Magnetic Field due to circular current loop is considered one the most difficult concept.
55 Questions around this concept.
A current $i$ ampere flows along an infinitely long straight thin walled tube, then the magnetic induction at any point inside the tube is
Two concentric coils each of radius equal to $2 \pi \mathrm{~cm}$ are placed at right angles to each other. 3 A and 4 A are the currents flowing in each coil, respectively. The magnetic induction in $\mathrm{Wb} / \mathrm{m}^2$ at the centre of the coils will be:
$\left(\mu_0=4 \pi \times 10^{-7} \mathrm{~Wb} / \mathrm{A}-\mathrm{m}\right)$
A current loop consists of two identical semicircular parts each of radius R, one lying in the x-y plane and the other in the x-z plane. If the current in the loop is i., the resultant magnetic field due to the two semicircular parts at their common centre is
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Choose the correct sketch of the magnetic field lines of a circular loop shown by the dot and
.
A conducting circular loop is placed in a uniform magnetic field, B = 0.025 T with its plane perpendicular to the loop. The radius of the loop is made to shrink at a constant rate of 1 mms-1. The induced emf when the radius is 2 cm is
A thin ring of radius R meter has charge q coulomb uniformly spread on it. The ring rotates about its axis with a constant frequency of f revolutions/s. The value of magnetic induction in Wb/m2 at the centre of the ring is:
Magnetic Field due to circular current loop at its centre:
Magnetic Field due to circular coil at Centre-

$$
B_0=B_{\text {Centre }}=\frac{\mu_0}{4 \pi} \frac{2 \pi N i}{r}=\frac{\mu_0 N i}{2 r}
$$
where $\mathrm{N}=$ number of turns, $\mathrm{i}=$ current and $\mathrm{r}=$ radius of a circular coil.
Similarly, if Arc subtend angle theta at the centre as shown below then
$$
B_0=\frac{\mu_0}{4 \pi} \cdot \frac{\theta i}{r}
$$

similarly, if Arc subtends angle $(2 \pi-\theta)$ at the centre then
$$
B_0=\frac{\mu_0}{4 \pi} \cdot \frac{(2 \pi-\theta) i}{r}
$$

So the magnetic field of Semicircular arc at the centre is
$$
B_0=\frac{\mu_o}{4 \pi} \frac{\pi i}{r}=\frac{\mu_o i}{4 r}
$$

So Magnetic field due to three quarter Semicircular Current-Carrying arc at the centre is
$$
B_0=\frac{\mu_o}{4 \pi} \frac{\left(2 \pi-\frac{\pi}{2}\right) i}{r}
$$

Right-Hand Thumb Rule gives the direction of the magnetic field of Circular Currents.
Right-hand thumb rule is stated below:
If the fingers are curled along the current, the stretched thumb will point towards the magnetic field.

1. If the current is in a clockwise direction then the direction of the magnetic field is away from the observer or perpendicular inwards.

2. If the current is in anti-clockwise direction then the direction of the magnetic field is towards the observer or perpendicular outwards

1. If the Distribution of current across the diameterthen $B_0=0$

2. if Current between any two points on the circumference-
Then $B_0=0$

3.Concentric co-planar circular loops carrying the same current in the Same Direction-

$$
B_{\text {centre }}=\frac{\mu_o}{4 \pi} 2 \pi i\left[\frac{1}{r_1}+\frac{1}{r_2}\right]
$$
If the direction of currents are the same in concentric circles but having a different number of turns then
$$
B_{\text {centre }}=\frac{\mu_o}{4 \pi} 2 \pi i\left[\frac{n_1}{r_1}+\frac{n_2}{r_2}\right]
$$
4.Concentric co-planar circular loops carrying the same current in the opposite Direction-

$$
B_{\text {centre }}=\frac{\mu_o}{4 \pi} 2 \pi i\left[\frac{1}{r_1}-\frac{1}{r_2}\right]
$$
If the number of turns is not the same i.e $n_1 \neq n_2$
$$
B_{\text {centre }}=\frac{\mu_o}{4 \pi} 2 \pi i\left[\frac{n_1}{r_1}-\frac{n_2}{r_2}\right]
$$
5. Concentric loops but their planes are perpendicular to each other-

Then $B_{\text {net }}=\sqrt{B_1^2+B_2^2}$
6. Concentric loops but their planes are at an angle ϴ with each other-

$B_{\text {net }}=\sqrt{B_1^2+B_2^2+2 B_1 B_2 \cos \theta}$
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