How to Simplify Inductor Expressions Using Calculus?

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SUMMARY

This discussion focuses on simplifying inductor expressions using calculus, specifically addressing the integral of current over time. The key expression derived is L∫_{−∞}^t i(τ)(di/dτ)dτ = (1/2)L(i^2(t)), assuming that the limit of current i(τ) approaches zero as τ approaches infinity. The distinction between treating "Li" as a constant times a function versus a single function is crucial for accurate simplification.

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  • Understanding of calculus, particularly integration techniques.
  • Familiarity with electrical engineering concepts, specifically inductance.
  • Knowledge of current as a function of time, denoted as i(t).
  • Basic grasp of limits in calculus.
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xconwing
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How can you get from the first expression to the second. I've done calculus, just need a fresher. I don't know how to deal with the dt/dt

thanks
 
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What you have written is not clear. Is "Li" a single function or is this the constant, L, times the function i?

If the latter this is easy. [itex]L\int_{-\infty}^t i(\tau) (di/d\tau)d\tau= L\int_{-\infty}^t i di = L\left[(1/2)i^2(\tau)\right]_{\infty}^t[/itex] which, if [itex]\lim_{\tau\to\infty} i(\tau)= 0[/itex] is [itex](1/2)i^2(\tau)[/itex]

If Li is a single function, then it is NOT always true.
 
Yeah, L is the constant value of the inductance. i(t) is the current as a function of time.
 

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