An Amperian loop encloses three conductors carrying currents of 4 A, 3 A, and 1 A. Two currents are directed into the page and one is directed out of the page. Which additional information is required to determine the enclosed current?
The direction of each current
Ampere’s law states \(\oint \vec{B} \cdot d\vec{l} = \mu_0 I_{enc}\), where Ienc is the algebraic (net) sum of currents passing through the loop.
Currents in one direction are taken positive and in the opposite direction negative, so the sign of each current depends on its direction.
Knowing that two currents go in and one comes out is not enough; we must know which of the 4 A, 3 A and 1 A is directed out. For example, if 1 A is out, \(I_{enc} = 4 + 3 - 1 = 6\) A; if 4 A is out, \(I_{enc} = 3 + 1 - 4 = 0\).
The other data are not needed: resistance and material of the conductors do not enter Ampere’s law, and the loop radius does not change the enclosed current as long as the conductors are inside the loop.
Hence, the answer is The direction of each current.
The magnetic field inside a long solenoid is 4 × 10−3 T when it carries a current of 2 A. If the current is increased to 6 A, the magnetic field becomes:
A long solenoid carries a steady current. An Amperian loop is chosen completely outside the solenoid. What is the magnetic field along this loop according to the ideal solenoid model?
Ampere's circuital law relates the line integral of the magnetic field around a closed path to:
The wire loop shown in the figure carries a steady current $I$. Each straight section of the loop has length $d$. A part of the loop lies in xy plane and the other part is tilted at $30^\circ$ with respect to the xz plane. The magnitude of the magnetic dipole moment of the loop (in appropriate units) is

An infinitely long cylinder of radius $R$ carries a frozen-in magnetization $\vec M = ke^{-s^2} \hat z$, where $k$ is a constant and $s$ is the distance from the axis of cylinder. The magnetic permeability of free space is $\mu_o$. There is no free current present anywhere. The magnetic flux density ($\vec B$) inside the cylinder is