Transition state theory: Difference between revisions

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'''[[Inductance]]''' is a measure of the amount of [[magnetic flux]] produced for a given [[electric current]]. The term was coined by [[Oliver Heaviside]] in February [[1886]]. The [[SI]] unit of inductance is the [[Henry (unit)|henry]] (symbol: H), in honour of [[Joseph Henry]]. The symbol ''L'' is used for inductance, possibly in honour of the physicist [[Heinrich Lenz]].
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The inductance has the following relationship:
:<math>L= \frac{\Phi}{i}</math>
where; ''L'' is the inductance in [[Henry (unit)|henrys]], ''i'' is the current in [[ampere]]s, ''Φ'' is the magnetic flux in [[Weber (unit)|weber]]s. Strictly speaking, the quantity just defined is called ''self-inductance'', because the magnetic field is created solely by the conductor that carries the current.
 
When a conductor is coiled upon itself N number of times around the same axis (forming a [[solenoid]]), the current required to produce a given amount of flux is reduced by a factor of N compared to a single turn of wire.  Thus, the inductance of a coil of wire of N turns is given by:
 
:<math>L= \frac{\lambda}{i} = N\frac{\Phi}{i}</math>
where, <math>\lambda</math> is the total 'flux linkage'.
 
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Latest revision as of 18:10, 31 July 2014

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