DC Circuits: Why Is Voltage Across Inductor 0 at Steady State?

AI Thread Summary
In a DC steady state, an inductor behaves like a short circuit, resulting in zero voltage across it. According to Ohm's law, with resistance at zero, the voltage must also be zero. As the current through the inductor reaches its maximum or minimum and stops changing, the rate of change of current (di/dt) becomes zero. This leads to a voltage drop of zero across the inductor, confirming that V = L(di/dt) equals zero volts. Understanding these principles clarifies the behavior of inductors in steady-state DC circuits.
dleccord
Messages
10
Reaction score
0
if the inductor is at dc steady state, the inductor would act like a short.

in this case, why would the voltage across the inductor be zero?

thanks in advance.
 
Physics news on Phys.org
According to Ohm's law E=IR if R=0 (a short) then E is also 0.
 
dleccord said:
if the inductor is at dc steady state, the inductor would act like a short.

in this case, why would the voltage across the inductor be zero?

thanks in advance.

A perfect electrical short means there is no electrical resistance. If there is no electrical resistance then there can be no voltage across the short. E=IR or Voltage=Amps times Resistance. As you can see as the resistance decreases so does the voltage.
 
wow thanks, i can't believe i didnt look at ohm's law's simplest.

i was looking for V=Ldi/dt, trying to figure that out but confused myself.

thanks ruko.
 
At t=\infty, the current through the inductor is maximum (for "charging" phase) or minimum (for "discharging" phase) and is no longer changing. Therefore, di/dt=0 amps/sec, so the voltage drop across the inductor is V= L(di/dt) = 0 volts.
 
I was using the Smith chart to determine the input impedance of a transmission line that has a reflection from the load. One can do this if one knows the characteristic impedance Zo, the degree of mismatch of the load ZL and the length of the transmission line in wavelengths. However, my question is: Consider the input impedance of a wave which appears back at the source after reflection from the load and has traveled for some fraction of a wavelength. The impedance of this wave as it...
Back
Top