Elementary charge
You don't need to be Editor-In-Chief to add or edit content to WikiDoc. You can begin to add to or edit text on this WikiDoc page by clicking on the edit button at the top of this page. Next enter or edit the information that you would like to appear here. Once you are done editing, scroll down and click the Save page button at the bottom of the page.
Please Take Over This Page and Apply to be Editor-In-Chief for this topic: There can be one or more than one Editor-In-Chief. You may also apply to be an Associate Editor-In-Chief of one of the subtopics below. Please mail us [1] to indicate your interest in serving either as an Editor-In-Chief of the entire topic or as an Associate Editor-In-Chief for a subtopic. Please be sure to attach your CV and or biographical sketch.
The elementary charge, e, is the electric charge carried by a single proton, or equivalently, the negative of the electric charge carried by a single electron.
This is a fundamental physical constant and the unit of electric charge in the system of atomic units as well as some other systems of natural units.
It has a measured value of approximately Template:Val/delimitnum×10Template:Su Template:Val/unitswithlink, according to the NIST posted CODATA value for e. See the 2006 Committee on Data for Science and Technology (CODATA) list of physical constants: CODATA report, TABLE XLVIII for uncertainty in e. In the centimetre gram second system of units, the value is Template:Val/delimitnum×10Template:Su statcoulombs.
Since it was first measured in Robert Millikan's famous oil-drop experiment in 1909, the elementary charge has been considered indivisible. Quarks, first posited in the 1960s, have fractional electric charges (in units of 1⁄3 e and 2⁄3 e so that now the term elementary charge referring to the charge on an electron is no longer strictly correct; this is irrelevant, however, in practical terms, since quarks are not detected except in groupings that have charges that are integer multiples of e. In 1982 Robert Laughlin tried to explain the fractional quantum Hall effect by predicting the existence of fractionally charged quasiparticles. In 1995, the fractional charge of Laughlin quasiparticles was measured directly in a quantum antidot electrometer at Stony Brook University, New York. In 1997, two groups of physicists at the Weizmann Institute of Science in Rehovot, Israel, and at the Commissariat à l'énergie atomique laboratory near Paris, claimed to have detected such quasiparticles carrying an electric current.
External links
- "Measurement of fractional charge" (Science Report) 1995
- "Quantum antidot electrometer"
- "Fractional charge carriers discovered" - Physics Web article 1997-10-24
- "Direct observation of a fractional charge" (letter to Nature) 1997
References
Fundamentals of Physics, 7th Ed., Halliday, Robert Resnick, and Jearl Walker. Wiley, 2005br:Karg elfennel ca:Càrrega elemental cs:Elementární náboj de:Elementarladung et:Elementaarlaengeo:Elementa elektra ŝargo fa:بار الکترونko:기본 전하 hr:Elementarni naboj id:Muatan listrik partikel it:Carica elementare he:מטען אלמנטרי lt:Elementarusis krūvis hu:Elemi töltés nl:Elementaire ladingno:Elementærladningsl:Osnovni naboj fi:Alkeisvaraus sv:Elementarladdninguk:Елементарний електричний заряд ur:بنیادی بار
Acknowledgement and Attribution Regarding Sources of Content
Some of the initial content on this page may be incorporated in part from copyleft sources in the public domain including wikis such as Wikipedia and AskDrWiki. Drug information for patients came from the The National Library of Medicine. Infectious disease information may have come from the Centers for Disease Control (CDC). Differential Diagnoses are drawn from clinicians as well as an amalgamation of 3 sources: 1.The Disease Database; 2. Kahan, Scott, Smith, Ellen G. In A Page: Signs and Symptoms. Malden, Massachusetts: Blackwell Publishing, 2004:3; 3. Sailer, Christian, Wasner, Susanne. Differential Diagnosis Pocket. Hermosa Beach, CA: Borm Bruckmeir Publishing LLC, 2002:7 .

