Stereotactic Radiosurgery for Pituitary Tumors
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4. Particle Generators/Accelerators
Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing 4. Particle Generators/Accelerators Diana Adlienė Department of Physics Kaunas University of Technolog y Joint innovative training and teaching/ learning program in enhancing development and transfer knowledge of application of ionizing radiation in materials processing This project has been funded with support from the European Commission. This publication reflects the views only of the author. Polish National Agency and the Commission cannot be held responsible for any use which may be made of the information contained therein. Date: Oct. 2017 DISCLAIMER This presentation contains some information addapted from open access education and training materials provided by IAEA TABLE OF CONTENTS 1. Introduction 2. X-ray machines 3. Particle generators/accelerators 4. Types of industrial irradiators The best accelerator in the universe… INTRODUCTION • Naturally occurring radioactive sources: – Up to 5 MeV Alpha’s (helium nuclei) – Up to 3 MeV Beta particles (electrons) • Natural sources are difficult to maintain, their applications are limited: – Chemical processing: purity, messy, and expensive; – Low intensity; – Poor geometry; – Uncontrolled energies, usually very broad Artificial sources (beams) are requested! INTRODUCTION • Beams of accelerated particles can be used to produce beams of secondary particles: Photons (x-rays, gamma-rays, visible light) are generated from beams -
Installation of the Cyclotron Based Clinical Neutron Therapy System in Seattle
Proceedings of the Tenth International Conference on Cyclotrons and their Applications, East Lansing, Michigan, USA INSTALLATION OF THE CYCLOTRON BASED CLINICAL NEUTRON THERAPY SYSTEM IN SEATTLE R. Risler, J. Eenmaa, J. Jacky, I. Kalet, and P. Wootton Medical Radiation Physics RC-08, University of Washington, Seattle ~ 98195, USA S. Lindbaeck Instrument AB Scanditronix, Uppsala, Sweden Sumnary radiation areas is via sliding shielding doors rather than a maze, mai nl y to save space. For the same reason A cyclotron facility has been built for cancer a single door is used to alternately close one or the treatment with fast neutrons. 50.5 MeV protons from a other therapy room. All power supplies and the control conventional, positive ion cyclotron are used to b0m computer are located on the second floor, above the bard a semi-thick Beryllium target located 150 am from maintenance area. The cooler room contains a heat the treatment site. Two treatment rooms are available, exchanger and other refrigeration equipment. Not shown one with a fixed horizontal beam and one with an iso in the diagram is the cooling tower located in another centric gantry capable of 360 degree rotation. In part of the building. Also not shown is the hot lab addition 33 51 MeV protons and 16.5 - 25.5 MeV now under construction an an area adjacent to the deuterons are generated for isotope production inside cyclotron vault. It will be used to process radio the cyclotron vault. The control computer is also used isotopes produced at a target station in the vault. to record and verify treatment parameters for indi vidual patients and to set up and monitor the actual radiation treatment. -
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons
22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering at the Massachusetts Institute of Technology June 2007 © 2007 Leslie Dewan All rights reserved The author hereby grants to MIT permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part in any medium now known or hereafter created. Signature of Author: Leslie Dewan Department of Nuclear Science and Engineering May 16, 2007 Certified by: David G. Cory Professor of Nuclear Science and Engineering Thesis Supervisor Accepted by: David G. Cory Professor of Nuclear Science and Engineering Chairman, NSE Committee for Undergraduate Students Leslie Dewan 1 of 23 5/16/07 22 Thesis Cyclotron Design and Construction Design and Construction of a Cyclotron Capable of Accelerating Protons to 2 MeV by Leslie Dewan Submitted to the Department of Nuclear Science and Engineering on May 16, 2007 in Partial Fulfillment of the Requirements for the Degree of Bachelor of Science in Nuclear Science and Engineering ABSTRACT This thesis describes the design and construction of a cyclotron capable of accelerating protons to 2 MeV. A cyclotron is a charged particle accelerator that uses a magnetic field to confine particles to a spiral flight path in a vacuum chamber. An applied electrical field accelerates these particles to high energies, typically on the order of mega-electron volts. -
Cyclotrons: Old but Still New
Cyclotrons: Old but Still New The history of accelerators is a history of inventions William A. Barletta Director, US Particle Accelerator School Dept. of Physics, MIT Economics Faculty, University of Ljubljana US Particle Accelerator School ~ 650 cyclotrons operating round the world Radioisotope production >$600M annually Proton beam radiation therapy ~30 machines Nuclear physics research Nuclear structure, unstable isotopes,etc High-energy physics research? DAEδALUS Cyclotrons are big business US Particle Accelerator School Cyclotrons start with the ion linac (Wiederoe) Vrf Vrf Phase shift between tubes is 180o As the ions increase their velocity, drift tubes must get longer 1 v 1 "c 1 Ldrift = = = "# rf 2 f rf 2 f rf 2 Etot = Ngap•Vrf ==> High energy implies large size US Particle Accelerator School ! To make it smaller, Let’s curl up the Wiederoe linac… Bend the drift tubes Connect equipotentials Eliminate excess Cu Supply magnetic field to bend beam 1 2# mc $ 2# mc " rev = = % = const. frf eZion B eZion B Orbits are isochronous, independent of energy ! US Particle Accelerator School … and we have Lawrence’s* cyclotron The electrodes are excited at a fixed frequency (rf-voltage source) Particles remain in resonance throughout acceleration A new bunch can be accelerated on every rf-voltage peak: ===> “continuous-wave (cw) operation” Lawrence, E.O. and Sloan, D.: Proc. Nat. Ac. Sc., 17, 64 (1931) Lawrence, E.O. & Livingstone M.S.: Phys. Rev 37, 1707 (1931). * The first cyclotron patent (German) was filed in 1929 by Leó Szilard but never published in a journal US Particle Accelerator School Synchronism only requires that τrev = N/frf “Isochronous” particles take the same revolution time for each turn. -
CURIUM Element Symbol: Cm Atomic Number: 96
CURIUM Element Symbol: Cm Atomic Number: 96 An initiative of IYC 2011 brought to you by the RACI ROBYN SILK www.raci.org.au CURIUM Element symbol: Cm Atomic number: 96 Curium is a radioactive metallic element of the actinide series, and named after Marie Skłodowska-Curie and her husband Pierre, who are noted for the discovery of Radium. Curium was the first element to be named after a historical person. Curium is a synthetic chemical element, first synthesized in 1944 by Glenn T. Seaborg, Ralph A. James, and Albert Ghiorso at the University of California, Berkeley, and then formally identified by the same research tea at the wartime Metallurgical Laboratory (now Argonne National Laboratory) at the University of Chicago. The discovery of Curium was closely related to the Manhattan Project, and thus results were kept confidential until after the end of World War II. Seaborg finally announced the discovery of Curium (and Americium) in November 1945 on ‘The Quiz Kids!’, a children’s radio show, five days before an official presentation at an American Chemical Society meeting. The first radioactive isotope of Curium discovered was Curium-242, which was made by bombarding alpha particles onto a Plutonium-239 target in a 60-inch cyclotron (University of California, Berkeley). Nineteen radioactive isotopes of Curium have now been characterized, ranging in atomic mass from 233 to 252. The most stable radioactive isotopes are Curium- 247 with a half-life of 15.6 million years, Curium-248 (half-life 340,000 years), Curium-250 (half-life of 9000 years), and Curium-245 (half-life of 8500 years). -
Cyclotron Basics
Unit 10 - Lectures 14 Cyclotron Basics MIT 8.277/6.808 Intro to Particle Accelerators Timothy A. Antaya Principal Investigator MIT Plasma Science and Fusion Center [email protected] / (617) 253-8155 1 Outline Introduce an important class of circular particle accelerators: Cyclotrons and Synchrocyclotrons Identify the key characteristics and performance of each type of cyclotron and discuss their primary applications Discuss the current status of an advance in both the science and engineering of these accelerators, including operation at high magnetic field Overall aim: reach a point where it will be possible for to work a practical exercise in which you will determine the properties of a prototype high field cyclotron design (next lecture) [email protected] / (617) 253-8155 2 Motion in a magnetic field [email protected] / (617) 253-8155 3 Magnetic forces are perpendicular to the B field and the motion [email protected] / (617) 253-8155 4 Sideways force must also be Centripedal [email protected] / (617) 253-8155 5 Governing Relation in Cyclotrons A charge q, in a uniform magnetic field B at radius r, and having tangential velocity v, sees a centripetal force at right angles to the direction of motion: mv2 r rˆ = qvr ! B r The angular frequency of rotation seems to be independent of velocity: ! = qB / m [email protected] / (617) 253-8155 6 Building an accelerator using cyclotron resonance condition A flat pole H-magnet electromagnet is sufficient to generate require magnetic field Synchronized electric fields can be used to raise -
Hyperprolactinaemia: a Monster Between the Woman and Her Conception *Seriki A
Archives of Reproductive Medicine and Sexual Health ISSN: 2639-1791 Volume 1, Issue 2, 2018, PP: 61-67 Hyperprolactinaemia: A Monster Between the Woman and Her Conception *Seriki A. Samuel1, Odetola O. Anthony2 1Department of Human Physiology, College of Medicine, Bingham University, Karu, Nigeria. 2Department of Human Physiology, College Medical Sciences, NnamdiAzikwe University, Awka, Nigeria. [email protected] *Corresponding Author: Seriki A. Samuel, Department of Human Physiology, College of Medicine, Bingham University, Karu, Nigeria. Abstract Hyperprolactinaemia is the presence of abnormally high levels of prolactin in the blood. Normal levels are less than 5000 ml U/L [20ng/mL or µg/L] for women, and less than 450 ml U/L for men.Prolactin is a peptide hormone produced by the adenohypophysis (also called anterior pituitary) that is primarily associated with milk production and plays a vital role in breast development during pregnancy. Hyperprolactinaemia may cause galactorrhea (production and sp; ontaneous ejection of breast milk without pregnancy or childbirth). It also alters/disrupts the normal menstrual cycle in women. In other women, menstruation may cease completely, resulting in infertility. In the man, it could causeerectile dysfunction.The present study is to review the pathophysiology of the abnormality in the woman, and how it relates to the functioning of the hypothalamo- hypophyseal-gonadal system. The article also looks at the effect of hyperprolactinaemia on the fertility of the woman, and attempts to proffer non-surgical remedy to the condition. Keywords: Galactorrhea, adenohypophysis,hypoestrogenism,prolactinoma, amenorrhoea, macroprolactin, microprolactin Introduction It is synthesized by the anterior pituitary lactotrophs and regulated by the hypothalamic–pituitary axis Hyperprolactinaemia, which is a high level of through the release of dopamine, which acts as a prolactin in the blood can be a part of normal prolactin inhibitory factor[2]. -
Electrostatic Particle Accelerators the Cyclotron Linear Particle Accelerators the Synchrotron +
Uses: Mass Spectrometry Uses Overview Uses: Hadron Therapy This is a technique in analytical chemistry. Ionising particles such as protons are fired into the It allows the identification of chemicals by ionising them body. They are aimed at cancerous tissue. and measuring the mass to charge ratio of each ion type Most methods like this irradiate the surrounding tissue too, against relative abundance. but protons release most of their energy at the end of their It also allows the relative atomic mass of different elements travel. (see graphs) be measured by comparing the relative abundance of the This allows the cancer cells to be targeted more precisely, with ions of different isotopes of the element. less damage to surrounding tissue. An example mass spectrum is shown below: Linear Particle Accelerators Electrostatic Particle Accelerators These are still in a straight line, but now the voltage is no longer static - it is oscillating. An electrostatic voltageis provided at one end of a vacuum tube. This means the voltage is changing - so if it were a magnet, it would be first positive, then This is like the charge on a magnet. negative. At the other end of the tube, there are particles Like the electrostatic accelerator, a charged particle is attracted to it as the charges are opposite, but just with the opposite charge. as the particle goes past the voltage changes, and the charge of the plate swaps (so it is now the same charge Like north and south poles on a magnet, the opposite charges as the particle). attract and the particle is pulled towards the voltage. -
Patent Application Publication ( 10 ) Pub . No . : US 2019 / 0192440 A1
US 20190192440A1 (19 ) United States (12 ) Patent Application Publication ( 10) Pub . No. : US 2019 /0192440 A1 LI (43 ) Pub . Date : Jun . 27 , 2019 ( 54 ) ORAL DRUG DOSAGE FORM COMPRISING Publication Classification DRUG IN THE FORM OF NANOPARTICLES (51 ) Int . CI. A61K 9 / 20 (2006 .01 ) ( 71 ) Applicant: Triastek , Inc. , Nanjing ( CN ) A61K 9 /00 ( 2006 . 01) A61K 31/ 192 ( 2006 .01 ) (72 ) Inventor : Xiaoling LI , Dublin , CA (US ) A61K 9 / 24 ( 2006 .01 ) ( 52 ) U . S . CI. ( 21 ) Appl. No. : 16 /289 ,499 CPC . .. .. A61K 9 /2031 (2013 . 01 ) ; A61K 9 /0065 ( 22 ) Filed : Feb . 28 , 2019 (2013 .01 ) ; A61K 9 / 209 ( 2013 .01 ) ; A61K 9 /2027 ( 2013 .01 ) ; A61K 31/ 192 ( 2013. 01 ) ; Related U . S . Application Data A61K 9 /2072 ( 2013 .01 ) (63 ) Continuation of application No. 16 /028 ,305 , filed on Jul. 5 , 2018 , now Pat . No . 10 , 258 ,575 , which is a (57 ) ABSTRACT continuation of application No . 15 / 173 ,596 , filed on The present disclosure provides a stable solid pharmaceuti Jun . 3 , 2016 . cal dosage form for oral administration . The dosage form (60 ) Provisional application No . 62 /313 ,092 , filed on Mar. includes a substrate that forms at least one compartment and 24 , 2016 , provisional application No . 62 / 296 , 087 , a drug content loaded into the compartment. The dosage filed on Feb . 17 , 2016 , provisional application No . form is so designed that the active pharmaceutical ingredient 62 / 170, 645 , filed on Jun . 3 , 2015 . of the drug content is released in a controlled manner. Patent Application Publication Jun . 27 , 2019 Sheet 1 of 20 US 2019 /0192440 A1 FIG . -
Particle Accelerators
Particle Accelerators By Stephen Lucas The subatomic Shakespeare of St.Neots Purposes of this presentation… To be able to explain how different particle accelerators work. To be able to explain the role of magnetic fields in particle accelerators. How the magnetic force provides the centripetal force in particle accelerators. Why have particle accelerators? They enable similarly charged particles to get close to each other - e.g. Rutherford blasted alpha particles at a thin piece of gold foil, in order to get the positively charged alpha particle near to the nucleus of a gold atom, high energies were needed to overcome the electrostatic force of repulsion. The more energy given to particles, the shorter their de Broglie wavelength (λ = h/mv), therefore the greater the detail that can be investigated using them as a probe e.g. – at the Stanford Linear Accelerator, electrons were accelerated to high energies and smashed into protons and neutrons revealing charge concentrated at three points – quarks. Colliding particles together, the energy is re-distributed producing new particles. The higher the collision energy the larger the mass of the particles that can be produced. E = mc2 The types of particle accelerator Linear Accelerators or a LINAC Cyclotron Synchrotron Basic Principles All accelerators are based on the same principle. A charged particle accelerates between a gap between two electrodes when there is a potential difference between them. Energy transferred, Ek = Charge, C x p.d, V Joules (J) Coulombs (C) Volts (V) Ek = QV Converting to electron volts 1 eV is the energy transferred to an electron when it moves through a potential difference of 1V. -
Guidance on the Treatment of Antipsychotic Induced Hyperprolactinaemia in Adults
Guidance on the Treatment of Antipsychotic Induced Hyperprolactinaemia in Adults Version 1 GUIDELINE NO RATIFYING COMMITTEE DRUGS AND THERAPEUTICS GROUP DATE RATIFIED April 2014 DATE AVAILABLE ON INTRANET NEXT REVIEW DATE April 2016 POLICY AUTHORS Nana Tomova, Clinical Pharmacist Dr Richard Whale, Consultant Psychiatrist In association with: Dr Gordon Caldwell, Consultant Physician, WSHT . If you require this document in an alternative format, ie easy read, large text, audio, Braille or a community language, please contact the Pharmacy Team on 01243 623349 (Text Relay calls welcome). Contents Section Title Page Number 1. Introduction 2 2. Causes of Hyperprolactinaemia 2 3. Antipsychotics Associated with 3 Hyperprolactinaemia 4. Effects of Hyperprolactinaemia 4 5. Long-term Complications of Hyperprolactinaemia 4 5.1 Sexual Development in Adolescents 4 5.2 Osteoporosis 4 5.3 Breast Cancer 5 6. Monitoring & Baseline Prolactin Levels 5 7. Management of Hyperprolactinaemia 6 8. Pharmacological Treatment of 7 Hyperprolactinaemia 8.1 Aripiprazole 7 8.2 Dopamine Agonists 8 8.3 Oestrogen and Testosterone 9 8.4 Herbal Remedies 9 9. References 10 1 1.0 Introduction Prolactin is a hormone which is secreted from the lactotroph cells in the anterior pituitary gland under the influence of dopamine, which exerts an inhibitory effect on prolactin secretion1. A reduction in dopaminergic input to the lactotroph cells results in a rapid increase in prolactin secretion. Such a reduction in dopamine can occur through the administration of antipsychotics which act on dopamine receptors (specifically D2) in the tuberoinfundibular pathway of the brain2. The administration of antipsychotic medication is responsible for the high prevalence of hyperprolactinaemia in people with severe mental illness1. -
Plutonium (Pu) Fact Sheet
Plutonium (Pu) November 2002 Fact Sheet 320-080 Division of Environmental Health Office of Radiation Protection WHO DISCOVERED PLUTONIUM? Plutonium was first produced by Glenn T. Seaborg, Joseph W. Kennedy, Edward M. McMillan and Arthur C. W ohl by bombarding an isotope of uranium, uranium-238, with deuterons that had been accelerated in a device called a cyclotron. This created neptunium-238 and two free neutrons. Neptunium-238 has a half-life of 2.1 days and decays into plutonium -238 through beta decay. Although they conducted their work at the University of California in 1941, their discovery was not revealed to the rest of the scientific community until 1946 because of wartime security concerns. Plutonium was the second transuranic elem ent of the actinide series to be discovered. By far of greatest importance is the isotope 239Pu, which has a half-life of more than 20,000 years. The complete detonation of a kilogram of plutonium produces an explosion equal to about 20,000 tons of chemical explosive. The isotope 238Pu was used in the American Apollo lunar missions to power seismic and other equipment on the lunar surface. WHAT IS PLUTONIUM USED FOR? Only two of plutonium's isotopes, plutonium-238 and plutonium-239, have found uses outside of basic research. Plutonium-238 is used in radioisotope thermoelectric generators to provide electricity for space probes that venture too far from the sun to use solar power, such as the Cassini and Galileo probes. It also provides the electricity source in implanted cardiac pacemakers, space satellites, and navigation beacons.