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24 ELECTRIC DISCHARGES, WAVB8 AND
I rl
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(6)
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The same equations may bo derived directly by the integration
of the differential equation: |
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(7)
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where Lj: is the inductance voltap, n the ri^wt
and their sum equals zero, an the «oil i« nhort-eircmitetl
Equation (7) transpoBod gives
di r u
nr - — 7 <ft
t L J
hence
i « - 7 t + logC,
ij |
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and, as for t » 0: i m t*0) it is: C •» i§;
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14. Usually single-energy tratwientu last an
and thereby become of onginaaring importtai^c^ only in highly inductive circuits, as motor fields, magnate, oto.
To get an idea on the duration of mush inngnetki tnai»k*iit«#
consider a motor field:
A A-polar motor has 8 ml (megalincn) of mapiatici flux jn^r
pole, produced by 6000 ampere turns m*m.f. per polo, arid pates normally 500 watts in the field oxdtatioDu
That is, if to » field-exciting current, n » number of fli*M tiirnn
per pole, r « resistance, Md JD - inductance of the fielck«dting circuit, it is
ioV » 500,
hence
„ 500
* *** ""Y1*^*11*
to1
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