.
Alan E. Nahum PhD
Physics Department
Physics Department
Clatterbridge Centre for Oncology
Bebington, Wirral CH63 4JY UK
(alan.nahum@ccotrust.nhs.uk)
( @ )
AAPM Summer School, CLINICAL DOSIMETRY FOR RADIOTHERAPY,
21-25 June 2009, Colorado College, Colorado Springs, USA 1
2. 3 1 INTRODUCTION
A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
3.1 INTRODUCTION
3.2 “LARGE” PHOTON DETECTORS
3.3 BRAGG-GRAY CAVITY THEORY
3.4 STOPPING-POWER RATIOS
3.5 THICK-WALLED ION CHAMBERS
3 6 CORRECTION OR PERTURBATION FACTORS
3.6 CORRECTION OR PERTURBATION FACTORS
FOR ION CHAMBERS
3 7 GENERAL CAVITY THEORY
3.7 GENERAL CAVITY THEORY
3.8 PRACTICAL DETECTORS
2
3.9 SUMMARY
3. Accurate knowledge of the (patient) dose
A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
g (p )
in radiation therapy is crucial to clinical
outcome
For a given fraction size
(%)
80
100 TCP
&
NTCP
40
60
C
Therapeutic Ratio
TCP
0
20
NTCP
Dose (Gy)
20 40 60 80 100
0
Dpr
3
4. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
Detectors almost never measure dose to
medium directly.
Therefore the interpretation of detector reading
Therefore, the interpretation of detector reading
requires dosimetry theory - “cavity theory”
4
5. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
med
Q
D
f
especially when converting
from calibration at Q to
Q
det
med
Q
D
f
5
from calibration at Q1 to
measurement at Q2
6. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
Also the “physics” of depth-dose curves:
Also the physics of depth-dose curves:
6
7. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
Dose computation in a TPS
Dose computation in a TPS
Terma
f K
cf. Kerma
7
8. First we will remind ourselves of two key results which relate
the particle fluence, , to energy deposition in the medium.
Under charged-particle equilibrium (CPE) conditions, the
absorbed dose in the medium, Dmed, is related to the photon
(energy) fluence in the medium, h med , by
en
CPE
h
Φ
K
D
med
en
med
med
c
med h
Φ
K
D
for monoenergetic photons of energy h and by
for monoenergetic photons of energy h, and by
dh
)
h
(
d en
med
CPE max
Φ
h
D
h
dh
)
(
dh med
en
med
0
med
h
D
for a spectrum of photon energies where ( /) d is the
8
for a spectrum of photon energies, where (en/)med is the
mass-energy absorption coefficient for the medium in question.
9. For charged particles the corresponding expressions are:
col
med
.
eqm
δ
med
S
Φ
D
med
where (Scol/)med is the (unrestricted) electron mass
collision stopping po er for the medi m
and for a spectrum of electron energies:
collision stopping power for the medium.
E
E
S
Φ
D
E
d
)
(
d col
med
.
eqm
δ
d
max
E
E
D d
d med
0
med
Note that in the charged particle case the requirement
9
Note that in the charged-particle case the requirement
is:
–ray equilibrium
10. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
“Photon” Detectors
DETECTOR
MEDIUM
DETECTOR
en
CPE
h
Φ
K
D
10
det
en
med
det
c
det h
Φ
K
D
11. Thus for the “photon” detector:
CPE
det
en
det
CPE
det
D
and for the medium:
det
en
med
CPE
med
D
med
and therefore we can write:
med
en
,
med
CPE
,
med
/
/
Q
Ψ
Ψ
D
f z
z
11
det
en
det
det /
Q
Ψ
D
f
12. The key assumption is now made that the photon energy
fluence in the detector is negligibly different from that
t i th di t b d di t th iti f th
present in the undisturbed medium at the position of the
detector i.e. det = med,z and thus:
d
d /
D
det
en
med
en
det
,
med
/
/
Q
D
D
f z
which is the well known / ratio usually written as
which is the well-known en/ -ratio usually written as
med
en
Q
f
det
Q
f
and finally for a spectrum of photon energies:
y p p g
E
E
E
Φ
E en
E
z
d
)
(
d
d
med
0
,
med
h
med
en
max
12
E
E
E
Φ
E en
E
z
d
)
(
d
d
det
0
,
med
h
det
max
13. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
The dependence of the en/ -ratio on
photon energy for water/medium
13
14. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
14
“Electron” detectors (Bragg-Gray)
15. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
15
16. BRAGG-GRAY
C O
CAVITY THEORY
We have seen that in the case of detectors with sensitive volumes large enough for the
t bli h t f CPE th ti D /D i i b ( / ) f th f i di tl
establishment of CPE, the ratio Dmed/Ddet is given by (en/)med,det for the case of indirectly
ionizing radiation. In the case of charged particles one requires an analogous relation in terms
of stopping powers. If we assume that the electron fluences in the detector and at the same
depth in the medium are given by det and med respectively then according to Equ 43 we
depth in the medium are given by det and med respectively, then according to Equ. 43 we
must be able to write
D S
med med col med
( / )
D
D
S
S
med med col med
col
det det det
( / )
( / )
(45)
18. For the more practical case of a spectrum of electron energies, the stopping-power ratio
must be evaluated from
must be evaluated from
D
S E E
E
E
col med d
max
( ( ) / )
D
D
S E E
E
E
col
med o
d
det
det
max
( ( ) / )
(48)
o
where the energy dependence of the stopping powers have been made explicit and it is
understood that E refers to the undisturbed medium in both the numerator and the
denominator. It must be stressed that this is the fluence of primary electrons only; no delta
rays are involved (see next section). For reasons that will become apparent in the next
paragraph, it is convenient to denote the stopping-power ratio evaluated according to Equ.
48 by sBG
d d t [12]
48 by s med,det [12].
20. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
The Spencer-Attix “solution”
medium
gas
gas
E
D
L E E S
E
E
E col
E
med
med med
d
max
( ( ) / ) ( )( ( ) / )
20
D
L E E S
E
E
E col
d
det
det det
max
( ( ) / ) ( )( ( ) / )
21. In the previous section we have neglected the question of delta-ray equilibrium, which is a
pre-requisite for the strict validity of the stopping-power ratio as evaluated in Equ. 43. The
original Bragg-Gray theory effectively assumed that all collision losses resulted in energy
original Bragg Gray theory effectively assumed that all collision losses resulted in energy
deposition within the cavity. Spencer and Attix proposed an extension of the Bragg-Gray
idea that took account, in an approximate manner, of the effect of the finite ranges of the
delta rays [11]. All the electrons above a cutoff energy , whether primary or delta rays,
id d b f h fl i id h i All
were now considered to be part of the fluence spectrum incident on the cavity. All energy
losses below in energy were assumed to be local to the cavity and all losses above were
assumed to escape entirely. The local energy loss was calculated by using the collision
stopping power restricted to losses less than , L (see lecture 3). This 2-component model
stopping power restricted to losses less than , L (see lecture 3). This 2 component model
leads to a stopping-power ratio given by [12,13]:
Emax
E
med
col
tot
E
med
med
tot
E
med S
E
E
L
E
L
/
)
(
)
(
d
/
)
(
)
(
max
max
gas
col
tot
E
gas
med
tot
E
gas
S
E
E
L
E
/
)
(
)
(
d
/
)
(
)
(
a
22. BRAGG-GRAY CAVITY
Th S i P R i
E
E
S
E
d
)
/
)
(
(
max
The Stopping-Power Ratio smed, det :
E
E
S
E
E
S
D
D
E
col
E
d
)
/
)
(
(
d
)
/
)
(
( med
o
det
med
max
E
E
Scol
E d
)
/
)
(
( det
o
det
The Spencer-Attix formulation:
med
med
d
)
/
)
(
)(
(
d
)
/
)
(
(
max
col
E
E
E S
E
E
L
D
The Spencer Attix formulation:
det
det
det
med
)
/
)
(
)(
(
d
)
/
)
(
(
max
col
E
E
E S
E
E
L
D
D
23. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
When is a cavity “Bragg-Gray?
In order for a detector to be treated as a
Bragg–Gray (B–G) cavity there is really only
y gg y
gg y ( ) y y y
one condition which must be fulfilled:
– The cavity must not disturb the charged particle
The cavity must not disturb the charged particle
fluence (including its distribution in energy) existing
in the medium in the absence of the cavity.
In practice this means that the cavity must
be small compared to the electron ranges,
p g ,
and in the case of photon beams, only gas-
filled cavities, i.e. ionisation chambers, fulfil
, ,
this. 23
24. A second condition is generally added:
A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
A second condition is generally added:
The absorbed dose in the cavity is deposited
ti l b th h d ti l i it
entirely by the charged particles crossing it.
This implies that any contribution to the dose due to
photon interactions in the cavity must be negligible.
Essentially it is a corollary to the first condition. If the cavity
is small enough to fulfil the first condition then the build-up
g p
of dose due to interactions in the cavity material itself must
be negligible; if this is not the case then the charged
particle fluence will differ from that in the undisturbed
particle fluence will differ from that in the undisturbed
medium for this very reason.
24
25. A third condition is sometimes erroneously
added:
Charged Particle Equilibrium must exist in the
absence of the cavity.
Greening (1981) wrote that Gray’s original theory required this.
g ( ) y g y q
In fact, this “condition” is incorrect but there are historical
reasons for finding it in old publications.
CPE is not required but what is required, however, is that the
stopping-power ratio be evaluated over the charged-particle (i.e.
electron) spectrum in the medium at the position of the detector.
electron) spectrum in the medium at the position of the detector.
Gray and other early workers invoked this CPE condition
because they did not have the theoretical tools to evaluate the
25
because they did not have the theoretical tools to evaluate the
electron fluence spectrum (E in the above expressions) unless
there was CPE. (but today we can do this using MC methods).
26. Do air-filled ionisation chambers function as Bragg-Gray
Do air filled ionisation chambers function as Bragg Gray
cavities at KILOVOLTAGE X-ray qualities?
26
27. Ma C-M and Nahum AE 1991 Bragg-Gray theory and ion chamber dosimetry for photon
beams Phys. Med. Biol. 36 413-428
28. The commonly used air-filled ionization chamber irradiated by a megavoltage photon beam
is the clearest case of a Bragg-Gray cavity. However for typical ion chamber dimensions for
kilovoltage x-ray beams, the percentage of the dose to the air in the cavity due to photon
interactions in the air is far from negligible as the Table, taken from [9], demonstrates:
29. Ma C-M and Nahum AE 1991 Bragg-Gray theory and ion chamber dosimetry for photon
beams Phys. Med. Biol. 36 413-428
30. 3 1 INTRODUCTION
A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
3.1 INTRODUCTION
3.2 “LARGE” PHOTON DETECTORS
3.3 BRAGG-GRAY CAVITY THEORY
3.4 STOPPING-POWER RATIOS
3.5 THICK-WALLED ION CHAMBERS
3 6 CORRECTION OR PERTURBATION FACTORS
3.6 CORRECTION OR PERTURBATION FACTORS
FOR ION CHAMBERS
3 7 GENERAL CAVITY THEORY
3.7 GENERAL CAVITY THEORY
3.8 PRACTICAL DETECTORS
30
3.9 SUMMARY
34. Depth variation of the Spencer-Attix water/air stopping-power
ratio, sw,air, for =10 keV, derived from Monte Carlo generated
l t t f ti l ll l b d
electron spectra for monoenergetic, plane-parallel, broad
electron beams (Andreo (1990); IAEA (1997b)).
1 10
1.15
electron energy (MeV)
30
25
20
18
14
10
7
5
1 3
ir
1.05
1.10
50
40
30
r
ratio,
s
w,a
1.00
ing-power
0.95
stoppi
0 4 8 12 16 20 24
0.90
depth in water (cm)
37. “THICK-WALLED” ION CHAMBERS
A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
med
en
D
D
)
C
(
)
C
(
CPE
wall
Δ
L
D
D
)
C
(
)
C
(
&
37
wall
wall
med D
D
)
C
(
)
C
(
air
Δ
air
wall D
D
)
C
(
)
C
(
&
38. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
med
en
wall
Δ
med L
D
Q
f
)
C
(
wall
air
air
D
Q
f
)
C
(
Thick-walled cavity chamber free-in-air
where the air volume is known precisely
where the air volume is known precisely
(Primary Standards Laboratories):
'
)
( K
L
D
C
K
air
en
wall
air
i
38
1
)
( K
g
C
K
wall
air
air
air
39. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
CORRECTION FACTORS
FOR ION CHAMBERS
FOR ION CHAMBERS
(measurements in phantom)
( p )
39
40. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
Are real practical Ion Chambers
Are real, practical Ion Chambers
really Bragg-Gray cavities?
y gg y
40
41. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
i
med
air
Δ
air
C
med P
L
D
Q
D
/
,
i
,
d
stem
cel
wall
repl
med
air
Δ
air
C
med P
P
P
P
L
D
Q
D
/
,
41
FARMER chamber (distances in millimetres)
42. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
THE EFFECT OF THE CHAMBER WALL
42
43. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
43
44. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
The Almond-Svensson (1977) expression:
med
wall
med
1
Δ
Δ
en L
L
med
air
air
wall
wall
Δ
L
P
44
air
Δ
45. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
45
46. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
46
47. THE EFFECT OF THE FINITE VOLUME
OF THE GAS CAVITY
A. E. Nahum: Cavity Theory,
Stopping-Power Ratios, Correction
Factors
47
48. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
48
49. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
49
50. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
FLUENCE PERTURBATION?
FLUENCE PERTURBATION?
Electrons
50
51. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
P
Φ
Φ P
z
E
fl
cav
med P
Φ
Φ
eff
P
Johansson et al used chambers of 3, 5 and 7-mm
radius and found an approximately linear relation
between (1 P ) and cavity radius (at a given energy)
between (1- Pfl) and cavity radius (at a given energy).
Summarising the experimental work by the
Wittkämper, Johansson and colleagues, for the
NE2571 li d i l h b P i
E E
z
E
NE2571 cylindrical chamber Pfl increases
steadily from ≈ 0.955 at = 2 MeV, to ≈ 0.980
at = 10 MeV and to ≈ 0 997 at = 20 MeV
51
z
E z
E
at = 10 MeV, and to ≈ 0.997 at = 20 MeV.
52. A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors.
52
53. GENERAL CAVITY THEORY
We have so far looked at two extreme cases:
i) detectors which are large compared to the electron
i) detectors which are large compared to the electron
ranges in which CPE is established (photon radiation only)
ii) d t t hi h ll d t th l t
ii) detectors which are small compared to the electron
ranges and which do not disturb the electron fluence (Bragg-
Gray cavities)
Many situations involve measuring the dose from photon (or
neutron) radiation using detectors which fall into neither of the
neutron) radiation using detectors which fall into neither of the
above categories. In such cases there is no exact theory.
However, so-called General Cavity Theory has been
developed as an approximation
developed as an approximation.
54. In essence these theories yield a factor which is a weighted
f
mean of the stopping-power ratio and the mass-energy
absorption coefficient ratio:
det
det
det
det
det
1
en
Δ
d
L
d
D
D
med
med
med
D
where d is the fraction of the dose in the cavity due to
electrons from the medium (Bragg-Gray part),
and (1 - d) is the fraction of the dose from photon
interactions in the cavity (“large cavity”/photon detector
part)
part)