vorcil
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I wanted to see the proof for the energy stored in an inductor equation was,
But i had trouble understand how part of this integration works i.e my math sucks
-
given \frac{dw}{dt} = iv
and VL = L \frac{di}{dt}
-
solving i get,
subtituting the ldt/dt for v
\frac{dw}{dt} = i L \frac{di}{dt}
the dt's cancel out
dw = i L di
then to find the work done I integrate the equation,
\int dw = \int i L di
and the integral of \int dw = w
but how do I integrate
\int i L di ?
I know L, the inductance of the inductor is constant so can pull that outside the integral,
and get
L \int i di
But what do I do here?
integrating i I get \frac{1}{2} i ^2 * i according to the integration rules I've learnt
but everyone knows that the energy inside an inductor equation is
wL = \frac{1}{2} L i^2,
but my integration shows it is \frac{1}{2} L i^3
can someone please explain it to me
But i had trouble understand how part of this integration works i.e my math sucks
-
given \frac{dw}{dt} = iv
and VL = L \frac{di}{dt}
-
solving i get,
subtituting the ldt/dt for v
\frac{dw}{dt} = i L \frac{di}{dt}
the dt's cancel out
dw = i L di
then to find the work done I integrate the equation,
\int dw = \int i L di
and the integral of \int dw = w
but how do I integrate
\int i L di ?
I know L, the inductance of the inductor is constant so can pull that outside the integral,
and get
L \int i di
But what do I do here?
integrating i I get \frac{1}{2} i ^2 * i according to the integration rules I've learnt
but everyone knows that the energy inside an inductor equation is
wL = \frac{1}{2} L i^2,
but my integration shows it is \frac{1}{2} L i^3
can someone please explain it to me