Inductors are not categorized in ohms. Inductors are categorized by their inductance measured in henrys. This is a measurement that can be measured by using a special meter. The only thing that the resistance will tell you is that the coil in not open circuited. So there is no real way to know if it is still good.
a bowl of cereal
The total impedance ( Z_t ) of a circuit with a resistor (R) and inductor (L) in series can be calculated using the formula ( Z_t = R + jX_L ), where ( X_L = \omega L ) is the inductive reactance. For a 100-ohm resistor and a 100-ohm inductor, the impedance will depend on the frequency ( f ) of the AC current. If the inductance and frequency are such that ( X_L = 100 ) ohms (e.g., at a specific frequency), then ( Z_t = 100 + j100 ) ohms, resulting in a magnitude of ( Z_t = \sqrt{100^2 + 100^2} = 100\sqrt{2} ) ohms.
An inductor has two properties. The first is resistance(measured in ohms), which is due to the length, cross-sectional area, and resistivity of the conductor from which it is wound. The second is inductance (measured in henrys), which is due to the length of the inductor, its cross-sectional area, the number of turns, and the permeability of its core.The inductor's resistance limits the value of current flowing through the inductor. The inductor's inductance opposes any change in current.
The resulting maximum current is limited by the resistance of the inductor. As the current increases from zero to that maximum value, its expanding magnetic field induces a voltage into the inductor which opposes the rise in that current. So, instead of reaching its maximum value instantaneously, it takes some time -determined by the equation:time to maximum current = 5 L / R (seconds)where L = inductance of inductor in henrys, and R = resistance of inductor in ohms.
.513 ohms is simply 0.513 ohms. The unit "ohm" measures electrical resistance, and the numerical value remains the same regardless of how it's expressed. Therefore, there are 0.513 ohms.
a bowl of cereal
Ohms, resistance in an inductor increases as the frequency of the AC signal increases, this "artificial resistance" is called impedence, and it is measured in ohms
In an ideal inductor, no, there is no voltage induced across an inductor unless the current in the inductor is changing. However, since there are no ideal inductors nor power supplies, eventually an inductor will draw a constant current, i.e. the limit of the power supply; and, since no inductor has zero ohms at equilibrium, that current will translate to voltage.
The total impedance ( Z_t ) of a circuit with a resistor (R) and inductor (L) in series can be calculated using the formula ( Z_t = R + jX_L ), where ( X_L = \omega L ) is the inductive reactance. For a 100-ohm resistor and a 100-ohm inductor, the impedance will depend on the frequency ( f ) of the AC current. If the inductance and frequency are such that ( X_L = 100 ) ohms (e.g., at a specific frequency), then ( Z_t = 100 + j100 ) ohms, resulting in a magnitude of ( Z_t = \sqrt{100^2 + 100^2} = 100\sqrt{2} ) ohms.
The reading will be very close to zero ohms.
An inductor has two properties. The first is resistance(measured in ohms), which is due to the length, cross-sectional area, and resistivity of the conductor from which it is wound. The second is inductance (measured in henrys), which is due to the length of the inductor, its cross-sectional area, the number of turns, and the permeability of its core.The inductor's resistance limits the value of current flowing through the inductor. The inductor's inductance opposes any change in current.
Opposition to the flow of AC current produced by an inductor. Measured in Ohms and varies in direct proportion to frequency.
With a meter that measures Ohms.
A changing current through an inductor induces a voltage into the inductor, the direction of which always opposes the change in that current.So, in a d.c. circuit, an inductor will oppose (not prevent) any rise or fall in current, although the magnitude of that current will be determined by the resistance of that inductor, not by its inductance.In an a.c. circuit, because the current is continuously changing both in magnitude and in direction, it acts to continuously oppose the current due to its inductive reactance. Inductive reactance is proportional to the inductance of the inductor and the frequency of the supply. The vector sum of the inductive reactance of the inductor and the resistance of the inductor, is termed the impedance of the inductor. Inductive reactance, resistance, and impedance are each measured in ohms.
The resulting maximum current is limited by the resistance of the inductor. As the current increases from zero to that maximum value, its expanding magnetic field induces a voltage into the inductor which opposes the rise in that current. So, instead of reaching its maximum value instantaneously, it takes some time -determined by the equation:time to maximum current = 5 L / R (seconds)where L = inductance of inductor in henrys, and R = resistance of inductor in ohms.
.513 ohms is simply 0.513 ohms. The unit "ohm" measures electrical resistance, and the numerical value remains the same regardless of how it's expressed. Therefore, there are 0.513 ohms.
That is possibly the input impedance of a loudspeaker - not an impedance of an amplifier.