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Excitation Temperature, Degree of Ionization of Added Iron Species, and Electron Density in an Exploding Thin Film Plasma
SpectmchimiccrACIO. Vol. MB. No. II. Pp.10814096. 1981. 0584-8547/81/111081-16SIZ.CNI/O Printedin Great Britain. PerpmonPress Ltd. Excitation temperature, degree of ionization of added iron species, and electron density in an exploding thin film plasma S. Y. SUH* and R. D. SACKS Department of Chemistry, University of Michigan, Ann Arbor, Ml 48109, U.S.A. (Received 7 April 1981) Abstract-Time and spatially resolved spectra of a cylindrically symmetric exploding thin film plasma were obtained with a rotating mirror camera and astigmatic imaging. These spectra were deconvoluted to obtain relative spectral emissivity profiles for nine Fe(H) and two Fe(I) lines. The effective (electronic) excitation temperature at various positions in the plasma and at various times during the first current halfcycle was computed from the Fe(H) emissivity values using the Boltzmann graphical method. The Fe(II)/Fe(I) emissivity ratios together with the temperature were used to determine the degree of ionization of Fe. Finally, the electron density was estimated from the Saha equilibrium. Electronic excitation temperatures range from lO,OOO-15,OOOKnear the electrode surface at peak discharge current to 700&10.000K at 6-10 mm above the electrode surface at the first current zero. Corresponding electron densities range from 10’7-10u cm-’ at peak current to 10’~-10’6cm-3 near zero current. Error propagation and criteria for thermodynamic equilibrium are discussed. 1. IN-~R~DU~~ION THE HIGH-TEMPERATURE plasmas produced by the rapid electrical vaporization of Ag thin films recently have been used as atomization cells and excitation sources for the direct determination of selected elements in micro-size powder samples [ 11. -
An Analytical Perspective on Determination of Free Base Nicotine in E-Liquids
Virginia Commonwealth University VCU Scholars Compass Pharmaceutics Publications Dept. of Pharmaceutics 2020 An Analytical Perspective on Determination of Free Base Nicotine in E-Liquids Vinit V. Gholap Virginia Commonwealth University Rodrigo S. Heyder Virginia Commonwealth University Leon Kosmider Medical University of Silesia Matthew S. Halquist Virginia Commonwealth University, [email protected] Follow this and additional works at: https://scholarscompass.vcu.edu/pceu_pubs Part of the Pharmacy and Pharmaceutical Sciences Commons Copyright © 2020 Vinit V. Gholap et al. -is is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited. Downloaded from https://scholarscompass.vcu.edu/pceu_pubs/19 This Article is brought to you for free and open access by the Dept. of Pharmaceutics at VCU Scholars Compass. It has been accepted for inclusion in Pharmaceutics Publications by an authorized administrator of VCU Scholars Compass. For more information, please contact [email protected]. Hindawi Journal of Analytical Methods in Chemistry Volume 2020, Article ID 6178570, 12 pages https://doi.org/10.1155/2020/6178570 Research Article An Analytical Perspective on Determination of Free Base Nicotine in E-Liquids Vinit V. Gholap ,1 Rodrigo S. Heyder,2 Leon Kosmider,3 and Matthew S. Halquist 1 1Department of Pharmaceutics, School of Pharmacy, Virginia Commonwealth University, Richmond 23298, VA, USA 2Department of Pharmaceutics, Pharmaceutical Engineering, School of Pharmacy, Virginia Commonwealth University, Richmond 23298, VA, USA 3Department of General and Inorganic Chemistry, Medical University of Silesia, Katowice FOPS in Sosnowiec, Jagiellonska 4, 41-200 Sosnowiec, Poland Correspondence should be addressed to Matthew S. -
Salts of Therapeutic Agents: Chemical, Physicochemical, and Biological Considerations
molecules Review Salts of Therapeutic Agents: Chemical, Physicochemical, and Biological Considerations Deepak Gupta 1, Deepak Bhatia 2 ID , Vivek Dave 3 ID , Vijaykumar Sutariya 4 and Sheeba Varghese Gupta 4,* 1 Department of Pharmaceutical Sciences, School of Pharmacy, Lake Erie College of Osteopathic Medicine, Bradenton, FL 34211, USA; [email protected] 2 ICPH Fairfax Bernard J. Dunn School of Pharmacy, Shenandoah University, Fairfax, VA 22031, USA; [email protected] 3 Wegmans School of Pharmacy, St. John Fisher College, Rochester, NY 14618, USA; [email protected] 4 Department of Pharmaceutical Sciences, USF College of Pharmacy, Tampa, FL 33612, USA; [email protected] * Correspondence: [email protected]; Tel.: +01-813-974-2635 Academic Editor: Peter Wipf Received: 7 June 2018; Accepted: 13 July 2018; Published: 14 July 2018 Abstract: The physicochemical and biological properties of active pharmaceutical ingredients (APIs) are greatly affected by their salt forms. The choice of a particular salt formulation is based on numerous factors such as API chemistry, intended dosage form, pharmacokinetics, and pharmacodynamics. The appropriate salt can improve the overall therapeutic and pharmaceutical effects of an API. However, the incorrect salt form can have the opposite effect, and can be quite detrimental for overall drug development. This review summarizes several criteria for choosing the appropriate salt forms, along with the effects of salt forms on the pharmaceutical properties of APIs. In addition to a comprehensive review of the selection criteria, this review also gives a brief historic perspective of the salt selection processes. Keywords: chemistry; salt; water solubility; routes of administration; physicochemical; stability; degradation 1. -
Ionization Balance in EBIT and Tokamak Plasmas N
Ionization balance in EBIT and tokamak plasmas N. J. Peacock, R. Barnsley, M. G. O’Mullane, M. R. Tarbutt, D. Crosby et al. Citation: Rev. Sci. Instrum. 72, 1250 (2001); doi: 10.1063/1.1324755 View online: http://dx.doi.org/10.1063/1.1324755 View Table of Contents: http://rsi.aip.org/resource/1/RSINAK/v72/i1 Published by the American Institute of Physics. Related Articles Bragg x-ray survey spectrometer for ITER Rev. Sci. Instrum. 83, 10E126 (2012) Novel energy resolving x-ray pinhole camera on Alcator C-Mod Rev. Sci. Instrum. 83, 10E526 (2012) Measurement of electron temperature of imploded capsules at the National Ignition Facility Rev. Sci. Instrum. 83, 10E121 (2012) South pole bang-time diagnostic on the National Ignition Facility (invited) Rev. Sci. Instrum. 83, 10E119 (2012) Temperature diagnostics of ECR plasma by measurement of electron bremsstrahlung Rev. Sci. Instrum. 83, 073111 (2012) Additional information on Rev. Sci. Instrum. Journal Homepage: http://rsi.aip.org Journal Information: http://rsi.aip.org/about/about_the_journal Top downloads: http://rsi.aip.org/features/most_downloaded Information for Authors: http://rsi.aip.org/authors Downloaded 08 Aug 2012 to 194.81.223.66. Redistribution subject to AIP license or copyright; see http://rsi.aip.org/about/rights_and_permissions REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 72, NUMBER 1 JANUARY 2001 Ionization balance in EBIT and tokamak plasmas N. J. Peacock,a) R. Barnsley,b) and M. G. O’Mullane Euratom/UKAEA Fusion Association, Culham Science Centre, Abingdon, Oxon OX14 3DB, United Kingdom M. R. Tarbutt, D. Crosby, and J. D. Silver The Clarendon Laboratory, University of Oxford, Parks Road, Oxford OX1 3PU, United Kingdom J. -
9.18.19 Didactic
STIMULANTS- PART I Michael H. Baumann, Ph.D. Designer Drug Research Unit (DDRU), Intramural Research Program, NIDA, NIH Baltimore, MD 21224 Chronology of Stimulant Misuse 1. 1980s: Cocaine 2. 1990s: Ecstasy 3. Summary 2 Topics Covered for Each Substance Chemistry Formulations and Methods of Use Pharmacokinetics and Metabolism Desired and Adverse Effects Chronic and Withdrawal Effects Neurobiology Treatments 1980s: Cocaine Cocaine, a Plant-Based Alkaloid Andean Cocaine is Trafficked Globally UNODC World Drug Report, 2012 Formulations and Methods of Use Cocaine Free Base (i.e., Crack) Smoking of free base “rock” using pipes Cocaine HCl Intravenous injection of solutions using needle and syringe Intranasal snorting of powder Pharmacokinetics and Metabolism Pharmacokinetics Smoked drug reaches brain within seconds Intravenous drug reaches brain within seconds Intranasal drug reaches brain within minutes Metabolism Ester hydrolysis to benzoylecgonine Ecgonine methyl ester Cone, 1995 Rate Hypothesis of Drug Reward Smoked and Intravenous Routes Faster rate of drug entry into the brain Enhanced subjective and rewarding effects Intranasal and Oral Routes Slower rate of drug entry into the brain Reduced subjective and rewarding effects Desired Effects Enhanced Mood and Euphoria Increased Attention and Alertness Decreased Need for Sleep Appetite Suppression Sexual Arousal Adverse Effects Psychosis Tachycardia, Arrhythmias, Heart Attack Hypertension, Stroke Hyperthermia, Rhabdomyolysis Multisystem Organ Failure Tolerance- -
Recommended Methods for the Identification and Analysis Of
Vienna International Centre, P.O. Box 500, 1400 Vienna, Austria Tel: (+43-1) 26060-0, Fax: (+43-1) 26060-5866, www.unodc.org RECOMMENDED METHODS FOR THE IDENTIFICATION AND ANALYSIS OF AMPHETAMINE, METHAMPHETAMINE AND THEIR RING-SUBSTITUTED ANALOGUES IN SEIZED MATERIALS (revised and updated) MANUAL FOR USE BY NATIONAL DRUG TESTING LABORATORIES Laboratory and Scientific Section United Nations Office on Drugs and Crime Vienna RECOMMENDED METHODS FOR THE IDENTIFICATION AND ANALYSIS OF AMPHETAMINE, METHAMPHETAMINE AND THEIR RING-SUBSTITUTED ANALOGUES IN SEIZED MATERIALS (revised and updated) MANUAL FOR USE BY NATIONAL DRUG TESTING LABORATORIES UNITED NATIONS New York, 2006 Note Mention of company names and commercial products does not imply the endorse- ment of the United Nations. This publication has not been formally edited. ST/NAR/34 UNITED NATIONS PUBLICATION Sales No. E.06.XI.1 ISBN 92-1-148208-9 Acknowledgements UNODC’s Laboratory and Scientific Section wishes to express its thanks to the experts who participated in the Consultative Meeting on “The Review of Methods for the Identification and Analysis of Amphetamine-type Stimulants (ATS) and Their Ring-substituted Analogues in Seized Material” for their contribution to the contents of this manual. Ms. Rosa Alis Rodríguez, Laboratorio de Drogas y Sanidad de Baleares, Palma de Mallorca, Spain Dr. Hans Bergkvist, SKL—National Laboratory of Forensic Science, Linköping, Sweden Ms. Warank Boonchuay, Division of Narcotics Analysis, Department of Medical Sciences, Ministry of Public Health, Nonthaburi, Thailand Dr. Rainer Dahlenburg, Bundeskriminalamt/KT34, Wiesbaden, Germany Mr. Adrian V. Kemmenoe, The Forensic Science Service, Birmingham Laboratory, Birmingham, United Kingdom Dr. Tohru Kishi, National Research Institute of Police Science, Chiba, Japan Dr. -
How the Saha Ionization Equation Was Discovered
How the Saha Ionization Equation Was Discovered Arnab Rai Choudhuri Department of Physics, Indian Institute of Science, Bangalore – 560012 Introduction Most youngsters aspiring for a career in physics research would be learning the basic research tools under the guidance of a supervisor at the age of 26. It was at this tender age of 26 that Meghnad Saha, who was working at Calcutta University far away from the world’s major centres of physics research and who never had a formal training from any research supervisor, formulated the celebrated Saha ionization equation and revolutionized astrophysics by applying it to solve some long-standing astrophysical problems. The Saha ionization equation is a standard topic in statistical mechanics and is covered in many well-known textbooks of thermodynamics and statistical mechanics [1–3]. Professional physicists are expected to be familiar with it and to know how it can be derived from the fundamental principles of statistical mechanics. But most professional physicists probably would not know the exact nature of Saha’s contributions in the field. Was he the first person who derived and arrived at this equation? It may come as a surprise to many to know that Saha did not derive the equation named after him! He was not even the first person to write down this equation! The equation now called the Saha ionization equation appeared in at least two papers (by J. Eggert [4] and by F.A. Lindemann [5]) published before the first paper by Saha on this subject. The story of how the theory of thermal ionization came into being is full of many dramatic twists and turns. -
International Quality Assurance Programme (Iqap)
INTERNATIONAL QUALITY ASSURANCE PROGRAMME (IQAP) INTERNATIONAL COLLABORATIVE EXERCISES (ICE) Summary Report SEIZED MATERIAL 2018/2 INTERNATIONAL QUALITY ASSURANCE PROGRAMME (IQAP) INTERNATIONAL COLLABORATIVE EXERCISES (ICE) Table of contents Introduction Page 3 Comments from the International Panel of Forensic Experts Page 3 NPS reported by ICE participants Page 5 Codes and Abbreviations Page 7 Sample 1 Analysis Page 8 Identified substances Page 8 Statement of findings Page 13 Identification methods Page 23 Summary Page 29 Z-Scores Page 30 Sample 2 Analysis Page 34 Identified substances Page 34 Statement of findings Page 39 Identification methods Page 49 Summary Page 55 Z-Scores Page 56 Sample 3 Analysis Page 59 Identified substances Page 59 Statement of findings Page 64 Identification methods Page 74 Summary Page 80 Z-Scores Page 81 Sample 4 Analysis Page 84 Identified substances Page 84 Statement of findings Page 89 Identification methods Page 99 Summary Page 105 Z-Scores Page 106 Test Samples Information Samples Comments on samples Sample 1 SM-1 was prepared from a seizure containing 22.7 % (w/w) Cocaine base. The test sample also contained lactose with methylecgonine, benzoylecgonine and cinnamoyl cocaine as minor components Sample 2 SM-2 was prepared from a seizure containing 9.8 % (w/w) 3,4-methylenedioxypyrovalerone base. The test sample also contained lactose. Sample 3 SM-3 was prepared from a seizure containing 19.6% (w/w) Metamfetamine base. The test sample also contained lactose Sample 4 SM-4 was prepared from a seizure containing -
1 Introduction
i i Karl-Heinz Spatschek: High Temperature Plasmas — Chap. spatscheck0415c01 — 2011/9/1 — page 1 — le-tex i i 1 1 Introduction A plasma is a many body system consisting of a huge number of interacting (charged and neutral) particles. More precisely, one defines a plasma as a quasineu- tral gas of charged and neutral particles which exhibits collective behavior. In many cases, one considers quasineutral gases consisting of charged particles, namely electrons and positively charged ions of one species. Plasmas may contain neutral atoms. In this case, the plasma is called partially or incompletely ionized. Other- wise the plasma is said to be completely or fully ionized. The term plasma is not limited to the most common electron–ion case. One may have electron–positron plasmas, quark-gluon plasmas, and so on. Semiconductors contain plasma con- sisting of electrons and holes. Most of the matter in the universe occurs in the plasma state. It is often said that 99% of the matter in the universe is in the plasma state. However, this estimate may not be very accurate. Remember the discussion on dark matter. Nevertheless, the plasma state is certainly dominating the universe. Modern plasma physics emerged in 1950s, when the idea of thermonuclear re- actor was introduced. Fortunately, modern plasma physics completely dissociated from weapons development. The progression of modern plasma physics can be retraced from many monographs, for example, [1–15]. In simple terms, plasmas can be characterized by two parameters, namely, charged particle density n and temperature T. The density varies over roughly 28 6 34 3 orders of magnitude, for example, from 10 to 10 m . -
Recommended Methods for the Identification and Analysis of Cocaine in Seized Materials
Recommended methods for the Identification and Analysis of Cocaine in Seized Materials MANUAL FOR USE BY NATIONAL DRUG ANALYSIS LABORATORIES Photo credits: UNODC Photo Library; UNODC/Ioulia Kondratovitch; Alessandro Scotti. Laboratory and Scientific Section UNITED NATIONS OFFICE ON DRUGS AND CRIME Vienna Recommended Methods for the Identification and Analysis of Cocaine in Seized Materials (Revised and updated) MANUAL FOR USE BY NATIONAL DRUG ANALYSIS LABORATORIES UNITED NATIONS New York, 2012 Note Operating and experimental conditions are reproduced from the original reference materials, including unpublished methods, validated and used in selected national laboratories as per the list of references. A number of alternative conditions and substitution of named commercial products may provide comparable results in many cases, but any modification has to be validated before it is integrated into laboratory routines. Mention of names of firms and commercial products does not imply the endorse- ment of the United Nations. ST/NAR/7/REV.1 Original language: English © United Nations, March 2012. All rights reserved. The designations employed and the presentation of material in this publication do not imply the expression of any opinion whatsoever on the part of the Secretariat of the United Nations concerning the legal status of any country, territory, city or area, or of its authorities, or concerning the delimitation of its frontiers or boundaries. This publication has not been formally edited. Publishing production: English, Publishing and Library Section, United Nations Office at Vienna. ii Contents Page 1. Introduction ................................................. 1 1.1 Background .............................................. 1 1.2 Purpose and use of the manual .............................. 1 2. Physical appearance and chemical characteristics of coca leaf and illicit materials containing cocaine ................................ -
Make Crack with Ammonia
Make crack with ammonia Continue Image via Wikipedia Updated November 2015 NOTE: Be sure to check out our article on cocaine - How do you take yours? This looks at the ways in which we take our coke, talks with peeps involved and gives some helpful harm reduction tips to users. This information has been collected through in-depth research on the internet (from the best users/chefs) from our crews of own experience, and some brilliant books - or rather, one brilliant book - Cocaine Handbook - from Dave Lee (there's a reprint I believe). Now it would be wrong to start this article, let alone that Cocaine Clean-Up is really about the two ends of the sword; In our black market world horrible adulterers and God knows that in our street cocaine these days is a really good thing to be able to do something to take control back into your own hands and do something to clear your cocaine of adulterers in it. And the truth is, while we can't get rid of them all, even through the freebasing old-school way (levisomole, cattle de-wormer is thought to survive in the process!), it significantly makes for a better tasting product - in that you'll feel much less wired, fast, agitated, etc. and quickly realize that a purified product is very different from the street's drugs. But when there's a good thing - there's a crappy thing around the corner - in this case - the incredible thrust after a single pipe base is waaaay more than a line or even an injectable.. -
Lecture 8: Statistical Equilibria, Saha Equation
Statistical Equilibria: Saha Equation We are now going to consider the statistics of equilibrium. Specifically, suppose we let a system stand still for an extremely long time, so that all processes can come into balance. We then measure the fraction of particles that are in each of several states (e.g., if we have a pure hydrogen gas, we might want to know the ionization fraction). How can we compute this fraction? We’ll take a look at this in several different ways. We will then step back and ask ourselves when these equilibrium formulae do not apply. This is important! To paraphrase Clint Eastwood, “An equation’s got to know its limitations”. In virtually all astronomical problems we deal with approximations, so we always need a sense of when those approximations fail. This serves a double purpose: it keeps us from making errors, but it also keeps us from applying too complex an approach to a simple problem. Let’s start out with a simple case. We consider a column of isothermal gas (temperature T ) in a constant gravitational acceleration g. Each molecule has mass m. If we can treat this like an ideal gas, Ask class: how do we figure out how the pressure vary with height h? An ideal gas has pressure P = nkT , where n is the number density. In equilibrium the pressure gradient balances the weight of the gas, so dP/dh = −ρg. Using ρ = nm = P m/kT and the constancy of T , we have dP/dh = −(mg/kT )P , so P = P0 exp(−mgh/kT ), where P0 is defined as the pressure at h = 0.