How Do I Correctly Integrate \(\int i L \, di\) for Inductor Energy Calculation?

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The discussion focuses on the integration process for calculating energy stored in an inductor, specifically the equation \( \int i L \, di \). A participant initially struggles with integrating \( i \) with respect to \( i \) and mistakenly believes the result is \( \frac{1}{2} L i^3 \) instead of the correct \( \frac{1}{2} L i^2 \). Clarifications are provided on the importance of understanding the variable of integration, emphasizing that \( dx \) indicates the variable being integrated. The conversation highlights the need to properly apply integration rules and includes reminders about including the constant of integration. Ultimately, the discussion reinforces the correct approach to integrating functions in the context of inductor energy calculations.
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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
 
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First I think this equation

<br /> VL = L \frac{di}{dt} <br />

should be

V=L\frac{di}{dt}

Well you got as far as W= L∫i di.


Now remember the rules of integration

\int x^n dx = \frac{x^{n+1}}{n+1}

so what does your integral become?
 
when I wrote VL i ment the voltage across the inductor Vl,

\int i^1 di = \frac{i^(1+1)}{1+1}

I just always assumed that the integral of something \int di = i
or \int dx = x

since when I integrate, \int dw = L \int i di
I get w = \frac{1}{2} L i^2

-

I can see now that the di disappears, and all I'm integrating is i, which I can do easily
 
vorcil said:
I just always assumed that the integral of something \int di = i
or \int dx = x

yes those are correct, but you were integrating i w.r.t i. Not just 1.
 
rock.freak667 said:
yes those are correct, but you were integrating i w.r.t i. Not just 1.

so when I integrate x w.r.t x, I get the integral of x only?

\int x dx = \int x = \frac{1}{2}x^2

but when I integrate dx,

\int dx = x ?

so that dx after an equation means with respect to dx?
like in an integral equation, \int x dx is means integrating x with respect to x?
 
vorcil said:
so when I integrate x w.r.t x, I get the integral of x only?

\int x dx = \int x = \frac{1}{2}x^2

but when I integrate dx,

\int dx = x ?

so that dx after an equation means with respect to dx?
like in an integral equation, \int x dx is means integrating x with respect to x?

Yes. But the 'dx' does not just disappear.

\int 1 dx = x+C


\int x dx = \frac{1}{2}x^2 +C

(constant C for indefinite integrals)
 
ok thanks, I'll figure out how differential/integral equations are set up properly

instead of just using my cheap way and plugging everything into

<br /> \int x^n dx = \frac{x^{n+1}}{n+1}<br />
 
The differential part in an integral tells you what the variable of integration is. Don't leave it out as you did here. Also, don't leave out the constant of integration.
vorcil said:
\int x = \frac{1}{2}x^2
It should be
\int x dx = \frac{1}{2}x^2 + C

In this integral, a is the variable of integration.
\int a da = \frac{1}{2}a^2 + C

In this one, x is the variable of integration, and a is just a constant.
\int a dx = a \int dx = ax + C
In the integral above I used a property of integrals - the integral of a constant times a function is the constant times the integral of the function. Here the function is 1.
 
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