Magnetism
A hollow tube is carrying an electric current along its length distributed uniformly over its surface. The magnetic field :
In a coaxial, straight cable, the central conductor and the outer conductor carry equal currents in opposite directions. The magnetic field is zero :
$$\vec{B} = \vec{B_{outer}} + \vec{B_{inner}}$$
Since the current carried by the outer and and inner are equal and in opposite direction,
magnetic field produced by the cylinders at a point P( distance r from central axis ) is
$$\vec{B_{outer}}= \dfrac{\mu_0}{4\pi}i\dfrac{\vec{dl}\times \vec{r}}{r^3}$$
$$\vec{B_{inner}}= -\dfrac{\mu_0}{4\pi}i\dfrac{\vec{dl}\times \vec{r}}{r^3}$$
$$ \therefore \vec{B} = \vec{B_{outer}} + \vec{B_{inner}} = 0$$
A hollow tube is carrying an electric current along its length distributed uniformly over its surface. The magnetic field :
A steady electric current is flowing through a cylindrical conductor
A long straight wire of radius R carries a current distributed uniformly over its cross-section. The magnitude of the magnetic field is
Sometimes we show an idealised magnetic field which is uniform in a given region and falls to zero abruptly. One such field is represented in figure. Using Ampere's law over the path PQRS, show that such a field is not possible.
Amperes circuital law is given by
The coil of a dynamo is rotating in a magnetic field. The developed induced emf changes and the number of magnetic lines of force also changes. Which of the following conditions is correct?
State Ampere's circuital law.
A current of $$\dfrac{1}{(4\pi)}$$ ampere is flowing in a long straight conductor. The line integral of magnetic induction around a closed path enclosing the current-carrying conductor is
Figure shows an Amperian path $$ABCDA$$. Part $$ABC$$ is in verical plane $$PSTU$$ while part $$CDA$$ is in horizontal plane $$PQRS$$. Direction of circulation along the path is shown by an arrow near point $$B$$ and $$D$$. $$\oint { \vec { B } .d\vec { l } } $$ for this path according to Ampere's law will be :