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{{Distinguish2|[[Iron|ferrum]]}}
{{Modulation techniques}}
{{good article}}
[[File:Amfm3-en-de.gif|thumb|right|250px|A signal may be carried by an [[Amplitude modulation|AM]] or FM radio wave.|alt=Animation of audio, AM and FM signals]]
{{infobox fermium}}
'''Fermium''' is a [[synthetic element]] with symbol&nbsp;'''Fm''' and [[atomic number]]&nbsp;100. It is a member of the [[actinide]] series. It is the heaviest element that can be formed by [[neutron]] bombardment of lighter elements, and hence the last element that can be prepared in macroscopic quantities, although pure fermium metal has not yet been prepared.<ref name="Silva"/> A total of 19 isotopes are known, with <sup>257</sup>Fm being the longest-lived with a half-life of 100.5 days.


It was discovered in the debris of the [[Ivy Mike|first]] [[hydrogen bomb]] explosion in 1952, and named after [[Enrico Fermi]], one of the pioneers of [[nuclear physics]]. Its chemistry is typical for the late actinides, with a preponderance of the +3 [[oxidation state]] but also an accessible +2 oxidation state. Owing to the small amounts of produced fermium and all of its isotopes having relatively short half-lives, there are currently no uses for it outside of basic scientific research.
In [[telecommunications]] and [[signal processing]], '''frequency modulation''' ('''FM''') is the encoding of [[information]] in a [[carrier wave]] by varying the [[instantaneous frequency]] of the wave. (Compare with [[amplitude modulation]], in which the [[amplitude]] of the carrier wave varies, while the frequency remains constant.)


==Discovery==
In [[analog signal]] applications, the difference between the instantaneous and the base frequency of the carrier is directly proportional to the instantaneous value of the input-signal amplitude.
[[File:Ivy Mike - mushroom cloud.jpg|thumb|left|Fermium was first observed in the fallout from the ''Ivy Mike'' nuclear test.]]
[[File:Enrico Fermi 1943-49.jpg|thumb|left|The element was named after Enrico Fermi.]]
[[File:Albert Ghiorso ca 1970.jpg|thumb|left|The element was discovered by a team headed by [[Albert Ghiorso]].]]
Fermium was first discovered in the fallout from the '[[Ivy Mike]]' nuclear test (1&nbsp;November 1952), the first successful test of a hydrogen bomb.<ref name="lanl">{{cite web| url=http://periodic.lanl.gov/elements/99.html|title=Einsteinium|accessdate=2007-12-07|archiveurl=http://web.archive.org/web/20071026052909/http://periodic.lanl.gov/elements/99.html <!--Added by H3llBot-->|archivedate=2007-10-26}}</ref><ref name="nrc">[http://www.nrc-cnrc.gc.ca/eng/education/elements/el/fm.html Fermium – National Research Council Canada]. Retrieved 2 December 2007</ref><ref name="Ghiorso"/> Initial examination of the debris from the explosion had shown the production of a new isotope of [[plutonium]], [[plutonium-244|{{Nuclide|Pu|Z=94|A=244}}]]: this could only have formed by the absorption of six [[neutron]]s by a [[uranium-238]] nucleus followed by two [[Beta decay|β<sup>−</sup>&nbsp;decays]]. At the time, the absorption of neutrons by a heavy nucleus was thought to be a rare process, but the identification of {{Nuclide|Pu|Z=94|A=244}} raised the possibility that still more neutrons could have been absorbed by the uranium nuclei, leading to new elements.<ref name="Ghiorso">{{cite journal|first = Albert|last = Ghiorso|authorlink = Albert Ghiorso|date = 2003 |title = Einsteinium and Fermium|journal = Chemical and Engineering News|url = http://pubs.acs.org/cen/80th/einsteiniumfermium.html|volume = 81|issue = 36|doi = 10.1021/cen-v081n036.p174|pages = 174}}</ref>


Element&nbsp;99 ([[einsteinium]]) was quickly discovered on filter papers which had been flown through the cloud from the explosion (the same sampling technique that had been used to discover {{Nuclide|Pu|Z=94|A=244}}).<ref name="Ghiorso"/> It was then identified in December 1952 by [[Albert Ghiorso]] and co-workers at the [[University of California at Berkeley]].<ref name="lanl"/><ref name="nrc">[http://www.nrc-cnrc.gc.ca/eng/education/elements/el/es.html Einsteinium – National Research Council Canada]. Retrieved 2 December 2007</ref><ref name="Ghiorso"/> They discovered the isotope <sup>253</sup>Es ([[half-life]] 20.5 days) that was made by the [[neutron capture|capture]] of 15 [[neutron]]s by [[uranium-238]] nuclei – which then underwent seven successive [[beta decay]]s:
[[Digital data]] can be encoded and transmitted via a carrier wave by shifting the carrier's frequency among a predefined set of frequencies—a technique known as [[frequency-shift keying]] (FSK). FSK is widely used in [[modem]]s and [[fax modem]]s, and can also be used to send [[Morse code]].<ref>{{Cite book
:<small><math>\mathrm{^{238}_{\ 92}U\ \xrightarrow {+\ 15 n,  7 \beta^-} \ ^{253}_{\ 99}Es}</math></small>
|title = Teach yourself electricity and electronics
Some <sup>238</sup>U atoms, however, could capture another amount of neutrons (most likely, 16 or 17).
|author = Stan Gibilisco
|publisher = McGraw-Hill Professional
|year = 2002
|isbn = 978-0-07-137730-0
|page = 477
|url = http://books.google.com/?id=-Q6SBAKsmXkC&pg=PA477&dq=morse-code+frequency-shift-keying+sent-using-fsk
}}</ref> [[Radioteletype]] also uses FSK.<ref>{{Cite book
|title = The Electronics of Radio
|author = David B. Rutledge
|publisher = Cambridge University Press
|year = 1999
|isbn = 978-0-521-64645-1
|page = 310
|url = http://books.google.com/?id=ZvJYLhk4N64C&pg=RA2-PA310&dq=radio-teletype+fsk
}}</ref>


The discovery of fermium (Z&nbsp;= 100) required more material, as the yield was expected to be at least an order of magnitude lower than that of element&nbsp;99, and so contaminated coral from the [[Enewetak atoll]] (where the test had taken place) was shipped to the [[University of California Radiation Laboratory]] in [[Berkeley, California]], for processing and analysis. About two months after the test, a new component was isolated emitting high-energy [[α-particle]]s (7.1&nbsp;MeV) with a [[half-life]] of about a day. With such a short half-life, it could only arise from the β<sup>−</sup>&nbsp;decay of an isotope of einsteinium, and so had to be an isotope of the new element&nbsp;100: it was quickly identified as <sup>255</sup>Fm (t</sub>&nbsp;= 20.07(7)&nbsp;hours).<ref name="Ghiorso"/>
Frequency modulation is used in [[radio]], [[telemetry]], [[radar]], seismic prospecting, and monitoring [[newborn]]s for seizures via [[EEG]].<ref>B. Boashash, editor, “Time-Frequency Signal Analysis and Processing – A Comprehensive Reference”, Elsevier Science, Oxford, 2003; ISBN 0-08-044335-4</ref> FM is widely used for [[FM broadcasting|broadcasting]] music and speech, [[two-way radio]] systems, magnetic tape-recording systems and some video-transmission systems. In radio systems, frequency modulation with sufficient [[Bandwidth (signal processing)|bandwidth]] provides an advantage in cancelling naturally-occurring noise.


The discovery of the new elements, and the new data on neutron capture, was initially kept secret on the orders of the U.S.&nbsp;military until 1955 due to [[Cold War]] tensions.<ref name="Ghiorso"/><ref name = "PhysRev.99.1048" >{{cite journal
Frequency modulation is known as [[phase modulation]] when the carrier phase modulation is the time [[integral]] of the FM signal.{{clarify|date=July 2013}}
| last1 = Ghiorso
| first1 = A.
| last2 = Thompson
| first2 = S.
| last3 = Higgins
| first3 = G.
| last4 = Seaborg
| first4 = G.
| last5 = Studier
| first5 = M.
| last6 = Fields
| first6 = P.
| last7 = Fried
| first7 = S.
| last8 = Diamond
| first8 = H.
| last9 = Mech
| first9 = J.
| last10 = Pyle
| first10 = G.
| last11 = Huizenga
| first11 = J.
| last12 = Hirsch
| first12 = A.
| last13 = Manning
| first13 = W.
| last14 = Browne
| first14 = C.
| last15 = Smith
| first15 = H.
| last16 = Spence
| first16 = R.
| title = New Elements Einsteinium and Fermium, Atomic Numbers 99 and 100
| journal = Phys. Rev.
| volume = 99
| issue = 3
| doi = 10.1103/PhysRev.99.1048
| pages = 1048–1049
| date = 1955|bibcode = 1955PhRv...99.1048G | display-authors = 8
}}</ref><ref>Fields, P. R.; Studier, M. H.; Diamond, H.; Mech, J. F.; Inghram, M. G. Pyle, G. L.; Stevens, C. M.; Fried, S.; Manning, W. M. (Argonne National Laboratory, Lemont, Illinois); Ghiorso, A.; Thompson, S. G.; Higgins, G. H.; Seaborg, G. T. (University of California, Berkeley, California): "Transplutonium Elements in Thermonuclear Test Debris", in: {{cite journal|last1=Fields|first1=P.|last2=Studier|first2=M.|last3=Diamond|first3=H.|last4=Mech|first4=J.|last5=Inghram|first5=M.|last6=Pyle|first6=G.|last7=Stevens|first7=C.|last8=Fried|first8=S.|last9=Manning|first9=W. |last10=Ghiorso|first10=A.|last11=Thompson|first11=S.|last12=Higgins|first12=G.|last13=Seaborg|first13=G.|title=Transplutonium Elements in Thermonuclear Test Debris|journal=Physical Review|volume=102|pages=180|date=1956|doi=10.1103/PhysRev.102.180|bibcode = 1956PhRv..102..180F }}</ref> Nevertheless, the Berkeley team were able to prepare elements 99 and 100 by civilian means, through the neutron bombardment of [[plutonium-239]], and published this work in 1954 with the disclaimer that it was not the first studies that had been carried out on the elements.<ref name = "PhysRev.93.908">{{cite journal|first1 = S. G.|last1 = Thompson |first2 = A.|last2 = Ghiorso|authorlink2 = Albert Ghiorso|first3 = B. G.|last3 = Harvey|first4 = G. R.|last4 = Choppin|title = Transcurium Isotopes Produced in the Neutron Irradiation of Plutonium|journal = Physical Review|volume = 93|issue = 4|page = 908|date = 1954|doi = 10.1103/PhysRev.93.908|bibcode = 1954PhRv...93..908T }}</ref><ref>{{cite journal|first1 = G. R.|last1 = Choppin|first2 = S. G.|last2 = Thompson|first3 = A.|last3 = Ghiorso|authorlink3 = Albert Ghiorso|first4 = B. G.|last4 = Harvey|title = Nuclear Properties of Some Isotopes of Californium, Elements 99 and 100|journal = Physical Review|volume = 94|issue = 4|pages = 1080–1081|date = 1954|doi = 10.1103/PhysRev.94.1080|bibcode = 1954PhRv...94.1080C }}</ref> The 'Ivy Mike' studies were declassified and published in 1955.<ref name = "PhysRev.99.1048"/>


The Berkeley team had been worried that another group might discover lighter isotopes of element&nbsp;100 through ion bombardment techniques before they could publish their classified research,<ref name="Ghiorso"/> and this proved to be the case. A group at the Nobel Institute for Physics in Stockholm independently discovered the element, producing an [[isotope]] later confirmed to be <sup>250</sup>Fm (t<sub>1/2</sub>&nbsp;= 30&nbsp;minutes) by bombarding a {{Nuclide|U|Z=92|A=238}} target with [[oxygen-16]] ions, and published their work in May 1954.<ref>{{cite journal|last1 = Atterling|first1 = Hugo|last2 = Forsling|first2 = Wilhelm|last3 = Holm |first3 = Lennart W.|last4 = Melander|first4 = Lars|last5 = Åström|first5 = Björn|date = 1954|title = Element 100 Produced by Means of Cyclotron-Accelerated Oxygen Ions|journal = Physical Review|volume = 95|issue = 2|pages = 585–586|doi = 10.1103/PhysRev.95.585.2|bibcode = 1954PhRv...95..585A }}</ref> Nevertheless, the priority of the Berkeley team was generally recognized, and with it the prerogative to name the new element in honour of the recently deceased [[Enrico Fermi]], the developer of the first artificial self-sustained nuclear reactor.
==Theory==
If the information to be transmitted (i.e., the [[baseband signal]]) is <math>x_m(t)</math> and the [[sinusoidal]] carrier is <math>x_c(t) = A_c \cos (2 \pi f_c t)\,</math>, where ''f<sub>c</sub>'' is the carrier's base frequency, and ''A<sub>c</sub>'' is the carrier's amplitude, the modulator combines the carrier with the baseband data signal to get the transmitted signal:


==Isotopes==
:<math>y(t) = A_c \cos \left( 2 \pi \int_{0}^{t} f(\tau) d \tau \right)</math>
{{Main|Isotopes of fermium}}
::<math>= A_{c} \cos \left( 2 \pi \int_{0}^{t} \left[ f_{c} + f_{\Delta} x_{m}(\tau) \right] d \tau \right)</math>
[[File:Decay of Fermium-257.PNG|thumb|center|750px|Decay pathway of fermium-257]]
::<math> = A_{c} \cos \left( 2 \pi f_{c} t + 2 \pi f_{\Delta} \int_{0}^{t}x_{m}(\tau) d \tau \right) </math>
{{clear}}
There are 19 isotopes of fermium listed in N<small>UBASE</small>&nbsp;2003,<ref name="NUBASE">{{NUBASE 2003}}</ref> with atomic weights of 242 to 260,{{#tag:ref|The discovery of <sup>260</sup>Fm is considered "unproven" in N<small>UBASE</small>&nbsp;2003.<ref name="NUBASE"/>|group=Note|name=Fm-260}} of which <sup>257</sup>Fm is the longest-lived with a [[half-life]] of 100.5&nbsp;days. <sup>253</sup>Fm has a half-life of 3 days, while <sup>251</sup>Fm of 5.3&nbsp;h, <sup>252</sup>Fm of 25.4&nbsp;h, <sup>254</sup>Fm of 3.2&nbsp;h, <sup>255</sup>Fm of 20.1&nbsp;h, and <sup>256</sup>Fm of 2.6&nbsp;hours. All the remaining ones have half-lives ranging from 30 minutes to less than a millisecond.<ref name="NUBASE"/>
The neutron-capture product of fermium-257, <sup>258</sup>Fm, undergoes [[spontaneous fission]] with a half-life of just 370(14)&nbsp;microseconds; <sup>259</sup>Fm and <sup>260</sup>Fm are also unstable with respect to spontaneous fission (t<sub>1/2</sub>&nbsp;= 1.5(3)&nbsp;s and 4&nbsp;ms respectively).<ref name="NUBASE"/><ref group="Note" name="Fm-260"/> This means that neutron capture cannot be used to create [[nuclide]]s with a [[mass number]] greater than 257, unless carried out in a nuclear explosion. As <sup>257</sup>Fm is an [[Alpha decay|α-emitter]], decaying to <sup>253</sup>Cf, and no fermium isotopes undergo [[beta minus decay]] (which would produce isotopes of the next element, mendelevium), fermium is also the last element that can be prepared by a neutron-capture process.<ref name="Silva">{{cite journal|last = Silva|first = Robert J.|contribution = Fermium, Mendelevium, Nobelium, and Lawrencium|title = The Chemistry of the Actinide and Transactinide Elements|editor1-first = Lester R.|editor1-last = Morss|editor2-first = Norman M.|editor2-last = Edelstein|editor3-first = Jean|editor3-last = Fuger|edition = 3rd|date = 2006|volume = 3|publisher = Springer|location = Dordrecht|pages = 1621–1651|url = http://radchem.nevada.edu/classes/rdch710/files/Fm%20to%20Lr.pdf |format=PDF| doi = 10.1007/1-4020-3598-5_13|isbn = 978-1-4020-3555-5}}</ref><ref name="G&E">{{Greenwood&Earnshaw1st|page=1262}}</ref><ref name=nuclidetable>{{cite web |url=http://www.nndc.bnl.gov/chart/reCenter.jsp?z=100&n=147 |title=Interactive Chart of Nuclides |publisher=Brookhaven National Laboratory |author=Sonzogni, Alejandro |location=National Nuclear Data Center |accessdate=2008-06-06}}</ref>
{{clear}}


==Production==
In this equation, <math>f(\tau)\,</math> is the ''[[instantaneous phase#Instantaneous frequency|instantaneous frequency]]'' of the oscillator and <math>f_{\Delta}\,</math> is the ''[[frequency deviation]]'', which represents the maximum shift away from ''f<sub>c</sub>'' in one direction, assuming ''x''<sub>''m''</sub>(''t'') is limited to the range ±1.
[[File:Elutionskurven Fm Es Cf Bk Cm Am.png|thumb|[[Elution]]: chromatographic separation of Fm(100), Es(99), Cf, Bk, Cm and Am.]]
Fermium is produced by the bombardment of lighter [[actinide]]s with [[neutron]]s in a nuclear reactor. Fermium-257 is the heaviest isotope that is obtained via neutron capture, and can only be produced in nanogram quantities.<ref group=Note>All isotopes of elements Z &gt; 100 can only be produced by accelerator-based nuclear reactions with charged particles and can be obtained only in tracer quantities (e.g., 1 million atoms for Md (Z = 101) per hour of irradiation (see reference 1 below)).</ref><ref>{{cite journal|last1=Luig |first1=Heribert|last2=Keller|first2=Cornelius|last3=Wolf|first3=Walter|last4=Shani |first4=Jashovam
|last5=Miska|first5=Horst|last6=Zyball |first6=Alfred |last7=Gervé|first7=Andreas|last8=Balaban|first8=Alexandru T.|last9=Kellerer|first9=Albrecht M.|last10=Griebel|first10=Jürgen|title=Ullmann's Encyclopedia of Industrial Chemistry|date=2000|doi=10.1002/14356007.a22_499|chapter=Radionuclides|isbn=3527306730}}</ref> The major source is the 85&nbsp;MW [[High Flux Isotope Reactor]] (HFIR) at the [[Oak Ridge National Laboratory]] in [[Tennessee]], USA, which is dedicated to the production of transcurium (''Z''&nbsp;> 96) elements.<ref>{{cite web|title = High Flux Isotope Reactor|url = http://neutrons.ornl.gov/facilities/HFIR/|publisher = Oak Ridge National Laboratory|accessdate = 2010-09-23}}</ref> In a "typical processing campaign" at Oak Ridge, tens of grams of [[curium]] are irradiated to produce decigram quantities of [[californium]], milligram quantities of [[berkelium]] and [[einsteinium]] and picogram quantities of fermium.<ref>{{cite journal|first1 = C. E.|last1 = Porter|first2 = F. D., Jr.|last2 = Riley|first3 = R. D.|last3 = Vandergrift|first4 = L. K.|last4 = Felker|title = Fermium Purification Using Teva Resin Extraction Chromatography|journal = Sep. Sci. Technol.|volume = 32|issue = 1–4|date = 1997|pages = 83–92|doi = 10.1080/01496399708003188}}</ref> However, nanogram<ref>{{cite journal|first1 = M.|last1 = Sewtz|first2 = H.|last2 = Backe|first3 = A.|last3 = Dretzke|first4 = G.|last4 = Kube|first5 = W.|last5 = Lauth|first6 = P.|last6 = Schwamb|first7 = K.|last7 = Eberhardt|first8 = C.|last8 = Grüning|first9 = P.|last10 = Trautmann|first10 = N.|last11 = Kunz|first11 = P.|last12 = Lassen|first12 = J.|last13 = Passler|first13 = G.|last14 = Dong|first14 = C.|last15 = Fritzsche|first15 = S.|last16 = Haire|first16 = R.|last9 = Thörle
|title = First Observation of Atomic Levels for the Element Fermium (''Z''=100)|journal = Phys. Rev. Lett.|volume = 90|issue = 16|page = 163002|date = 2003|doi = 10.1103/PhysRevLett.90.163002|bibcode=2003PhRvL..90p3002S}}</ref> and microgram<ref name="G&E"/> quantities of fermium can be prepared for specific experiments. The quantities of fermium produced in 20–200&nbsp;kiloton thermonuclear explosions is believed to be of the order of milligrams, although it is mixed in with a huge quantity of debris; 40&nbsp;picograms of <sup>257</sup>Fm was recovered from 10&nbsp;kilograms of debris from the '[[Operation Mandrel|Hutch]]' test (16&nbsp;July 1969).<ref>{{cite journal|last1 = Hoff|first1 = R. W.|last2 = Hulet|first2 = E. K.|date = 1970|title = Engineering with Nuclear Explosives|volume = 2|pages = 1283–1294}}</ref>


After production, the fermium must be separated from other actinides and from [[lanthanoid]] fission products. This is usually achieved by [[ion exchange chromatography]], with the standard process using a cation exchanger such as Dowex&nbsp;50 or T<small>EVA</small> eluted with a solution of ammonium α-hydroxyisobutyrate.<ref name="Silva"/><ref>{{cite journal|last1 = Choppin|first1 = G. R.|last2 = Harvey|first2 = B. G.|last3 = Thompson|first3 = S. G.|date = 1956|title = A new eluant for the separation of the actinide elements|journal = J. Inorg. Nucl. Chem.|volume = 2|issue = 1|pages = 66–68|doi = 10.1016/0022-1902(56)80105-X}}</ref> Smaller cations form more stable complexes with the α-hydroxyisobutyrate anion, and so are preferentially eluted from the column.<ref name="Silva"/> A rapid [[fractional crystallization (chemistry)|fractional crystallization]] method has also been described.<ref name="Silva"/><ref>{{cite journal|last1 = Mikheev|first1 = N. B.|last2 = Kamenskaya|first2 = A. N.|last3 = Konovalova|first3 = N. A.|last4 = Rumer|first4 = I. A.|last5 = Kulyukhin|first5 = S. A.|title = High-speed method for the separation of fermium from actinides and lanthanides|date =1983|journal = Radiokhimiya|volume = 25|issue = 2|pages = 158–161}}</ref>
While most of the energy of the signal is contained within  ''f<sub>c</sub>'' ± ''f''<sub>Δ</sub>, it can be shown by [[Fourier analysis]] that a wider range of frequencies is required to precisely represent an FM signal. The [[frequency spectrum]] of an actual FM signal has components extending infinitely, although their amplitude decreases and higher-order components are often neglected in practical design problems.<ref name=TGTSCS05/>


Although the most stable isotope of fermium is <sup>257</sup>Fm, with a [[half-life]] of 100.5&nbsp;days, most studies are conducted on <sup>255</sup>Fm (t<sub>1/2</sub>&nbsp;= 20.07(7)&nbsp;hours) as this isotope can be easily isolated as required as the decay product of <sup>255</sup>Es (t<sub>1/2</sub>&nbsp;= 39.8(12)&nbsp;days).<ref name="Silva"/>
===Sinusoidal baseband signal===
Mathematically, a baseband modulated signal may be approximated by a [[Sine wave|sinusoid]]al [[continuous wave]] signal with a frequency ''f<sub>m</sub>''. The integral of such a signal is:


==Synthesis in nuclear explosions==
:<math>\int_{0}^{t}x_m(\tau)d \tau = \frac{A_m \cos (2 \pi f_m t)}{2 \pi f_m}\,</math>
The analysis of the debris at the 10-[[TNT equivalent|megaton]] ''Ivy Mike'' nuclear test was a part of long-term project, one of the goals of which was studying the efficiency of production of transuranium elements in high-power nuclear explosions. The motivation for these experiments was as follows: synthesis of such elements from uranium requires multiple neutron capture. The probability of such events increases with the neutron flux, and nuclear explosions are the most powerful neutron sources, providing densities of the order 10<sup>23</sup> neutrons/cm<sup>2</sup> within a microsecond, i.e. about 10<sup>29</sup> neutrons/(cm<sup>2</sup>·s). In comparison, the flux of the HFIR reactor is 5{{e|15}} neutrons/(cm<sup>2</sup>·s). A dedicated laboratory was set up right at [[Enewetak Atoll]] for preliminary analysis of debris, as some isotopes could have decayed by the time the debris samples reached the U.S. The laboratory was receiving samples for analysis, as soon as possible, from airplanes equipped with paper filters which flew over the atoll after the tests. Whereas it was hoped to discover new chemical elements heavier than fermium, those were not found after a series of megaton explosions conducted between 1954 and 1956 at the atoll.<ref name=s39>Seaborg, p. 39</ref>


[[File:ActinideExplosionSynthesis.png|thumb|300px|left|Estimated yield of transuranium elements in the U.S. nuclear tests Hutch and Cyclamen.<ref name=s40/>]]
In this case, the expression for y(t) above simplifies to:
The atmospheric results were supplemented by the underground test data accumulated in the 1960s at the [[Nevada National Security Site|Nevada Test Site]], as it was hoped that powerful explosions conducted in confined space might result in improved yields and heavier isotopes. Apart from traditional uranium charges, combinations of uranium with americium and thorium have been tried, as well as a mixed plutonium-neptunium charge. They were less successful in terms of yield that was attributed to stronger losses of heavy isotopes due to enhanced fission rates in heavy-element charges. Isolation of the products was found to be rather problematic, as the explosions were spreading debris through melting and vaporizing rocks under the great depth of 300–600 meters, and drilling to such depth in order to extract the products was both slow and inefficient in terms of collected volumes.<ref name=s39/><ref name=s40>Seaborg, p. 40</ref>


Among the nine underground tests, which were carried between 1962 and 1969 and codenamed Anacostia (5.2 [[TNT equivalent|kilotons]], 1962), Kennebec (<5 kilotons, 1963), Par (38, kilotons, 1964), Barbel (<20 kilotons, 1964), Tweed (<20 kilotons, 1965), Cyclamen (13 kilotons, 1966), Kankakee (20-200 kilotons, 1966), Vulcan (25 kilotons, 1966) and Hutch (20-200 kilotons, 1969),<ref>[http://www.nv.doe.gov/library/publications/historical/DOENV_209_REV15.pdf United States Nuclear Tests July 1945 through September 1992], DOE/NV--209-REV 15, December 2000</ref> the last one was most powerful and had the highest yield of transuranium elements. In the dependence on the atomic mass number, the yield showed a saw-tooth behavior with the lower values for odd isotopes, due to their higher fission rates.<ref name=s40/> The major practical problem of the entire proposal was however collecting the radioactive debris dispersed by the powerful blast. Aircraft filters adsorbed only about 4{{e|-14}} of the total amount and collection of tons of corals at Enewetak Atoll increased this fraction by only two orders of magnitude. Extraction of about 500 kilograms of underground rocks 60 days after the Hutch explosion recovered only about 10<sup>−7</sup> of the total charge. The amount of transuranium elements in this 500-kg batch was only 30 times higher than in a 0.4&nbsp;kg rock picked up 7 days after the test. This observation demonstrated the highly nonlinear dependence of the transuranium elements yield on the amount of retrieved radioactive rock.<ref name=s43>Seaborg, p. 43</ref> In order to accelerate sample collection after explosion, shafts were drilled at the site not after but before the test, so that explosion would expel radioactive material from the epicenter, through the shafts, to collecting volumes near the surface. This method was tried in the Anacostia and Kennebec tests and instantly provided hundreds kilograms of material, but with actinide concentration 3 times lower than in samples obtained after drilling; whereas such method could have been efficient in scientific studies of short-lived isotopes, it could not improve the overall collection efficiency of the produced actinides.<ref name=s44>Seaborg, p. 44</ref>
:<math> y(t) = A_{c} \cos \left( 2 \pi f_{c} t + \frac{f_{\Delta}}{f_{m}} \cos \left( 2 \pi f_{m} t \right) \right)\,</math>


Although no new elements (apart from einsteinium and fermium) could be detected in the nuclear test debris, and the total yields of transuranium elements were disappointingly low, these tests did provide significantly higher amounts of rare heavy isotopes than previously available in laboratories. So 6{{e|9}} atoms of <sup>257</sup>Fm could be recovered after the Hutch detonation. They were then used in the studies of thermal-neutron induced fission of <sup>257</sup>Fm and in discovery of a new fermium isotope <sup>258</sup>Fm. Also the rare <sup>250</sup>Cm isotope was synthesized in large quantities, which is very difficult to produce in nuclear reactors from its progenitor <sup>249</sup>Cm – the half-life of <sup>249</sup>Cm (64 minutes) is much too short for months-long reactor irradiations, but is very "long" on the explosion timescale.<ref name=s47>Seaborg, p. 47</ref>
where the amplitude <math>A_{m}\,</math> of the modulating [[Sine wave|sinusoid]] is represented by the peak deviation <math>f_{\Delta}\,</math> (see [[frequency deviation]]).


==Natural occurrence==
The [[harmonic]] distribution of a [[sine wave]] carrier modulated by such a [[sinusoidal]] signal can be represented with [[Bessel function]]s; this provides the basis for a mathematical understanding of frequency modulation in the frequency domain.
Because of the short half-life of all isotopes of fermium, any [[Primordial nuclide|primordial]] fermium, that is fermium that could possibly be present on the Earth during its formation, has decayed by now. Synthesis of fermium from naturally occurring actinides uranium and thorium in the Earth crust requires multiple neutron capture, which is an extremely unlikely event. Therefore, most fermium is produced on Earth in scientific laboratories, high-power nuclear reactors, or in [[nuclear weapons testing|nuclear weapons tests]], and is present only within a few months from the time of the synthesis. [[Einsteinium]] and fermium did occur naturally in the [[natural nuclear fission reactor]] at [[Oklo]], but no longer do so.<ref name="emsley">{{cite book|last=Emsley|first=John|title=Nature's Building Blocks: An A-Z Guide to the Elements|edition=New|date=2011|publisher=Oxford University Press|location=New York, NY|isbn=978-0-19-960563-7}}</ref>


==Chemistry==
===Modulation index===
[[File:Fermium-Ytterbium Alloy.jpg|thumb|A fermium-[[ytterbium]] alloy used for measuring the [[enthalpy of vaporization]] of fermium metal.]]
As in other modulation systems, the value of the modulation index indicates by how much the modulated variable varies around its unmodulated level. It relates to variations in the carrier frequency:


The chemistry of fermium has only been studied in solution using tracer techniques, and no solid compounds have been prepared. Under normal conditions, fermium exists in solution as the Fm<sup>3+</sup> ion, which has a hydration number of 16.9 and an [[acid dissociation constant]] of 1.6{{e|−4}} (p''K''<sub>a</sub>&nbsp;= 3.8).<ref>{{cite journal|last1 = Lundqvist|first1 = Robert|last2 = Hulet|first2 = E. K.|last3 = Baisden|first3 = T. A.|date = 1981|last4 = Näsäkkälä|first4 = Elina|last5 = Wahlberg|first5 = Olof|title = Electromigration Method in Tracer Studies of Complex Chemistry. II. Hydrated Radii and Hydration Numbers of Trivalent Actinides|journal = Acta Chem. Scand., Ser. A|volume = 35|pages = 653–661|doi = 10.3891/acta.chem.scand.35a-0653}}</ref><ref>{{cite journal|last1 = Hussonnois|first1 = H.|last2 = Hubert|first2 = S.|last3 = Aubin|first3 = L.|last4 = Guillaumont|first4 = R.|last5 = Boussieres|first5 = G.|date = 1972|journal = Radiochem. Radioanal. Lett.|volume = 10|pages = 231–238}}</ref> Fm<sup>3+</sup> forms complexes with a wide variety of organic ligands with [[HSAB theory|hard]] donor atoms such as oxygen, and these complexes are usually more stable than those of the preceding actinides.<ref name="Silva"/> It also forms anionic complexes with ligands such as [[chloride]] or [[nitrate]] and, again, these complexes appear to be more stable than those formed by [[einsteinium]] or [[californium]].<ref>{{cite journal|last1 = Thompson|first1 = S. G.|last2 = Harvey|first2 = B. G.|last3 = Choppin|first3 = G. R.|last4 = Seaborg|first4 = G. T.|authorlink4 = Glenn T. Seaborg|date = 1954|title = Chemical Properties of Elements 99 and 100|journal = J. Am. Chem. Soc.|volume = 76|issue = 24|pages = 6229–6236|doi = 10.1021/ja01653a004}}</ref> It is believed that the bonding in the complexes of the later actinides is mostly [[Ionic bond|ionic]] in character: the Fm<sup>3+</sup> ion is expected to be smaller than the preceding An<sup>3+</sup> ions because of the higher [[effective nuclear charge]] of fermium, and hence fermium would be expected to form shorter and stronger metal–ligand bonds.<ref name="Silva"/>
:<math>h = \frac{\Delta{}f}{f_m} = \frac{f_\Delta |x_m(t)|}{f_m} \ </math>


Fermium(III) can be fairly easily reduced to fermium(II),<ref>{{cite journal|last = Malý|first = Jaromír|date = 1967|title = The amalgamation behaviour of heavy elements 1. Observation of anomalous preference in formation of amalgams of californium, einsteinium, and fermium|journal = Inorg. Nucl. Chem. Lett.|volume = 3|issue = 9|pages = 373–381|doi = 10.1016/0020-1650(67)80046-1}}</ref> for example with [[samarium(II) chloride]], with which fermium coprecipitates.<ref>{{cite journal|last1 = Mikheev|first1 = N. B.|last2 = Spitsyn|first2 = V. I.|last3 = Kamenskaya|first3 = A. N.|last4 = Gvozdec|first4 = B. A.|last5 = Druin|first5 = V. A.|last6 = Rumer|first6 = I. A.|last7 = Dyachkova|first7 = R. A.|last8 = Rozenkevitch|first8 = N. A.|last9 = Auerman|first9 = L. N.|date = 1972|title = Reduction of fermium to divalent state in chloride aqueous ethanolic solutions|journal = Inorg. Nucl. Chem. Lett.|volume = 8|issue = 11|pages = 929–936|doi = 10.1016/0020-1650(72)80202-2}}</ref><ref>{{cite journal|last1 = Hulet|first1 = E. K.|last2 = Lougheed|first2 = R. W.|last3 = Baisden|first3 = P. A.|last4 = Landrum|first4 = J. H.|last5 = Wild|first5 = J. F.|last6 = Lundqvist|first6 = R. F.|date = 1979|title = Non-observance of monovalent Md|journal = J. Inorg. Nucl. Chem.|volume = 41|issue = 12|pages = 1743–1747|doi = 10.1016/0022-1902(79)80116-5}}</ref> The [[electrode potential]] has been estimated to be similar to that of the [[ytterbium]](III)/(II) couple, or about −1.15&nbsp;V with respect to the [[standard hydrogen electrode]],<ref>{{cite journal|last1 = Mikheev|first1 = N. B.|last2 = Spitsyn|first2 = V. I.|last3 = Kamenskaya|first3 = A. N.|last4 = Konovalova|first4 = N. A.|last5 = Rumer|first5 = I. A.|last6 = Auerman|first6 = L. N.|last7 = Podorozhnyi|first7 = A. M.|date = 1977|title = Determination of oxidation potential of the pair Fm<sup>2+</sup>/Fm<sup>3+</sup>|journal = Inorg. Nucl. Chem. Lett.|volume = 13|issue = 12|pages = 651–656|doi = 10.1016/0020-1650(77)80074-3}}</ref> a value which agrees with theoretical calculations.<ref>{{cite journal|last = Nugent|first = L. J.|date = 1975|journal = MTP Int. Rev. Sci.: Inorg. Chem., Ser. One|volume = 7|pages = 195–219}}</ref> The Fm<sup>2+</sup>/Fm<sup>0</sup> couple has an electrode potential of −2.37(10)&nbsp;V based on [[Polarography|polarographic]] measurements.<ref>{{cite journal|last1 = Samhoun|first1 = K.|last2 = David|first2 = F.|last3 = Hahn|first3 = R. L.|last4 = O'Kelley|first4 = G. D.|last5 = Tarrant|first5 = J. R.|last6 = Hobart|first6 = D. E.|date = 1979|title = Electrochemical study of mendelevium in aqueous solution: No evidence for monovalent ions|journal = J. Inorg. Nucl. Chem.| volume = 41|issue = 12|pages = 1749–1754|doi = 10.1016/0022-1902(79)80117-7}}</ref>
where <math>f_m\,</math> is the highest frequency component present in the modulating signal ''x''<sub>''m''</sub>(''t''), and <math>\Delta{}f\,</math> is the peak frequency-deviation—i.e. the maximum deviation of the ''[[instantaneous phase#Instantaneous frequency|instantaneous frequency]]'' from the carrier frequency. If <math>h \ll 1</math>, the modulation is called ''narrowband FM'', and its bandwidth is approximately <math>2 f_m\,</math>.


==Toxicity==
If <math>h \gg 1</math>, the modulation is called ''wideband FM'' and its bandwidth is approximately <math>2 f_\Delta\,</math>. While wideband FM uses more bandwidth, it can improve the [[signal-to-noise ratio]] significantly; for example, doubling the value of <math>\Delta{}f\,</math>, while keeping <math>f_m</math> constant, results in an eight-fold improvement in the signal-to-noise ratio.<ref>Der, Lawrence, Ph.D., ''Frequency Modulation (FM) Tutorial'', http://www.silabs.com/Marcom%20Documents/Resources/FMTutorial.pdf, Silicon Laboratories, Inc., accessed 2013 February 24, p. 5</ref> (Compare this with [[Chirp spread spectrum]], which uses extremely wide frequency deviations to achieve processing gains comparable to traditional, better-known spread-spectrum modes).
Although few people come in contact with fermium, the [[International Commission on Radiological Protection]] has set annual exposure limits for the two most stable isotopes. For fermium-253, the ingestion limit was set at 10<sup>7</sup> [[Becquerel]]s (1 Bq is equivalent to one decay per second), and the inhalation limit at 10<sup>5</sup> Bq; for fermium-257, at 10<sup>5</sup> Bq and 4000 Bq respectively.<ref>{{cite book|last1=Koch|first1=Lothar|title=Transuranium Elements, in Ullmann's Encyclopedia of Industrial Chemistry|publisher=Wiley|date=2000|doi=10.1002/14356007.a27_167}}</ref>


==Notes and references==
With a tone-modulated FM wave, if the modulation frequency is held constant and the modulation index is increased, the (non-negligible) bandwidth of the FM signal increases but the spacing between spectra remains the same; some spectral components decrease in strength as others increase. If the frequency deviation is held constant and the modulation frequency increased, the spacing between spectra increases.


===Notes===
Frequency modulation can be classified as narrowband if the change in the carrier frequency is about the same as the signal frequency, or as wideband if the change in the carrier frequency is much higher (modulation index >1) than the signal frequency.
{{Reflist|group=Note}}
<ref>B. P. Lathi, ''Communication Systems'', John Wiley and Sons, 1968 ISBN 0-471-51832-8, p, 214–217</ref> For example, narrowband FM is used for [[two way radio]] systems such as [[Family Radio Service]], in which the carrier is allowed to deviate only 2.5&nbsp;kHz above and below the center frequency with speech signals of no more than 3.5&nbsp;kHz bandwidth. Wideband FM is used for [[FM broadcasting]], in which music and speech are transmitted with up to 75&nbsp;kHz deviation from the center frequency and carry audio with up to a 20-kHz bandwidth.


===References===
===Bessel functions===
{{Reflist|colwidth=30em}}
For the case of a carrier modulated by a single sine wave, the resulting frequency spectrum can be calculated using [[Bessel function]]s of the first kind, as a function of the sideband number and the modulation index. The carrier and sideband amplitudes are illustrated for different modulation indices of FM signals. For particular values of the modulation index, the carrier amplitude becomes zero and all the signal power is in the sidebands.<ref name=TGTSCS05>T.G. Thomas, S. C. Sekhar  ''Communication Theory'', Tata-McGraw Hill 2005, ISBN 0070590915  page 136</ref>
 
Since the sidebands are on both sides of the carrier, their count is doubled, and then multiplied by the modulating frequency to find the bandwidth. For example, 3 kHz deviation modulated by a 2.2 kHz audio tone produces a modulation index of 1.36. Examining the chart shows this modulation index will produce three sidebands. These three sidebands, when doubled, gives us (6 * 2.2 kHz) or a 13.2 kHz required bandwidth.
<!--   and   are spaces the width of a digit and punctuation, respectively; see [[Space (punctuation)#Table of spaces]]-->
{| class="wikitable" style="text-align:right;"
|-
!rowspan=2| Modulation<br />index
!colspan=17| Sideband
|-
! Carrier
! 1
! 2
! 3
! 4
! 5
! 6
! 7
! 8
! 9
! 10
! 11
! 12
! 13
! 14
! 15
! 16
|-
! 0.00
| 1.00
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|-
! 0.25
| 0.98
| 0.12
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|-
! 0.5 
| 0.94
| 0.24
| 0.03
|
|
|
|
|
|
|
|
|
|
|
|
|
|
|-
! 1.0 
| 0.77
| 0.44
| 0.11
| 0.02
|
|
|
|
|
|
|
|
|
|
|
|
|
|-
! 1.5 
| 0.51
| 0.56
| 0.23
| 0.06
| 0.01
|
|
|
|
|
|
|
|
|
|
|
|
|-
! 2.0 
| 0.22
| 0.58
| 0.35
| 0.13
| 0.03
|
|
|
|
|
|
|
|
|
|
|
|
|-
! 2.41
| 0   
| 0.52
| 0.43
| 0.20
| 0.06
| 0.02
|
|
|
|
|
|
|
|
|
|
|
|-
! 2.5 
|−0.05
| 0.50
| 0.45
| 0.22
| 0.07
| 0.02
| 0.01
|
|
|
|
|
|
|
|
|
|
|-
! 3.0 
|−0.26
| 0.34
| 0.49
| 0.31
| 0.13
| 0.04
| 0.01
|
|
|
|
|
|
|
|
|
|
|-
! 4.0 
|−0.40
|−0.07
| 0.36
| 0.43
| 0.28
| 0.13
| 0.05
| 0.02
|
|
|
|
|
|
|
|
|
|-
! 5.0 
|−0.18
|−0.33
| 0.05
| 0.36
| 0.39
| 0.26
| 0.13
| 0.05
| 0.02
|
|
|
|
|
|
|
|
|-
! 5.53
| 0   
| −0.34
| −0.13
| 0.25
| 0.40
| 0.32
| 0.19
| 0.09
| 0.03
| 0.01
|
|
|
|
|
|
|
|-
! 6.0 
| 0.15
|−0.28
|−0.24
| 0.11
| 0.36
| 0.36
| 0.25
| 0.13
| 0.06
| 0.02
|
|
|
|
|
|
|
|-
! 7.0 
| 0.30
| 0.00
|−0.30
|−0.17
| 0.16
| 0.35
| 0.34
| 0.23
| 0.13
| 0.06
| 0.02
|
|
|
|
|
|
|-
! 8.0 
| 0.17
| 0.23
|−0.11
|−0.29
|−0.10
| 0.19
| 0.34
| 0.32
| 0.22
| 0.13
| 0.06
| 0.03
|
|
|
|
|
|-
! 8.65
| 0   
| 0.27
| 0.06
|−0.24
|−0.23
| 0.03
| 0.26
| 0.34
| 0.28
| 0.18
| 0.10
| 0.05
| 0.02
|
|
|
|
|-
! 9.0 
|−0.09
| 0.25
| 0.14
|−0.18
|−0.27
|−0.06
| 0.20
| 0.33
| 0.31
| 0.21
| 0.12
| 0.06
| 0.03
| 0.01
|
|
|
|-
! 10.0 
|−0.25
| 0.04
| 0.25
| 0.06
|−0.22
|−0.23
|−0.01
| 0.22
| 0.32
| 0.29
| 0.21
| 0.12
| 0.06
| 0.03
| 0.01
|
|
|-
! 12.0 
| 0.05
|−0.22
|−0.08
| 0.20
| 0.18
|−0.07
|−0.24
|−0.17
| 0.05
| 0.23
| 0.30
| 0.27
| 0.20
| 0.12
| 0.07
| 0.03
| 0.01
|}
 
===Carson's rule===
{{Main|Carson bandwidth rule}}
 
A [[rule of thumb]], ''Carson's rule'' states that nearly all (~98 percent) of the power of a frequency-modulated signal lies within a [[bandwidth (signal processing)|bandwidth]] <math> B_T\, </math> of:
 
:<math>\ B_T = 2(\Delta f +f_m)\,</math>
 
where <math>\Delta f\,</math>, as defined above, is the peak deviation of the instantaneous frequency <math>f(t)\,</math> from the center carrier frequency <math>f_c\,</math>.
 
==Noise Reduction==
A major advantage of FM in a communications circuit, compared for example with [[Amplitude modulation|AM]], is the possibility of improved [[Signal-to-noise ratio]] (SNR). Compared with an optimum AM scheme, FM typically has poorer SNR below a certain signal level called the noise threshold, but above a higher level – the full improvement or full quieting threshold – the SNR is much improved over AM. The improvement depends on modulation level and deviation.  For typical voice communications channels, improvements are typically 5-15 dB.  FM broadcasting using wider deviation can achieve even greater improvements.  Additional techniques, such as pre-emphasis of higher audio frequencies with corresponding de-emphasis in the receiver, are generally used to improve overall SNR in FM circuits. Since FM signals have constant amplitude, FM receivers normally have limiters that remove AM noise, further improving SNR.<ref>{{cite book |title=Reference Data for Radio Engineers |edition=Fifth |page=21-11 |year=1970 |publisher=Howard W. Sams & Co. |editor=H. P. Westman}}</ref><ref>{{cite book |title=The ARRL Handbook for Radio Communications |publisher=American Radio Relay League |year=2010 |editor=H. Ward Silver and Mark J. Wilson (Eds) |author=Alan Bloom |chapter=Chapter 8. Modulation |page=8.7 |isbn=0-87259-144-8}}</ref>
 
=={{anchor|Practical Implementation}}Implementation==
 
===Modulation===
FM signals can be generated using either direct or indirect frequency modulation:
* Direct FM modulation can be achieved by directly feeding the message into the input of a [[Voltage-controlled oscillator|VCO]].
* For indirect FM modulation, the message signal is integrated to generate a [[phase modulation|phase-modulated signal]]. This is used to modulate a [[crystal oscillator|crystal-controlled oscillator]], and the result is passed through a [[frequency multiplier]] to give an FM signal.<ref>"Communication Systems" 4th Ed, Simon Haykin, 2001</ref>
 
===Demodulation===
{{See also|Detector_(radio)#Frequency_and_phase_modulation_detectors|l1=Detectors}}
Many FM detector circuits exist. A common method for recovering the information signal is through a [[Foster-Seeley discriminator]]. A [[phase-locked loop]] can be used as an FM demodulator. ''Slope detection'' demodulates an FM signal by using a tuned circuit which has its resonant frequency slightly offset from the carrier. As the frequency rises and falls the tuned circuit provides a changing amplitude of response, converting FM to AM. AM receivers may detect some FM transmissions by this means, although it does not provide an efficient means of [[Detector (radio)|detection]] for FM broadcasts.
 
==Applications==
 
===Magnetic tape storage===
FM is also used at [[Intermediate frequency|intermediate frequencies]] by analog [[Video cassette recorder|VCR]] systems (including [[VHS]]) to record the [[Luminance (video)|luminance]] (black and white) portions of the video signal. Commonly, the chrominance component is recorded as a conventional AM signal, using the higher-frequency FM signal as bias. FM is the only feasible method of recording the luminance ("black and white") component of video to (and retrieving video from) [[magnetic tape]] without distortion; video signals have a large range of frequency components – from a few [[hertz]] to several [[megahertz]], too wide for [[Equalization|equalizers]] to work with due to electronic noise below −60&nbsp;[[decibel|dB]]. FM also keeps the tape at saturation level, acting as a form of [[noise reduction]]; a [[audio level compression|limiter]] can mask variations in playback output, and the [[FM capture]] effect removes [[print-through]] and [[pre-echo]]. A continuous pilot-tone, if added to the signal – as was done on [[V2000]] and many Hi-band formats – can keep mechanical jitter under control and assist [[timebase correction]].
 
These FM systems are unusual, in that they have a ratio of carrier to maximum modulation frequency of less than two; contrast this with FM audio broadcasting, where the ratio is around 10,000. Consider, for example, a 6-MHz carrier modulated at a 3.5-MHz rate; by Bessel analysis, the first sidebands are on 9.5 and 2.5&nbsp;MHz and the second sidebands are on 13&nbsp;MHz and −1&nbsp;MHz. The result is a reversed-phase sideband on +1&nbsp;MHz; on demodulation, this results in unwanted output at 6−1 = 5&nbsp;MHz. The system must be designed so that this unwanted output is reduced to an acceptable level.<ref>: "FM Systems Of Exceptional Bandwidth" Proc. IEEE vol 112, no. 9, p. 1664, September 1965</ref>
 
===Sound===
FM is also used at [[audio frequency|audio frequencies]] to synthesize sound. This technique, known as [[frequency modulation synthesis|FM synthesis]], was popularized by early digital [[synthesizer]]s and became a standard feature in several generations of [[personal computer]] [[sound card]]s.
 
===Radio===
[[File:FM Broadcast Transmitter High Power.jpg|200px|thumb|An American FM radio transmitter in Buffalo, NY at WEDG]]
{{Main|FM broadcasting}}
[[Edwin Howard Armstrong]] (1890–1954) was an American electrical engineer who invented wideband frequency modulation (FM) radio.<ref>{{Cite book
|title = Principles of modern communications technology
|author = A. Michael Noll
|publisher = Artech House
|year = 2001
|isbn = 978-1-58053-284-6
|page = 104
|url = http://books.google.com/books?id=6tDEZlwiMK0C&pg=PA104
}}</ref>
He patented the regenerative circuit in 1914, the superheterodyne receiver in 1918 and the super-regenerative circuit in 1922.<ref>{{patent|US|1342885}}</ref> Armstrong presented his paper, "A Method of Reducing Disturbances in Radio Signaling by a System of Frequency Modulation", (which first described FM radio) before the New York section of the [[Institute of Radio Engineers]] on November 6, 1935. The paper was published in 1936.<ref>{{Cite journal
|first = E. H.
|last = Armstrong
|title = A Method of Reducing Disturbances in Radio Signaling by a System of Frequency Modulation
|journal = Proceedings of the IRE
|volume = 24
|issue = 5
|pages = 689–740
|publisher = IRE
|date= May 1936
|doi = 10.1109/JRPROC.1936.227383
}}</ref>
 
As the name implies, wideband FM (WFM) requires a wider [[signal bandwidth]] than [[amplitude modulation]] by an equivalent modulating signal; this also makes the signal more robust against [[Noise (radio)|noise]] and [[Interference (communication)|interference]]. Frequency modulation is also more robust against signal-amplitude-fading phenomena. As a result, FM was chosen as the modulation standard for high frequency, [[high fidelity]] [[radio]] transmission, hence the term "[[FM radio]]" (although for many years the [[BBC]] called it "VHF radio" because commercial FM broadcasting uses part of the [[VHF]] band—the [[FM broadcast band]]). FM [[receiver (radio)|receivers]] employ a special [[Detector (radio)|detector]] for FM signals and exhibit a phenomenon known as the ''[[capture effect]]'', in which the [[Tuner (radio)|tuner]] "captures" the stronger of two stations on the same frequency while rejecting the other (compare this with a similar situation on an AM receiver, where both stations can be heard simultaneously). However, [[frequency drift]] or a lack of [[Electronic selectivity|selectivity]] may cause one station to be overtaken by another on an [[adjacent channel]]. Frequency [[drift (telecommunication)|drift]] was a problem in early (or inexpensive) receivers; inadequate selectivity may affect any tuner.
 
An FM signal can also be used to carry a [[stereophonic sound|stereo]] signal; this is done with [[multiplexing]] and demultiplexing before and after the FM process. The FM modulation and demodulation process is identical in stereo and monaural processes. A high-efficiency radio-frequency [[switching amplifier]] can be used to transmit FM signals (and other [[constant envelope|constant-amplitude signals]]). For a given signal strength (measured at the receiver antenna), switching amplifiers use [[low-power electronics|less battery power]] and typically cost less than a [[linear amplifier]]. This gives FM another advantage over other modulation methods requiring linear amplifiers, such as AM and [[Quadrature amplitude modulation|QAM]].
 
FM is commonly used at [[VHF]] [[radio frequencies]] for [[high-fidelity]] [[radio broadcasting|broadcasts]] of music and [[Speech communication|speech]]. Analog TV sound is also broadcast using FM. Narrowband FM is used for voice communications in commercial and [[amateur radio]] settings. In broadcast services, where audio fidelity is important, wideband FM is generally used. In [[two-way radio]], narrowband FM (NBFM) is used to conserve bandwidth for land mobile, marine mobile and other radio services.
 
==See also==
* [[Amplitude modulation]]
* [[Continuous-wave frequency-modulated radar]]
* [[Chirp]]
* [[FM broadcasting]]
* [[FM stereo]]
* [[FM-UWB]] (FM and Ultra Wideband)
* [[History of radio]]
* [[Modulation]], for a list of other modulation techniques
 
==References==
{{Reflist|35em}}


==Further reading==
==Further reading==
* Robert J. Silva: [http://radchem.nevada.edu/classes/rdch710/files/Fm%20to%20Lr.pdf Fermium, Mendelevium, Nobelium, and Lawrencium], in: Lester R. Morss, Norman M. Edelstein, Jean Fuger (Hrsg.): ''The Chemistry of the Actinide and Transactinide Elements'', Springer, Dordrecht 2006; ISBN 1-4020-3555-1, p.&nbsp;1621–1651; {{DOI|10.1007/1-4020-3598-5_13}}.
* A. Bruce Carlson. ''Communication Systems, 4th edition.'' McGraw-Hill Science/Engineering/Math. 2001. ISBN 0-07-011127-8, ISBN 978-0-07-011127-1.
* Seaborg, G.T. (ed.) (1978) ''[http://www.escholarship.org/uc/item/92g2p7cd.pdf Proceedings of the Symposium Commemorating the 25th Anniversary of Elements 99 and 100]'', 23 January 1978, Report LBL-7701
* Gary L. Frost. ''Early FM Radio: Incremental Technology in Twentieth-Century America.'' Baltimore: Johns Hopkins University Press, 2010. ISBN 0-8018-9440-9, ISBN 978-0-8018-9440-4.
* ''[[Gmelins Handbuch der anorganischen Chemie]]'', System Nr. 71, Transurane: Teil A 1 II, p.&nbsp;19–20; Teil A 2, p.&nbsp;47; Teil B 1, p.&nbsp;84.
* Ken Seymour, AT&T Wireless (Mobility). ''Frequency Modulation, The Electronics Handbook, pp 1188-1200, 1st Edition, 1996. 2nd Edition, 2005'' CRC Press, Inc., ISBN 0-8493-8345-5 (1st Edition).
 
==External links==
{{Commons|Fermium}}
{{Wiktionary|fermium}}
* [http://www.periodicvideos.com/videos/100.htm Fermium] at ''[[The Periodic Table of Videos]]'' (University of Nottingham)


{{Clear}}
{{Analogue TV transmitter topics}}
{{compact periodic table}}
{{Telecommunications}}
{{Chemical elements named after scientists}}
{{Audio broadcasting}}


[[Category:Chemical elements]]
[[Category:Radio modulation modes]]
[[Category:Actinides]]
[[Category:Synthetic elements]]
[[Category:Fermium]]
[[Category:Enrico Fermi]]

Revision as of 16:01, 8 August 2014

Template:Modulation techniques

Animation of audio, AM and FM signals
A signal may be carried by an AM or FM radio wave.

In telecommunications and signal processing, frequency modulation (FM) is the encoding of information in a carrier wave by varying the instantaneous frequency of the wave. (Compare with amplitude modulation, in which the amplitude of the carrier wave varies, while the frequency remains constant.)

In analog signal applications, the difference between the instantaneous and the base frequency of the carrier is directly proportional to the instantaneous value of the input-signal amplitude.

Digital data can be encoded and transmitted via a carrier wave by shifting the carrier's frequency among a predefined set of frequencies—a technique known as frequency-shift keying (FSK). FSK is widely used in modems and fax modems, and can also be used to send Morse code.[1] Radioteletype also uses FSK.[2]

Frequency modulation is used in radio, telemetry, radar, seismic prospecting, and monitoring newborns for seizures via EEG.[3] FM is widely used for broadcasting music and speech, two-way radio systems, magnetic tape-recording systems and some video-transmission systems. In radio systems, frequency modulation with sufficient bandwidth provides an advantage in cancelling naturally-occurring noise.

Frequency modulation is known as phase modulation when the carrier phase modulation is the time integral of the FM signal.Template:Clarify

Theory

If the information to be transmitted (i.e., the baseband signal) is and the sinusoidal carrier is , where fc is the carrier's base frequency, and Ac is the carrier's amplitude, the modulator combines the carrier with the baseband data signal to get the transmitted signal:

In this equation, is the instantaneous frequency of the oscillator and is the frequency deviation, which represents the maximum shift away from fc in one direction, assuming xm(t) is limited to the range ±1.

While most of the energy of the signal is contained within fc ± fΔ, it can be shown by Fourier analysis that a wider range of frequencies is required to precisely represent an FM signal. The frequency spectrum of an actual FM signal has components extending infinitely, although their amplitude decreases and higher-order components are often neglected in practical design problems.[4]

Sinusoidal baseband signal

Mathematically, a baseband modulated signal may be approximated by a sinusoidal continuous wave signal with a frequency fm. The integral of such a signal is:

In this case, the expression for y(t) above simplifies to:

where the amplitude of the modulating sinusoid is represented by the peak deviation (see frequency deviation).

The harmonic distribution of a sine wave carrier modulated by such a sinusoidal signal can be represented with Bessel functions; this provides the basis for a mathematical understanding of frequency modulation in the frequency domain.

Modulation index

As in other modulation systems, the value of the modulation index indicates by how much the modulated variable varies around its unmodulated level. It relates to variations in the carrier frequency:

where is the highest frequency component present in the modulating signal xm(t), and is the peak frequency-deviation—i.e. the maximum deviation of the instantaneous frequency from the carrier frequency. If , the modulation is called narrowband FM, and its bandwidth is approximately .

If , the modulation is called wideband FM and its bandwidth is approximately . While wideband FM uses more bandwidth, it can improve the signal-to-noise ratio significantly; for example, doubling the value of , while keeping constant, results in an eight-fold improvement in the signal-to-noise ratio.[5] (Compare this with Chirp spread spectrum, which uses extremely wide frequency deviations to achieve processing gains comparable to traditional, better-known spread-spectrum modes).

With a tone-modulated FM wave, if the modulation frequency is held constant and the modulation index is increased, the (non-negligible) bandwidth of the FM signal increases but the spacing between spectra remains the same; some spectral components decrease in strength as others increase. If the frequency deviation is held constant and the modulation frequency increased, the spacing between spectra increases.

Frequency modulation can be classified as narrowband if the change in the carrier frequency is about the same as the signal frequency, or as wideband if the change in the carrier frequency is much higher (modulation index >1) than the signal frequency. [6] For example, narrowband FM is used for two way radio systems such as Family Radio Service, in which the carrier is allowed to deviate only 2.5 kHz above and below the center frequency with speech signals of no more than 3.5 kHz bandwidth. Wideband FM is used for FM broadcasting, in which music and speech are transmitted with up to 75 kHz deviation from the center frequency and carry audio with up to a 20-kHz bandwidth.

Bessel functions

For the case of a carrier modulated by a single sine wave, the resulting frequency spectrum can be calculated using Bessel functions of the first kind, as a function of the sideband number and the modulation index. The carrier and sideband amplitudes are illustrated for different modulation indices of FM signals. For particular values of the modulation index, the carrier amplitude becomes zero and all the signal power is in the sidebands.[4]

Since the sidebands are on both sides of the carrier, their count is doubled, and then multiplied by the modulating frequency to find the bandwidth. For example, 3 kHz deviation modulated by a 2.2 kHz audio tone produces a modulation index of 1.36. Examining the chart shows this modulation index will produce three sidebands. These three sidebands, when doubled, gives us (6 * 2.2 kHz) or a 13.2 kHz required bandwidth.

Modulation
index
Sideband
Carrier 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16
0.00 1.00
0.25 0.98 0.12
0.5  0.94 0.24 0.03
1.0  0.77 0.44 0.11 0.02
1.5  0.51 0.56 0.23 0.06 0.01
2.0  0.22 0.58 0.35 0.13 0.03
2.41 0    0.52 0.43 0.20 0.06 0.02
2.5  −0.05 0.50 0.45 0.22 0.07 0.02 0.01
3.0  −0.26 0.34 0.49 0.31 0.13 0.04 0.01
4.0  −0.40 −0.07 0.36 0.43 0.28 0.13 0.05 0.02
5.0  −0.18 −0.33 0.05 0.36 0.39 0.26 0.13 0.05 0.02
5.53 0    −0.34 −0.13 0.25 0.40 0.32 0.19 0.09 0.03 0.01
6.0  0.15 −0.28 −0.24 0.11 0.36 0.36 0.25 0.13 0.06 0.02
7.0  0.30 0.00 −0.30 −0.17 0.16 0.35 0.34 0.23 0.13 0.06 0.02
8.0  0.17 0.23 −0.11 −0.29 −0.10 0.19 0.34 0.32 0.22 0.13 0.06 0.03
8.65 0    0.27 0.06 −0.24 −0.23 0.03 0.26 0.34 0.28 0.18 0.10 0.05 0.02
9.0  −0.09 0.25 0.14 −0.18 −0.27 −0.06 0.20 0.33 0.31 0.21 0.12 0.06 0.03 0.01
10.0  −0.25 0.04 0.25 0.06 −0.22 −0.23 −0.01 0.22 0.32 0.29 0.21 0.12 0.06 0.03 0.01
12.0  0.05 −0.22 −0.08 0.20 0.18 −0.07 −0.24 −0.17 0.05 0.23 0.30 0.27 0.20 0.12 0.07 0.03 0.01

Carson's rule

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A rule of thumb, Carson's rule states that nearly all (~98 percent) of the power of a frequency-modulated signal lies within a bandwidth of:

where , as defined above, is the peak deviation of the instantaneous frequency from the center carrier frequency .

Noise Reduction

A major advantage of FM in a communications circuit, compared for example with AM, is the possibility of improved Signal-to-noise ratio (SNR). Compared with an optimum AM scheme, FM typically has poorer SNR below a certain signal level called the noise threshold, but above a higher level – the full improvement or full quieting threshold – the SNR is much improved over AM. The improvement depends on modulation level and deviation. For typical voice communications channels, improvements are typically 5-15 dB. FM broadcasting using wider deviation can achieve even greater improvements. Additional techniques, such as pre-emphasis of higher audio frequencies with corresponding de-emphasis in the receiver, are generally used to improve overall SNR in FM circuits. Since FM signals have constant amplitude, FM receivers normally have limiters that remove AM noise, further improving SNR.[7][8]

<Practical Implementation>...</Practical Implementation>Implementation

Modulation

FM signals can be generated using either direct or indirect frequency modulation:

Demodulation

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Applications

Magnetic tape storage

FM is also used at intermediate frequencies by analog VCR systems (including VHS) to record the luminance (black and white) portions of the video signal. Commonly, the chrominance component is recorded as a conventional AM signal, using the higher-frequency FM signal as bias. FM is the only feasible method of recording the luminance ("black and white") component of video to (and retrieving video from) magnetic tape without distortion; video signals have a large range of frequency components – from a few hertz to several megahertz, too wide for equalizers to work with due to electronic noise below −60 dB. FM also keeps the tape at saturation level, acting as a form of noise reduction; a limiter can mask variations in playback output, and the FM capture effect removes print-through and pre-echo. A continuous pilot-tone, if added to the signal – as was done on V2000 and many Hi-band formats – can keep mechanical jitter under control and assist timebase correction.

These FM systems are unusual, in that they have a ratio of carrier to maximum modulation frequency of less than two; contrast this with FM audio broadcasting, where the ratio is around 10,000. Consider, for example, a 6-MHz carrier modulated at a 3.5-MHz rate; by Bessel analysis, the first sidebands are on 9.5 and 2.5 MHz and the second sidebands are on 13 MHz and −1 MHz. The result is a reversed-phase sideband on +1 MHz; on demodulation, this results in unwanted output at 6−1 = 5 MHz. The system must be designed so that this unwanted output is reduced to an acceptable level.[10]

Sound

FM is also used at audio frequencies to synthesize sound. This technique, known as FM synthesis, was popularized by early digital synthesizers and became a standard feature in several generations of personal computer sound cards.

Radio

An American FM radio transmitter in Buffalo, NY at WEDG

Mining Engineer (Excluding Oil ) Truman from Alma, loves to spend time knotting, largest property developers in singapore developers in singapore and stamp collecting. Recently had a family visit to Urnes Stave Church. Edwin Howard Armstrong (1890–1954) was an American electrical engineer who invented wideband frequency modulation (FM) radio.[11] He patented the regenerative circuit in 1914, the superheterodyne receiver in 1918 and the super-regenerative circuit in 1922.[12] Armstrong presented his paper, "A Method of Reducing Disturbances in Radio Signaling by a System of Frequency Modulation", (which first described FM radio) before the New York section of the Institute of Radio Engineers on November 6, 1935. The paper was published in 1936.[13]

As the name implies, wideband FM (WFM) requires a wider signal bandwidth than amplitude modulation by an equivalent modulating signal; this also makes the signal more robust against noise and interference. Frequency modulation is also more robust against signal-amplitude-fading phenomena. As a result, FM was chosen as the modulation standard for high frequency, high fidelity radio transmission, hence the term "FM radio" (although for many years the BBC called it "VHF radio" because commercial FM broadcasting uses part of the VHF band—the FM broadcast band). FM receivers employ a special detector for FM signals and exhibit a phenomenon known as the capture effect, in which the tuner "captures" the stronger of two stations on the same frequency while rejecting the other (compare this with a similar situation on an AM receiver, where both stations can be heard simultaneously). However, frequency drift or a lack of selectivity may cause one station to be overtaken by another on an adjacent channel. Frequency drift was a problem in early (or inexpensive) receivers; inadequate selectivity may affect any tuner.

An FM signal can also be used to carry a stereo signal; this is done with multiplexing and demultiplexing before and after the FM process. The FM modulation and demodulation process is identical in stereo and monaural processes. A high-efficiency radio-frequency switching amplifier can be used to transmit FM signals (and other constant-amplitude signals). For a given signal strength (measured at the receiver antenna), switching amplifiers use less battery power and typically cost less than a linear amplifier. This gives FM another advantage over other modulation methods requiring linear amplifiers, such as AM and QAM.

FM is commonly used at VHF radio frequencies for high-fidelity broadcasts of music and speech. Analog TV sound is also broadcast using FM. Narrowband FM is used for voice communications in commercial and amateur radio settings. In broadcast services, where audio fidelity is important, wideband FM is generally used. In two-way radio, narrowband FM (NBFM) is used to conserve bandwidth for land mobile, marine mobile and other radio services.

See also

References

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Further reading

  • A. Bruce Carlson. Communication Systems, 4th edition. McGraw-Hill Science/Engineering/Math. 2001. ISBN 0-07-011127-8, ISBN 978-0-07-011127-1.
  • Gary L. Frost. Early FM Radio: Incremental Technology in Twentieth-Century America. Baltimore: Johns Hopkins University Press, 2010. ISBN 0-8018-9440-9, ISBN 978-0-8018-9440-4.
  • Ken Seymour, AT&T Wireless (Mobility). Frequency Modulation, The Electronics Handbook, pp 1188-1200, 1st Edition, 1996. 2nd Edition, 2005 CRC Press, Inc., ISBN 0-8493-8345-5 (1st Edition).

Template:Analogue TV transmitter topics Template:Telecommunications Template:Audio broadcasting

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  2. 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

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  3. B. Boashash, editor, “Time-Frequency Signal Analysis and Processing – A Comprehensive Reference”, Elsevier Science, Oxford, 2003; ISBN 0-08-044335-4
  4. 4.0 4.1 T.G. Thomas, S. C. Sekhar Communication Theory, Tata-McGraw Hill 2005, ISBN 0070590915 page 136
  5. Der, Lawrence, Ph.D., Frequency Modulation (FM) Tutorial, http://www.silabs.com/Marcom%20Documents/Resources/FMTutorial.pdf, Silicon Laboratories, Inc., accessed 2013 February 24, p. 5
  6. B. P. Lathi, Communication Systems, John Wiley and Sons, 1968 ISBN 0-471-51832-8, p, 214–217
  7. 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

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  8. 20 year-old Real Estate Agent Rusty from Saint-Paul, has hobbies and interests which includes monopoly, property developers in singapore and poker. Will soon undertake a contiki trip that may include going to the Lower Valley of the Omo.

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  9. "Communication Systems" 4th Ed, Simon Haykin, 2001
  10. : "FM Systems Of Exceptional Bandwidth" Proc. IEEE vol 112, no. 9, p. 1664, September 1965
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  12. Template:Patent
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