**There are two methods of magnetic induction B calculation. The first method is using the Biot-Savart-Laplace and induction superposition principle. The second method is using the B vector circulation theorem, which will be explained below.**

It is very easy to use this theorem with cylindrical, sphere or flat symmetry of a conductor. Vector circulation by the enclosed loop *A *is

Figure 28. *( B,dr) *is a projection of

*on the vector*

**B***d*, which is integral algebraic sum of the projections of

**r***on the*

**B***d*vector, when the loop A is a set of fragments. It is important to note that we cannot derive the loop to the electrons, because an electron is an accelerating particle. However, magnetic field devices in our approximation are characterised by a velocity component. Thus, vector

**r***circulation theorem states the following:*

**B**Magnetic field * B* circulation by the enclosed loop A, is proportional to the algebraic sum of currents going through this loop

If there is a distributed current flowing through the surface Ω surrounded by the closed loop or path A, then

${\sum}_{i}{I}_{i}$should be replaced by

${\int}_{\Omega}jdS$where j is a density of a current flow through the surface Ω enclosed by the loop A.

If we generalise the circulation statements for simple cases, it will lead us to the most complex case.

- Considering a wire with electric current, we choose the path A perpendicular to the conductor – this path will correlate to the one of magnetic induction lines. Figure 29. Then

$\oint (\mathit{B},d\mathit{r})=\oint B\left(r\right)dr=B\left(r\right)2\pi r$ By the Biot-Savart-Laplace Law*B(r)*this conductor is$\frac{{\mu}_{0}I}{2\pi r}$ then$\oint (\mathit{B},d\mathit{r})=\frac{{\mu}_{0}I}{2\pi r}*2\pi r={\mu}_{0}I$ This result corresponds to the theorem we stated before.

2. 2. Let’s consider the case with the same straight wire, but taking a closed path with a random form. Then

$\oint (\mathit{B},d\mathit{r})=\oint {B}_{r}dr=B*r*d\alpha $The magnetic induction for the wire is

$B\left(r\right)=\frac{{\mu}_{0}I}{2\pi r}$then

$\oint (B,dr)=\oint \frac{{\mu}_{0}I}{2\pi d\alpha}=\frac{{\mu}_{0}I}{2\pi}\oint d\alpha ={\mu}_{0}I$3. Let’s consider the case when the conductor is outside of the path A. Figure 31. The path with be divided into two parts, then the result will be evident:

$\oint (\mathit{B},d\mathit{r})=\frac{{\mu}_{0}I}{2\pi r}({\int}_{1}^{2}d\alpha +{\int}_{2}^{1}d\alpha )=0$4. If the path A is oriented with some angle to the conductor and has a random form, we can also divide projections of * B *on the

*d*– to parallel and perpendicular components:

**r**(perpendicular component – result related to previous case).

5. In the case of several conductors crossing the loop, we can generalise the result above and make an algebraic sum of the magnetic induction circulation integrals. This generalisation will lead us to the result

$\int {\mu}_{0}{j}_{s}dS$Let’s resolve some examples using the theorem of magnetic field circulation.

**Example 1. The conductor with the radius**

*R***is characterised by the uniform current density**

*j, μ*_{i}=μ_{o}=1**. Determine the magnetic field**

*B(r)***along the axis of the wire**

For radius-vector r coordinates are (0,0,z), for radius vector **r**_{1} coordinates are (Rcosα,Rsinα,0). Then for d**r**_{1} (-Rsinαdα,Rcosαdα,0) and **r- r**_{1}=(-Rcosα,-Rsinα,z). For **r-r**_{1} × d**r _{1}** we have (zcosα,zsinα,R)Rdα.

For

$B=\frac{{\mu}_{0}I}{4\pi}\frac{R}{({R}^{2}+{z}^{2}{)}^{3/2}}{\int}_{0}^{2\pi}(os\alpha ,zsin\alpha ,R)d\alpha =\frac{{\mu}_{0}I}{4\pi}\frac{R}{({R}^{2}+{z}^{2}{)}^{3/2}}2\pi R{e}_{z}=\frac{{\mu}_{0}I{R}^{2}}{({R}^{2}+{z}^{2}{)}^{3/2}}{e}_{z}$**Example 2. Determine the magnetic field**

*B(r)*of solenoid**for symmetrical coils are parallel to the coil axis, and the magnetic field occurs parallel to the coil axis inside and outside of the coil. Let’s choose the contour abcd, as it is shown in the Figure b. Circulation of vector**

*B(r)***for this contour is $B={\int}_{a}^{b}{B}_{l}dl+{\int}_{b}^{c}{B}_{l}dl+{\int}_{c}^{d}{B}_{l}dl+{\int}_{d}^{a}{B}_{l}dl=Bl$**

*B*then

$Bl={\mu}_{0}{\sum}_{i}{I}_{i}={\mu}_{0}NI,B={\mu}_{0}nI$Magnetic fields outside of the solenoid are very small, and nearly all the magnetic fields ars concentrated inside of it. The magnetic field of the solenoid is uniform.

Sometimes wires form complex structures. So how do we use the Biot-Savart-Laplace Law in this case? To resolve these cases the structure can be divided into segments. And Biot-Savart-Laplace Law can be applied individually to each segment. Then for a complex structure we get:

$B=\frac{{\mu}_{0}I}{4\pi}{\sum}_{i}\int \frac{rdr}{{r}^{3}}$Let’s consider the segment of a wire depicted on the Figure c. * rdr=dhdl*, where h is the line from the point where we are estimating the magnetic field to the wire segment, or its extrapolation.

*l*is coinciding with the wire segment. As h is perpendicular to the wire segment, then

*And*

**hxl**=h*l.*d*Then

**r**x**r**=d**h**xd**l**.Here

${r}^{2}={l}^{2}+{h}^{2},and{r}^{3}=({l}^{2}+{h}^{2}{)}^{3/2}$So

$B=\frac{{\mu}_{0}I}{4\pi}{{\int}_{{l}_{1}}}^{{l}_{2}}\frac{hdl}{({l}^{2}+{h}^{2}{)}^{3/2}}$Let’s express l_{1} and l_{2} with known variables – *h* and *α*.

Then

${{\int}_{{l}_{1}}}^{{l}_{2}}\frac{hdl}{({l}^{2}+{h}^{2}{)}^{3/2}}=\frac{\u20131}{h}{{\int}_{{\alpha}_{1}}}^{{\alpha}_{2}}dcos\alpha =\frac{\mathrm{cos}{\alpha}_{1}\u2013\mathrm{cos}{\alpha}_{2}}{h}$For the given straight segment of wire

$\mathit{B}=\frac{{\mu}_{0}I}{4\pi}\frac{\mathrm{cos}{\alpha}_{1}\u2013\mathrm{cos}{\alpha}_{2}}{h}{\mathit{e}}_{z}$**Example 3. Let’s calculate the magnetic field for the circuit in Figure d**

The square sides are d, the

${\alpha}_{1}=45,{\alpha}_{2}=135$Magnetic field at the centre of the square

$B=\frac{{\mu}_{0}I}{2\pi d}(cos45\u2013cos135)=\frac{\surd 2}{2\pi}\frac{{\mu}_{0}I}{d}$(magnetic field for the triangle).

$B=\frac{2\surd 2}{\pi}\frac{{\mu}_{0}I}{d}$