DC voltage across the inductor?

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Applying DC voltage across an inductor primarily results in a voltage drop across the series internal resistance of the coil, as the reactance term becomes negligible at DC. The impedance of an inductor combines both resistance and reactance, expressed as Z = R + jωL, but at DC, the reactance (jωL) is zero. Consequently, the current through the inductor can be described by the equation i = V/R, assuming R is the only factor affecting the current. If R is zero, as in superconducting conditions, the current would theoretically be infinite, represented as i = Vt/L. In contrast, applying AC voltage introduces frequency-dependent reactance, increasing the perceived resistance as frequency rises.
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what happens when u apply DC voltage across the inductor? i.e is the voltage drop only across the series internal resistance of the coil? can we just determine this resistance by simply saying: V_supply = I x r(series)? or do we have to include the inductance?
 
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hint: Do you know the impedance of an inductor?
 


Ouabache said:
hint: Do you know the impedance of an inductor?

whats an impedance?
do you mean X_L=wL?
 


V = Ri + L*di/dt

i = (V/R)*(1 - exp(-Rt/L))

If R=0 (superconducting), then

i = Vt/L

Claude
 


Before we get too far along, I hope you have more in your circuit besides the inductor, otherwise what do you think would happen when you apply a voltage across a coil of wire?
php said:
whats an impedance?
do you mean X_L=wL?
You're on the right track, however you've given only the inductive reactance.
The impedance Z of an inductor includes both real (pure resistance) and imaginary terms (reactance).
Z = R + jX_L = R+ j \omega L
So the voltage across it would be? V = IZ = I (R + j \omega L)

Since you are applying only a DC voltage (no frequency component), what happens to the reactance term?
 


Most likely the wire will get hot. You are right, at DC the resistance is only the series resistance of the wire.

If you were to apply an AC signal then it is different. As you increase the frequency the perceived resistance to the AC signal would increase. Many small signal inductors are rated at 100MHz. The rating will be something like 300 ohms at 100MHz meaning that to the source, the line the signal is traveling on will look like a 300 ohm resistor. This is in magnitude impedance format, which is the perceived resistance. At slightly over DC the perceived resistance will be near zero ohms, as the frequency increases, so will the perceived resistance. There is a point at which the resistance will reach a maximum and then it will go back down

There are a few simplifications here but the concept is sound.
 
It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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