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=== Inductance === {{See also|Inductance with physical symmetry}} As shown above, the magnetic flux density <math>B</math> within the coil is practically constant and given by :<math>B = \mu_0 \frac{NI}{l},</math> where ''μ''<sub>0</sub> is the [[Permeability (electromagnetism)|magnetic constant]], <math>N</math> the number of turns, <math>I</math> the current and <math>l</math> the length of the coil. Ignoring end effects, the total [[magnetic flux]] through the coil is obtained by multiplying the flux density <math>B</math> by the cross-section area <math>A</math>: :<math>\Phi = \mu_0 \frac{NIA}{l}.</math> Combining this with the definition of [[inductance]] :<math>L = \frac{N \Phi}{I},</math> the inductance of a solenoid follows as :<math>L = \mu_0 \frac{N^2A}{l}.</math> A table of inductance for short solenoids of various diameter to length ratios has been calculated by Dellinger, Whittmore, and Ould.<ref>{{cite book |url= https://books.google.com/books?id=Xn8KbsgeFrwC&pg=PA248 |title=Radio Instruments and Measurements |author1=D. Howard Dellinger |author2=L. E. Whittmore |author3=R. S. Ould |name-list-style=amp |year= 1924 |journal=NBS Circular |volume= C74 |access-date=7 September 2009 |isbn=9780849302527 }}</ref> This, and the inductance of more complicated shapes, can be derived from [[Maxwell's equations]]. For rigid air-core coils, inductance is a function of coil geometry and number of turns, and is independent of current. Similar analysis applies to a solenoid with a magnetic core, but only if the length of the coil is much greater than the product of the relative [[Permeability (electromagnetism)|permeability]] of the magnetic core and the diameter. That limits the simple analysis to low-permeability cores, or extremely long thin solenoids. The presence of a core can be taken into account in the above equations by replacing the magnetic constant ''μ<sub>0</sub>'' with ''μ'' or ''μ<sub>0</sub>μ<sub>r</sub>'', where ''μ'' represents permeability and ''μ<sub>r</sub>'' [[Permeability (electromagnetism)|relative permeability]]. Note that since the permeability of [[ferromagnetic]] materials changes with applied magnetic flux, the inductance of a coil with a ferromagnetic core will generally vary with current.
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