\(\frac{2\sqrt2 \mu_0L^2}{\pi l}\)
\(\frac{\mu_0L^2}{2\sqrt2 \pi L}\)
\(\frac{2\sqrt 2 \mu_0 l^2}{\pi L}\)
\(\frac{\mu_0L^2}{2\sqrt2\pi l}\)
B1=4B=\(\frac{4μ_0i}{4π(\frac{L}{2})(2sin45°)}\)
B1=\(\frac{2\sqrt 2 \mu_0 l^2}{\pi L}\)
M=\(\frac{Flux inner loop}{i}\)=\(\frac{2\sqrt 2 \mu_0 il^2}{i\pi ^2}\)
=\(\frac{2\sqrt2 \mu_0l^2}{\pi L}\)
Inductance is a key parameter in electrical and electronic circuit designs. Like resistance and capacitance, it is a basic electrical measurement that affects all circuits to some degree.
Inductance is used in many areas of electrical and electronic systems and circuits. The electronic components can be in a variety of forms and may be called by a variety of names: coils, inductors, chokes, transformers, . . . Each of these may also have a variety of different variants: with and without cores and the core materials may be of different types.
There are two ways in which inductance is used: