Magnetism
A hollow tube is carrying an electric current along its length distributed uniformly over its surface. The magnetic field :
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 :
$$\mu_0(I_{enc})=\oint \bar B.\bar dl$$
Area vector of ABC is along the right direction, while ACD is along the upward direction.
Now currents passing through ABC are $$I_1,I_3$$ along the area directions.
Now through ACD, $$I_2,I_3; I_2$$ along the area vector while $$I_3$$ is opposite to it.
Thus, $$\mu_0(I_1+I_3+I_2-I_3) = \oint \bar B.\bar dl = \mu_0 (I_1+I_2)$$
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
In a coaxial, straight cable, the central conductor and the outer conductor carry equal currents in opposite directions. The magnetic field is zero :
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