Current through a single inductor

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In a circuit with two parallel inductors (5H and 20H) and a resistive network, the discussion focuses on understanding the current through each inductor after a switch is opened. The derived voltage and current equations indicate that the integral of voltage divided by inductance, minus the initial current, yields the current through each inductor over time. The mathematical relationship stems from the fundamental V/I characteristics of inductors, expressed as di/dt = v/L. The conversation highlights that while combined inductance can simplify analysis, the basic laws still apply to individual components. This approach is valid as long as the voltage across each inductor is appropriately accounted for.
modulation
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Homework Statement



Ok, so this isn't a question of how to solve, but rather why the solution works.

Say you have a circuit with 2 inductors in parallel, a 5H and a 20H, in parallel to the inductors is a resistive network with a resistance of 8Ω, and a switch, which has been closed long enough for the inductors to reach DC steady state. The power source is not shown, but initially there is a current through each inductor, 8A through the 5H, and 4A through the 20H. When the switch is opened, the problem asks to find the voltage and current for the inductors, as well as the current through each individual inductor.


Homework Equations



So the solution for the voltage is v(t)=96(e)^{-2t}
, and current for both inductors is i(t)=12(e)^{-2t}

The solution to the current through the individual 5H inductor is
i_1(t)= \frac{1}{5} \int_{0}^{t} 96(e)^{-2x}dx -8

and for the 20H inductor is
i_2(t)= \frac{1}{20} \int_{0}^{t} 96(e)^{-2x}dx -4



The Attempt at a Solution



So what I do not understand is, how does the integral of the voltage, divided by the inductance, subtract the initial current, give the current through an individual inductor over time??
Really curious as to how this is possible mathematically and why??
Am I missing something?
 
Last edited:
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That follows fundamentally from the V/I characteristics of an inductor.

\frac{di}{dt} = v/L

so

i(t) = \frac{1}{L} \int_0^t v(\lambda) \, d\lambda + i(0)

BTW. The sign of the voltage in your example is technically inconsistent with the direction you're using for current, hence the reason I used "+ i(0)" instead of the minus you had.
 
So even though the voltage was derived from a combined inductance, you can simply divide by the individual inductance to get the current?
<br /> \frac{di}{dt} = v/L<br />

It is just odd , that first off the combined inductance is the product/sum, and then the voltage is the i(t)*R.
Strange that division can undo this. I have searched in my textbook for a more detailed proof of this but no luck.
 
Last edited:
modulation said:
So even though the voltage was derived from a combined inductance, you can simply divide by the individual inductance to get the current?
<br /> \frac{di}{dt} = v/L<br />

It is just odd , that first off the combined inductance is the product/sum, and then the voltage is the i(t)*R.
Strange that division can undo this. I have searched in my textbook for a more detailed proof of this but no luck.

Sometimes it's just easier to lump some components together before solving a circuit. This doesn't mean that the basic circuit laws don't still hold for each individual element however.

There are times when you do run into problems here, but this only when the voltages you need to analyze the individual elements get "swallowed up" in the lumping together process. This sometimes happens with Thevenin equivalents for example, but it's not an issue in this case.
 

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